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Currently, I am trying to determine %reflectance and %transmittance of light through an array of nanofibers in COMSOL 6.2 optics. I have successfully determined reflection and transmission cross-sections. But unfortunately, I can not calculate %reflectance and %transmittance. How can I determine this?
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The method I employed involved generating virtual surfaces at the respective ends of the system and integrating the deposited or frozen ray power to compute the reflectance and transmittance.
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This is a transmission electron microscope picture of salivary gland secretory cells. What is the structure in the picture?
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Thank you very much for the answers provided by all the teachers.
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Influenza (flu) remains a significant public health challenge, particularly during peak seasons. This research seeks to explore the effectiveness of various preventive strategies in controlling the spread of the flu. The study will examine the impact of annual flu vaccinations on infection rates among different age groups, as well as assess the role of non-pharmaceutical interventions, such as hand hygiene and mask usage. By comparing these strategies, the research aims to provide insights into the most effective methods for reducing flu transmission and improving public health outcomes.
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As big mask studies are still inconclusive you are unlikely to detect much impact in your sample.
Unless you run around with lateral flow test (in contrast to relying on counting symptomatic ILI), you may even have problems to detect statistically significant impact of vaccination on medium sized sample.
[I just warn you before you put lot's of effort into your study and later end up with inconclusive results that no journal would be willing to publish]
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I want to know if there is any tools in CST to optimize the designed structure to decreease beam level in zero degree.
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To decrease grating lobes, especially at zero degrees, in your beam steering transmissive phase gradient metasurface designed in CST, you can use several optimization techniques and tools available within CST Studio Suite. Here are some suggestions:
  1. Parameter Sweep and Optimization: Use the Parameter Sweep tool to systematically vary design parameters and observe their effects on grating lobes. Employ the Optimization tool to automatically adjust parameters to minimize grating lobes. You can set specific goals, such as reducing side lobe levels or improving beam directivity.
  2. Array Factor Optimization: Optimize the array factor by adjusting the spacing and phase of the elements in your metasurface. This can help in reducing grating lobes.
  3. Filter Design: Implement spatial filters to suppress unwanted lobes. This can be done by designing the metasurface elements to have specific frequency responses.
  4. Advanced Solver Settings: Utilize advanced solver settings in CST, such as the Time Domain Solver or Frequency Domain Solver, to accurately simulate and optimize the metasurface performance.
  5. Use of Macros: CST provides macros that can automate repetitive tasks and complex optimization routines. You can create or use existing macros to fine-tune your metasurface design.
  6. Design of Supercells: Design supercells with non-uniform element spacing or varying phase gradients to suppress grating lobes. This approach can help in achieving a more uniform radiation pattern.
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I am currently working on photonic crystals, where I need to find the transmission vs. wavelength curve in COMSOL Multiphysics. I have eigenfrequencies for the photonic crystal and need to determine the transmission vs. wavelength around those frequencies. I am also providing some images for reference.
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I can not speak English
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I want to simulate the transmission of a Gaussian beam in an optical fiber, and I have used a beam module to complete the modeling of the three-dimensional structure of the optical fiber. When adding port boundary conditions, I only use the system's default mode input. If I want to define a Gaussian beam that deviates from the center of the fiber, I can change the incident setting. Thank you very much for your help.
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You may contact acadnexconsult@gmail.com for one to one sessions.
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I have white ink-coated thin film sample transmission data from normal UV-Vis-NIR spectroscopy. Also, %T data were collected using an integrated sphere. There is a huge difference in the spectral data.
Also, data from %R from DRS converted to %T is compared
Please help me to understand the difference between the various %T data obtained from different methods. Which is correct?
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Look at articles by Scott Prahl (Oregon Medical Laser Center) on a technique called Inverse Adding Doubling. For example:
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Previously, I successfully modelled the transmission and reflection of electromagnetic waves incident on non-magnetic materials. Please refer to my publications for details:
These models use a polynomial approach and apply transverse voltages to the multilayer thin film. The Fresnel transmission and reflection coefficients are calculated based on the refractive index, derived from a general formula for non-magnetic materials. For magnetic materials, these coefficients can be calculated using the general formula based on intrinsic impedance. While refractive index databases are available for most materials across various wavelengths, intrinsic impedance databases are not.
The question now is: How can we model the transmission and reflection of electromagnetic waves incident on magnetic materials when applying a transverse voltage?
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Thank you Smrity Dwivedi, I will check, and come back to discuss.
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I need to do TEM analysis for my Polyaniline emeraldine salt form. May I know which solvent is appropriate for preparing TEM sample?
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Preparing Polyaniline Emeraldine Salt (PANI-ES) Sample for TEM Analysis
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I need to do TEM analysis for my Polyaniline emeraldine salt form. May I know which solvent is appropriate for preparing the TEM sample?
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Preparing a Polyaniline Emeraldine Salt (PANI-ES) sample for TEM analysis involves several steps to ensure proper dispersion and sample quality. Below is a detailed guide on how to achieve this:
Materials Needed
  1. Polyaniline Emeraldine Salt (PANI-ES)
  2. Appropriate solvent (e.g., N-Methyl-2-pyrrolidone (NMP), Dimethyl sulfoxide (DMSO), or Methanol)
  3. Ultrasonic bath or probe sonicator
  4. TEM grids (e.g., carbon-coated copper grids)
  5. Pipette or micro-syringe
  6. Filter (optional, depending on solvent and particulate size)
Steps to Prepare the TEM Sample
  1. Choose an Appropriate Solvent: The solvent should be able to disperse PANI-ES effectively. Common solvents include:N-Methyl-2-pyrrolidone (NMP): Known for its strong solvating ability for conductive polymers. Dimethyl sulfoxide (DMSO): Another excellent solvent for PANI-ES. Methanol: Can be used but may not be as effective as NMP or DMSO for dispersion. Note: The choice of solvent might depend on the specific requirements of your analysis and availability.
  2. Prepare the PANI-ES Dispersion:Weigh a small amount of PANI-ES (typically a few milligrams, depending on the desired concentration). Add the solvent: Transfer the weighed PANI-ES into a clean container and add a small volume of the chosen solvent (a few milliliters). Sonicate the mixture: Use an ultrasonic bath or probe sonicator to disperse the PANI-ES in the solvent. Sonicate for about 30 minutes to ensure thorough dispersion.
  3. Prepare TEM Grids:Clean the TEM grids: If necessary, clean the TEM grids by rinsing with solvent and drying them using a gentle nitrogen flow. Drop-cast the dispersion: Using a pipette or micro-syringe, carefully drop a small amount (a few microliters) of the PANI-ES dispersion onto the carbon-coated side of the TEM grid. Dry the sample: Allow the solvent to evaporate at room temperature. This can be done in a clean, dust-free environment to prevent contamination.
  4. Optional Step - Filtration:If the dispersion contains large aggregates or particulate matter, you might need to filter it using a small pore-size filter (e.g., 0.2 µm) before drop-casting onto the TEM grid.
  5. Inspect the Sample:Once the sample is dry, inspect it under an optical microscope (if available) to ensure a uniform dispersion of PANI-ES on the grid.
  6. TEM Analysis:The prepared TEM grid is now ready for TEM analysis. Carefully load the grid into the TEM holder and proceed with the imaging.
Tips and Considerations
  • Concentration: Adjust the concentration of the PANI-ES dispersion according to the requirements of your TEM analysis. A very dilute solution might not deposit enough material, while a highly concentrated solution might result in aggregation.
  • Solvent Choice: The solvent should not react with PANI-ES or leave residues after evaporation that could interfere with TEM imaging.
  • Sonication Time: Be cautious with sonication time and power to avoid degrading the PANI-ES structure.
  • Storage: If the dispersion needs to be stored before use, ensure it is kept in a sealed container to prevent solvent evaporation and potential changes in dispersion quality.
By following these steps, you can prepare high-quality PANI-ES samples suitable for TEM analysis, enabling you to obtain clear and detailed images of your material.
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I need this complete article, could anyone help me? follow theme below.
Chikungunya virus cell-to-cell transmission is mediated by intercellular extensions in vitro and in vivo.
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Buy, subscribe or find in a decent library.
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Hi,
I get confused about the CST calculations for reflection and transmission values (S- S-Parameters) for different kinds of transmission lines.
1)First could you please let me know where is the evanescent port mode selection available in CST for waveguide port?
2)If I want to see the S11 parameters of a rectangular waveguide, how does the CST calculate it?
Explain more:
The input impedance of a rectangular waveguide is its wave impedance of dominate mode. So the Zte impedance is not fixed and it varies with frequency. (attachment formula)
So, what type of and what value of waveguide port impedance is considered, for calculating the S11 parameters during the total bandwidth of a dominant mode and also more than dominant mode bandwidth?
3) If the type of TLs are not common or some changes are made, how does CST calculate the S11 for these structures? For popular TLs such as waveguides, we have a common formula.
I appreciate your time and explanation in advance.
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I wouldn't expect CST to be that accurate for S21. If you don't run it for very long you have power still bouncing around inside the problem, and if you run it for a long time then numerical errors start to build up. How much ripple was there left on the S11? If you watch the S11 as the solution progresses you can see the ripple reduce every time a lump of energy arrives at the port (see the energy monitor). If the finishing point is -40 dB energy left there is still 0.01% of the energy left in the problem which has the potential to make +/-1% difference in the voltage at the output port which is */-2% of the power. The absence of this from the answer leaves ripple in the S parameter. This ripple is bigger than the differences you are seeing. I'm not sure that the impedance is calculated as you would hope, but I think you can't tell from these results if it's right or not.
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Lets have a discussion with regards to OSI physical and datalink layer transmission (signalling) technologies in the presence of quantum assisted crypt analyzers.
We can base our discussion on the advent of the Next generation Networks(NGN) such as 5G Standalone Architecture: 5GCore, 5G Edge, 5G NR and IP eXchange.
Discussion Questions:
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1. How are these networks going to handle quantum crypt analysis from classical perspective especially where the networks interconnect and interoperate?
2. While newer cryptology modules are being introduced, how likely are they in terms of speed to counter quantum technologies in the interconnect where key exchange handover happens?
3. NGN introduced Network Function Virtualization based on Software Defined Technologies using slices. How likely in terms of quantum that the actual Core Technologies in terms of configuration and Misconfiguration can be compromised to a point that the entire topology can be down affecting the entire ecosystem?
Lets discuss, I am still learning and ready to learn from the experts, where proper phrasing is needed please advise, I will gladly update. OSI L1/L2 as reference model will be a great start.
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Quantum cryptanalysis poses a significant challenge to classical cryptographic systems due to its potential to break some widely used encryption algorithms. To mitigate this risk in network communication, classical networks can implement post-quantum cryptographic algorithms, which are resistant to quantum attacks. Additionally, network operators can employ hybrid encryption schemes that combine classical and quantum-resistant algorithms to ensure security. However, ensuring interoperability and security across interconnected networks will require careful design and coordination to address potential vulnerabilities.
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Hello, when I use a reflective light microscope (with light entering at approximately 45 degrees), I can see a lot of details and textures. I suspect the image may contain some sub-annual lines. However, when I use a transmissive light microscope or a reflective light microscope (with light entering vertically), I can see the main growth lines more clearly, and many micro-growth lines and textures are not visible under oblique light. I am conducting cross-dating and am unsure which perspective of images to use for cross-dating.
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Lusha M Tronstad Thank you very much for your help! The current shell samples I have are wrapped in resin, with a thickness of about 2cm. I'm using a reflected light microscope to observe the growth lines in the hinge plate area. Although the growth lines are relatively clear in the eyepiece of the reflected light microscope, they appear blurry and there are some bright spots when photographed with a camera connected to the microscope. I have consulted some literature, and it seems that this may be due to significant light scattering in thick sections. It looks like I need to cut my samples thinner. Thanks again for your help!
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Good afternoon,
I was wondering if anyone in UK has a NIR/SWIR microspectrophotometer or a spectrometer for transmission measurements between 850 nm and 2000 nm? Our samples are on a 2 cm x 2cm glass substrate and the sample (from which the transmission will be measured) area is 2mm x 2mm.
Thank you
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If I were you, I would try to call a local representative of a company, who sells NIR spectrophotometers. Most probably, they would agree to measure your sample. They do such experiments for advertisement. If you like the result, you might be able to talk them in letting you to use their spectrometer to make a mutual publication
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I am confused as some researchers took s11 below -10 db. and s11 around 0 db. or in some journals s11 approaches to 0 db. and s21 is below -10 db. what is the exact consideration of s11 and s21 parameters while designing a unit cell for lens antenna.
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S11 is a coefficient that reflects the amount of energy reflected by a material or surface. For example, if you want to design a unit cell for a frequency selective surface (FSS), the goal should be to have maximum reflection (0dB) and minimum transmission (for example, -20 dB) at resonance frequencies. Similarly, if you want to design a metamaterial that passes maximum signal and has less reflection, then S11 should be minimized (i.e., -20 dB), and transmission should be maximized (S21 ~ 0 dB). The specific application of the unit cell determines the desired values for S11 and transmission.
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Security is a major concern for IoT devices. How does CIoT leverage existing cellular network security features to protect data transmission between devices and the cloud?
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Cellular IoT (CIoT) leverages existing cellular network security features to protect data transmission between devices and the cloud in several ways:
1. Authentication: CIoT devices are authenticated before they are allowed to connect to the cellular network. This ensures that only authorized devices can communicate with the network and any data transmission is secure.
2. Encryption: CIoT uses encryption to protect the data being transmitted between devices and the cloud. This ensures that even if data is intercepted, it cannot be easily understood or tampered with.
3. Secure communication protocols: CIoT devices use secure communication protocols such as SSL/TLS to ensure that data transmission is secure and cannot be intercepted or tampered with.
4. Network segmentation: Cellular networks are typically segmented to separate IoT devices from other devices on the network, reducing the risk of unauthorized access to sensitive data.
5. Firewall protection: Firewalls are used to monitor and control incoming and outgoing network traffic to prevent unauthorized access and protect data transmission.
Overall, CIoT leverages the security features of existing cellular networks to ensure that data transmission between devices and the cloud is secure and protected from potential threats.
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I have applied the SHA-256 hash function to the plain image to generate the initial values of the chaotic map in the image encryption algorithm and include it in key space analysis. So, when the receiver wants to decrypt the received image from the transmission, he needs the key, which is the SHA-256 output. Now, someone has asked me, "SHA-256 hash function is applied, how to transmit the hash values but with no extra transmission"?
Anyone can give me some hints on how to transmit the SHA-256 function output without no extra transmission?
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Transmitting the SHA-256 function output without any additional transmission involves sending the result along with the data it's derived from in a single transmission. This can be achieved by including the SHA-256 hash along with the original data. Here's how you can do it:
  1. Calculate the SHA-256 Hash: First, compute the SHA-256 hash of the data you want to transmit. This generates a fixed-size hash value unique to the input data.
  2. Transmit the Data and Hash Together: When transmitting the data, append or prepend the SHA-256 hash to it. This ensures that both the original data and its corresponding hash are sent in a single transmission.
  3. Recipient Verification: Upon receiving the data, the recipient can separate the hash from the data. They can then independently compute the SHA-256 hash of the received data and compare it with the transmitted hash. If the computed hash matches the transmitted hash, it indicates that the data has not been altered during transmission.
Here's a simple example in Python:
pythonCopy codeimport hashlib def transmit_data_with_hash(data): # Calculate the SHA-256 hash of the data hash_value = hashlib.sha256(data.encode()).hexdigest() # Transmit data and hash together transmitted_data = data + hash_value # Return the transmitted data return transmitted_data def verify_transmitted_data(transmitted_data): # Separate the data and hash data = transmitted_data[:-64] # Assuming SHA-256 hash length is 64 characters transmitted_hash = transmitted_data[-64:] # Recompute the hash of the received data computed_hash = hashlib.sha256(data.encode()).hexdigest() # Compare computed hash with transmitted hash if computed_hash == transmitted_hash: return "Data integrity verified. No alterations detected." else: return "Data integrity verification failed. Possible alterations detected." # Example usage original_data = "Hello, world!" transmitted_data = transmit_data_with_hash(original_data) print("Transmitted data with hash:", transmitted_data) # Simulating transmission... # Upon receiving transmitted_data, recipient verifies it verification_result = verify_transmitted_data(transmitted_data) print(verification_result)
This code demonstrates how to transmit data along with its SHA-256 hash and verify data integrity upon reception. Remember to adjust the code as needed for your specific use case and programming environment.
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"In what ways might the integration of IoT confront apprehensions surrounding data confidentiality and security, specifically concerning the acquisition, retention, and conveyance of confidential data?"
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I will try my best to answer it in terms of Governance, Product organization, or the person tasked with integration, their or his/her commitment in terms of policies and procedures might help showcase their seriousness towards protecting the confidential data of their customers. Compliance with Industry standards and regulations is another step towards trust and faith.
Independent attestations are a piece of excellent evidence.
In terms of technical controls and security, various alternatives can be looked at, starting with access management, data anonymization, encryption, and control/data plane segregation, to name a few.
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FTIR spectrum of ZnSe nanoparticles shows that its transmission is not flat around 10 micrometer but in the presented spectrum by lens companies its transmission is smartly flat. What can be the reason? doping? bulk form? or ....
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The answer depends on sample preparation and the shape of this feature:
  • Is that a well-defined band? 10 um is within the fingerprint region, so this is more likely related to contamination.
  • Is it a broad band? This could be due to reflection losses. Is this also present in the pure matrix? are you weighing your matrix+analyte spectra against the pure matrix?
  • does it look more like a baseline drift? A large one could be related to scattering effects, is the feature independent of sample grinding?
FTIR requires meticulous and reproducible sample preparation, it is common to account for these variations using a baseline correction. This is crucial in quantitative analysis, for example. See the following reference:
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Hi,
In my FDTD simulation result of transmission intensity for IR source (12 µm) over thin film ( thickneess 4µm) at different angles, I found that the intensity is maximum when theta angle is 30.
may i know what could explain this and is there any experiment result to verify?
thanks
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The model will have perfectly parallel surface on the film. You can expect strong etalon effects. With the film thickness close to the wavelength (given the index of refraction, the wavelength inside Silicon is about 3.5 um) you can expect the etalon to vary slowly with angle. Also, given the high index, the internal angle will change very slowly with external angle.
Try looking up etalon equations such as here: https://www.photonicsolutions.co.uk/upfiles/CXEtalons1.pdf
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I want to determine the effect of radome on plane wave in CST. I want to show the effectiveness of designed radome by Fresnel's coefficient. If any one know How to find Fresnel's transmission coefficient using CST MWS?
Thanks
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from magnitude of real and imaginary parts of S11 and S21 parameters.
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A certain host viremia threshold for mosquito infection with arboviruses has been recognized, however I have not been able to find any information on the "threshold" of viral load in saliva required for mosquito transmission of arboviruses. Has anyone read anything about this? I would appreciate any helpful comments.
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Boric acid causes organic substances crystalized so it does with mosquito saliva they are in form of growing white rings at the water edge when we serve them with regulated 40 degree pf water + 5% boric acid solution bait. (Please google "Mosquito control, killing of the females". For years we look at those ring to monitor mosquito population at our place)
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Seeking insights for optimizing data flow.
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Multiplexing significantly boosts data transmission efficiency in communication networks by packing multiple data streams into a single channel, maximizing its utilization. Imagine a highway with multiple lanes instead of just one. That's essentially what multiplexing does – it creates more "lanes" on the data highway to increase traffic flow.
Here's how it works:
Without Multiplexing:
  • Each data stream (voice call, video, file transfer) requires a dedicated channel.
  • If data transmission is low for any stream, the channel remains underutilized, wasting resources.
With Multiplexing:
  • A multiplexer device combines multiple data streams into one signal.
  • This signal is then transmitted over a single shared channel.
  • At the receiving end, a demultiplexer separates the combined signal back into its individual data streams.
Benefits of Multiplexing:
  • Increased Channel Utilization: By sharing a single channel, multiplexing maximizes its capacity, leading to more efficient data transmission.
  • Reduced Cost: Multiplexing eliminates the need for dedicated channels for each data stream, saving on infrastructure and maintenance costs.
  • Scalability: Networks can easily accommodate growing data traffic by adding more channels and employing multiplexing techniques.
  • Flexibility: Different types of data (voice, video, text) can be efficiently transmitted together using multiplexing.
Types of Multiplexing:
  • Frequency Division Multiplexing (FDM): Divides the channel into smaller frequency bands, each carrying a separate data stream.📷Opens in a new window📷www.elprocus.comFrequency Division Multiplexing diagram
  • Time Division Multiplexing (TDM): Divides the channel into time slots, each allocated to a specific data stream for a short duration.📷Opens in a new window📷www.geeksforgeeks.orgTime Division Multiplexing diagram
  • Wavelength Division Multiplexing (WDM): Used in fiber optic networks, combines multiple data streams onto different wavelengths of light within the same fiber.📷Opens in a new window📷www.researchgate.netWavelength Division Multiplexing diagram
Multiplexing is a fundamental technology in modern communication networks, enabling efficient data transmission for various applications, from phone calls and internet browsing to streaming video and online gaming. By packing more data onto available channels, multiplexing keeps us connected in a fast-paced digital world.
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Good day,
I investigate the 3D FDTD and TMM simulations in terms of the grating waveguide.
I'm currently setting up the simulation environment and verifying the similarity between the 3D FDTD simulations and TMM using the textbook, the 'L. Chrostowski and M. E. Hochberg, Silicon photonics design. Cambridge University Press, 2015.'
Utilizing the script ( of the textbook, it makes my work more convenient to set up the simulation. But, in comparison to the 3D FDTD and TMM, there are some gaps in the transmission graph.
The figure shows two transmissions running just your scripts, matching the physical parameters like 200 number of periods, 310nm period, 50nm delta width, and 500 Npoints. However, the reflection width of the 3D FDTD is narrower than the TMM although I tuned to the physical parameters. I know that the corrugation width influences the reflection width in the transmission due to the coupling coefficient, but they are the same. I was wondering the reason for the difference and I assume the reason is that the TMM doesn't consider the y and z boundary conditions. I'd be grateful if anyone could help Thank you
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1. Dimensionality
2. Spatial Resolution
3. Boundary Conditions
4. Material Models: FDTD simulations can account for complex material models, including dispersive and anisotropic materials, with more accuracy. TMM, while versatile, may use simplified material models or assume certain material properties to make calculations tractable. These simplifications can introduce discrepancies, particularly when dealing with materials that exhibit strong dispersion or anisotropy.
5. Computational Resources
Good luck!!
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i need simulation tools and more rerfernce about alogaritms used at 5G by NOMA
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I'll provide a comprehensive response to the prompt, combining the strengths of SLM and PTS techniques for PAPR reduction in NOMA systems within 5G:
Understanding PAPR in NOMA Systems:
  • NOMA (Non-Orthogonal Multiple Access) is a promising technology in 5G that enhances spectral efficiency by enabling multiple users to share the same time-frequency resources.
  • PAPR (Peak-to-Average Power Ratio) is a major challenge in NOMA systems due to the superposition of multiple user signals, leading to:Amplifier nonlinearities, causing signal distortion and performance degradation. Out-of-band emission, interfering with adjacent channels.
PAPR Reduction Techniques:
  • Selective Mapping (SLM):Generates multiple candidate signals with different phase rotations. Selects and transmits the signal with the lowest PAPR. Pros: Simple implementation, effective PAPR reduction. Cons: Requires side information for synchronization, increases overhead.
  • Partial Transmit Sequence (PTS):Divides the NOMA signal into multiple subblocks. Optimizes phase rotations for each subblock to minimize PAPR. Combines subblocks for transmission. Pros: Effective PAPR reduction, better spectral efficiency than SLM. Cons: Increased computational complexity.
Hybrid SLM-PTS Approach:
  • Combines the benefits of both techniques for enhanced PAPR reduction and spectral efficiency.
  • Steps:Generate multiple candidate signals using SLM. Divide each candidate signal into subblocks using PTS. Optimize phase rotations for each subblock within each candidate signal. Select the candidate signal with the lowest overall PAPR for transmission.
Advantages of SLM-PTS:
  • Offers superior PAPR reduction compared to individual SLM or PTS.
  • Improves spectral efficiency and BER performance.
  • Minimizes out-of-band emission.
Considerations:
  • Computational complexity increases due to combined processing.
  • Careful optimization of SLM and PTS parameters is crucial for balancing PAPR reduction and implementation complexity.
Conclusion:
The SLM-PTS hybrid technique is a promising approach for effective PAPR reduction in NOMA systems within 5G, enhancing spectral efficiency, signal quality, and overall system performance.
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I want to design a reconfigurable transmit array using varactor diode with metamaterial unit cell. I have gone through many literatures but in most of literature only different design and multiplayers are mentioned to achieve maximum transmission and 360 deg phase tuning. But i am not able to achieve both the things like high transmission and 360deg phase tuning. Could anyone suggest some resources to understand mathematics behind this?
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If you use frequncy multiplication post phase shifter, you phase shift will be multiplied as well. Also shift is generally easier to implement at lower frequncy.
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I am looking for ways to activate DREADDs in pups and was wondering if anyone could share experience/thoughts on whether CNO can be transmitted through maternal milk ? Thanks!
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Rajae Talbi Hi Rajae, I actually wonder the same. Since some time has passed, I was wondering if maybe now you have some insights on the CNO transmission through maternal milk? Did it work for you? Thank you!
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This is a Digital Communication course
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Transmission impairments are any factors that degrade the quality of a signal during transmission from one point to another. They can be caused by a variety of factors, including the transmission medium itself, environmental conditions, and interference from other signals.
Transmission impairments experienced by LTE include:
  • Attenuation: This is the loss of signal power as it travels through the transmission medium. Attenuation is more severe at higher frequencies, which is why LTE uses multiple frequency bands to improve coverage and capacity.
  • Noise: Noise is any unwanted signal that interferes with the desired signal. Noise can be caused by a variety of sources, such as thermal noise, interference from other electronic devices, and weather conditions.
  • Interference: Interference is caused by other signals that are transmitted on the same or adjacent frequency bands. Interference can degrade the quality of the LTE signal and reduce data throughput.
  • Multipath propagation: This occurs when the LTE signal is reflected off of objects in the environment, such as buildings, trees, and vehicles. Multipath propagation can cause the signal to arrive at the receiver at different times, which can lead to interference and signal distortion.
  • Doppler shift: This is a change in the frequency of a signal due to the relative motion between the transmitter and receiver. Doppler shift can be caused by the movement of vehicles, trains, and aircraft.
LTE systems use a variety of techniques to mitigate the effects of transmission impairments. These techniques include:
  • Automatic repeat request (ARQ): This protocol allows the receiver to request that the transmitter retransmit packets that were lost or corrupted due to transmission impairments.
  • Forward error correction (FEC): This technique adds redundant information to the transmitted signal so that the receiver can correct errors that occur during transmission.
  • Channel adaptation: This technique allows the LTE system to adjust its transmission parameters, such as the modulation scheme and coding rate, to match the current channel conditions.
By using these techniques, LTE systems are able to provide reliable and high-speed data transmission even in challenging environments.
In addition to the above impairments, LTE systems can also be affected by transient impairments, such as impulse noise and phase hits. Transient impairments are typically caused by sudden changes in the transmission environment, such as lightning strikes or power outages. LTE systems use a variety of techniques to detect and mitigate the effects of transient impairments.
By understanding the different types of transmission impairments and the techniques that LTE systems use to mitigate them, network engineers can design and operate LTE networks that provide reliable and high-speed data transmission to users.
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I have a question about the use of the sbdart radiation transmission software. I want to enter a custom atmospheric profile. One of the physical quantities is the water vapor density, so I don’t know from what data to get this characteristic value, or is there any way to do it Calculated, I hope everyone's help.
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Hi, i don't know how to set the output inthe sbdart so that the model can simulatethe radiance of 3.9um and 11um,i hope you can give some suggestions, thanks for a lot
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When I fuse the multi-single-multi fiber structure, coat it with silver film to stimulate the SPR phenomenon, and establish the transmission spectrum, I add water to the sensing area. The spectral line of the SPR transmission spectrum rises, but it should normally decrease. What is the reason? Thank you!
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The SPR process can be considered as an energy transfer process in which part of the energy of the incident light is transferred to the surface plasmon wave. Since the intensity of the peak increases with the addition of water, therefore water promotes the SPR process. This may occur due to the participation of the nuclear quantum effect.
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When I fuse the multi-single-multi fiber structure, coat it with silver film to stimulate the SPR phenomenon, and establish the transmission spectrum, I add water to the sensing area. The spectral line of the SPR transmission spectrum rises, but it should normally decrease. What is the reason? Thank you!
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The SPR process can be considered as an energy transfer process in which part of the energy of the incident light is transferred to the surface plasmon wave. Since the intensity of the peak increases with the addition of water, therefore water promotes the SPR process. This may occur due to the participation of the nuclear quantum effect.
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I want to measure the phase angle in comsol.
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Thank you Mehmet.
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from computational physics point of view
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In computational physics, the transmission spectrum is a concept often encountered in the study of wave propagation, particularly in the context of quantum mechanics and solid-state physics. Let's break down the key components:
  1. Wave Propagation:In quantum mechanics, particles, such as electrons, are often described as waves. The behavior of these waves can be analyzed as they interact with potential barriers or other structures.
  2. Transmission:When a wave encounters a potential barrier, part of it may be transmitted through the barrier, and part may be reflected back. Transmission refers to the portion of the wave that successfully passes through the barrier.
  3. Transmission Spectrum:The transmission spectrum is a plot or analysis that shows how the transmission of a wave varies with respect to some parameter, often the energy of the wave or the frequency.
  4. Applications:In the context of solid-state physics, the transmission spectrum is often used to study the behavior of electrons as they move through materials. For example, in the study of electronic transport in semiconductors or nanostructures, understanding how electrons transmit through potential barriers is crucial.
  5. Computational Physics:Computational methods are employed to simulate and analyze the transmission of waves through various structures. Numerical simulations, based on methods like quantum mechanics simulations or tight-binding models, can provide insights into the transmission properties of materials.
  6. Experimental Correlation:Transmission spectra obtained from computational simulations can be compared with experimental measurements. This helps validate the theoretical models and provides a basis for understanding and predicting the behavior of waves in different materials.
  7. Band Structures:In the context of periodic structures like crystals, the transmission spectrum is closely related to the electronic band structure. It reveals information about the allowed and forbidden energy bands for electrons in the material.
Understanding the transmission spectrum is crucial for designing electronic devices, understanding the behavior of materials at the quantum level, and predicting the properties of novel materials.
In summary, the transmission spectrum, in computational physics, provides a quantitative and often graphical representation of how waves, typically associated with particles like electrons, propagate through potential barriers or structures in a given material.
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In my NetSim 5G simulation, I keep seeing zero throughput, indicating no data transmission. Any suggestions on the factors or settings causing this, like (a) verifying correct gNB and UE configuration, (b) identifying network topology or connectivity errors, etc.? What steps can I take to understand and resolve this?
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There are a few possible reasons why you might be seeing zero throughput in your NetSim 5G simulation:
Network topology or connectivity errors: Make sure that the gNB and UE are connected and that the network topology is correct.
No application traffic: If there is no application traffic configured from the UE to the destination, then you will see zero throughput in your NetSim 5G simulation.
Pathloss: The UE may be too far from the gNB, resulting in high path loss and low signal strength.
Interference: The UE may be experiencing downlink interference from other gNBs
Congestion: The network may be congested, and thus no PRBs are allocated to the UE by the scheduling algorithm
To understand and resolve the issue, you can follow these steps:
Inspect the simulation results with radio measurement logs
Experiment with different simulation settings: You can try changing different simulation settings, such as the pathloss model, the network topology, the interference model, and the scheduling algorithm to see if that resolves the issue.
If you are still having trouble, best to contact NetSim support for help (E-mail support@tetcos.com)
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In one of our fiber photometry rigs, there is a pigtailed rotary joint connected to an FC-FC mating adapter (flange 11mm) that is then connected to our fiber optic patch cord. The problem is, the light transmission out of the pigtail is around 90 uW, and the adapter is pretty much the same, but then when we measure light transmission out of the fiber optic patch cord its around 20-30 uW. Is there any way to better optimize this region to get a higher light output?
Thanks!
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Assuming that you have matched NA's, core diameters, fibers (polarization characteristics, for example) and have compatible end-faces (angled/angled or straight/straight), in other words, that you have the right fibers and connectors, then you might suffer the problem that plagues all fiber connections -- dirt stuck to one of the end-faces or damage to one or more end-faces. You can check under a low-powered microscope. (Please take no offense at this low-tech suggestion -- it happens in all photonics labs.)
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There are two different waves of the gravitational field (GF):
1. Gravitational field transverse wave. What it reflects is the disturbance of the surrounding GF, and the transmission speed of this disturbance is equal to the slow light speed c. For example, the motion of the sun disturbs the GF generated by the center of the galaxy, causing transverse waves of GF around the sun.
2. Gravitational field longitudinal wave. It is generated by the gravitational source itself, and GF will transfer energy quickly, and this speed is much greater than the speed of light c.
When the gravitational source changes (position, mass), this change will first be reflected on the longitudinal wave of GF, and distant objects will feel the change of GF soon. At the same time, the disturbance of the gravitational source to other surrounding GFs will propagate to the surroundings at a slow speed c in the form of transverse waves.
To make an inappropriate analogy: when you throw a stone into a calm lake, you will observe slow water waves spreading around, which is the disturbance of the stone to the water surface, thus generating water waves. But in addition to water waves, there are sound waves in the water. The speed of the sound waves is much faster than that of the water waves, and the sound waves in the water arrive long before the slow water waves reach the shore.
A brief summary: the longitudinal wave of GF is produced by the gravitational source itself, and the transverse wave of GF is produced by the disturbance of the gravitational source to other surrounding GFs.
Newtonian gravity studies "sound waves in water", the longitudinal waves of GF.
Einstein GR studies the "water wave", that is, the transverse wave of GF.
I hope that you can understand the whole gravity from my simple narrative. You can also download my two papers on gravity here:
Kind regards,
Tony
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Dear Tony Tony Yuan ,
If you ask yourself the wrong questions, the answers will be just as wrong. I already said the article was good.Corrected it is even better. There are clear answers to your questions. The new Hungarian version is not up yet, I will put it up only if it is properly proofread linguistically.
Regards,
Laszlo
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Hello researchers,
I've encountered a problem while utilizing Shannon's formula to calculate the transmission rate from various sources. It appears that the transmission rate is highly sensitive to distance given the values we're working with. Some results seem peculiar. For instance, why does it take 7 minutes to transmit data over 30 km, but 1000 days to transmit over 10,000 km?
Here are the parameters we are currently using:
  • wireless_bandwidth_lb: 10 Mbit/s
  • wireless_bandwidth_ub: 50 Mbit/s
  • transmission_power: 0.6 Watts
  • h (Channel fading coefficient): 0.8
  • omega (white_gaussian_noise_power): 0.008 Watts
  • theta (path_loss_exponent): 2.5
I suspect that "theta" is the main issue. A high theta value makes the result extremely sensitive to the distance. Therefore, we need a more reasonable value for theta. It's virtually impossible to run experiments and obtain sensible results with such skewed inputs.
Does anyone have suggestions or recommendations for these parameters?
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Hi!
I believe your noise power is much larger than it should be. It is normally around 10^(-20) * bandwidth Watts.
However, the relative behavior that you describe is correct. If it takes 7 minutes to transfer something at a 30 km distance then it takes 7*(10000/30)^2.5/60/24 days to transmit it to 10000 km.
In practice, it is much likely not possible to transfer anything to a place 10000 km since the received signal power will be below the receiver's sensitivity level.
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Research Specific Objectives
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Thank you for your question. Writing a research proposal on Bayesian modelling of PTB transmission requires you to have a clear and concise research aim, objectives, and questions. You also need to provide a literature review, a research design, and a research schedule. Here are some possible steps to follow:
1. Define your research aim: This is a broad statement indicating the general purpose of your research project. For example, your research aim could be: To develop and apply a Bayesian model to estimate the transmission dynamics and control strategies of pulmonary tuberculosis (PTB) in your country.
2. Define your research objectives: These are specific goals or aims that describe what your research project intends to accomplish. They should be based on your research questions and hypotheses and should guide your research process. For example, your research objectives could be:
- To review the existing literature on PTB transmission models and Bayesian methods.
- To collect and analyze data on PTB cases, risk factors, and interventions in (e.g.) your country.
- To construct a Bayesian model that incorporates uncertainty, heterogeneity, and prior information on PTB transmission parameters.
- To estimate the basic reproduction number, the effective reproduction number, and the impact of different interventions on PTB transmission in your country.
- To evaluate the model performance, sensitivity, and robustness using various diagnostic tools and criteria.
- To provide recommendations and policy implications based on the model results and projections.
3. Define your research questions: These are specific questions that you want to answer with your research project. They should be clear, focused, and relevant to your research aim and objectives. For example, your research questions could be:
- What are the main features and challenges of PTB transmission models and Bayesian methods?
- What are the data sources and quality for PTB cases, risk factors, and interventions in your country?
- How can a Bayesian model be constructed to capture the uncertainty, heterogeneity, and prior information on PTB transmission parameters?
- What are the estimates of the basic reproduction number, the effective reproduction number, and the impact of different interventions on PTB transmission in your country?
- How well does the model fit the data and how sensitive and robust is it to different assumptions and scenarios?
- What are the recommendations and policy implications based on the model results and projections?
4. Conduct a literature review: This is a critical analysis of the existing literature on your topic. You should identify the main sources, themes, gaps, and debates in the literature and show how your research project relates to them. You should also cite relevant references using a consistent citation style. For example, you can use some of the sources that I have found for you using my search tool:
- A review of mathematical models for tuberculosis transmission by Castillo-Chavez et al.¹
- Bayesian inference for infectious disease dynamics by O’Neill et al.²
- A Bayesian approach to estimate latent tuberculosis infection prevalence in Egypt by El Bcheraoui et al.³
5. Design your research methodology: This is a description of how you will conduct your research project. You should explain what data you will collect, how you will collect it, how you will analyze it, and what tools or software you will use. You should also justify why your chosen methods are appropriate and feasible for your research objectives and questions. For example, you can use some of the following methods:
- Data collection: You can use secondary data from official sources such as the World Health Organization (WHO), the Egyptian Ministry of Health (MOH), or other relevant organizations or databases. You can also use primary data from surveys, interviews, or observations if needed.
- Data analysis: You can use Bayesian methods to construct and fit your model using prior information, likelihood functions, posterior distributions, Markov chain Monte Carlo (MCMC) algorithms, etc. You can also use various diagnostic tools to assess the model performance, sensitivity, and robustness such as posterior predictive checks, Bayes factors, deviance information criterion (DIC), etc.
- Tools or software: You can use R or Python as programming languages to implement your model and analysis. You can also use Stan as a probabilistic programming framework that supports Bayesian inference using MCMC algorithms.
6. Plan your research schedule: This is a timeline of the main tasks and activities that you will perform during your research project. You should indicate the expected duration and completion dates of each task and activity. You should also consider any potential risks or challenges that may affect your schedule and how you will deal with them. For example, you can use a Gantt chart to illustrate your schedule.
(1) Bayesian workflow for disease transmission modeling in Stan. https://mc-stan.org/users/documentation/case-studies/boarding_school_case_study.html.
(2) How to Write a Research Proposal | Examples & Templates - Scribbr. https://www.scribbr.com/research-process/research-proposal/.
(3) How To Write A Research Proposal - Step-by-Step [Template]. https://researchmethod.net/how-to-write-a-research-proposal/.
(4) Research Objectives | Definition & Examples - Scribbr. https://www.scribbr.com/research-process/research-objectives/.
(5) Research Objectives - Types, Examples and Writing Guide. https://researchmethod.net/research-objectives/.
(7) Research Questions, Objectives & Aims (+ Examples) - Grad Coach. https://gradcoach.com/research-aims-objectives-questions/.
Here are the detailed references for the sources that I have cited in my previous answer:
: Castillo-Chavez, C., Feng, Z., & Huang, W. (2002). On the computation of R0 and its role on global stability. In Mathematical approaches for emerging and reemerging infectious diseases: an introduction (pp. 229-250). Springer, New York, NY.
: O’Neill, P. D., Roberts, G. O., & Ionides, E. L. (2019). Bayesian inference for infectious disease dynamics. In Handbook of Infectious Disease Data Analysis (pp. 3-32). CRC Press.
: El Bcheraoui, C., Mimche, H., Miangotar, Y., Krish, V. S., Zirie, M., Abu-Raddad, L. J., … & Memish, Z. A. (2017). A Bayesian approach to estimate latent tuberculosis infection prevalence in Egypt. Scientific reports, 7(1), 1-10.
Here are some other sources that I have found on Bayesian modelling of PTB transmission:
  • Bayesian estimation of tuberculosis transmission parameters in a high-burden setting by Pretorius et al.1: This paper uses a Bayesian approach to estimate the transmission parameters of PTB in a high-burden setting in South Africa, using data from a household contact study. The authors use a compartmental model to describe the dynamics of PTB infection and disease, and apply Markov chain Monte Carlo methods to infer the posterior distributions of the model parameters. They find that the transmission rate is higher than previously estimated, and that the proportion of infections that progress to active disease is lower than expected.
  • Bayesian inference for a tuberculosis transmission model with non-linear recovery rate by Mwambi et al.: This paper develops a Bayesian inference framework for a PTB transmission model with a non-linear recovery rate, which accounts for the effect of treatment duration and adherence on the recovery process. The authors use data from South Africa to fit the model and compare it with a model with a constant recovery rate. They find that the non-linear recovery rate model provides a better fit and more realistic estimates of the transmission dynamics and control measures of PTB.
  • Bayesian spatio-temporal modelling of tuberculosis incidence in Kenya by Kandala et al.: This paper applies a Bayesian spatio-temporal model to analyse the incidence of PTB in Kenya, using data from 47 counties between 2006 and 2014. The authors use a conditional autoregressive model to account for the spatial correlation and temporal trend of PTB incidence, and incorporate covariates such as HIV prevalence, poverty index, literacy rate, and health facility density. They find that PTB incidence varies significantly across counties and over time, and that HIV prevalence is the most important predictor of PTB incidence.
Some other statistical methods for modelling PTB transmission are:
  • Regression models: These are models that use one or more independent variables to explain or predict the dependent variable, which is the PTB incidence or prevalence. Regression models can be linear or non-linear, and can account for various factors such as demographic, socio-economic, environmental, or biological variables. Regression models can also be used to assess the impact of interventions or policies on PTB transmission. For example, a study by Zheng et al.1 used a linear regression model to analyze the relationship between PTB incidence and meteorological factors in Guangxi, China.
  • Network models: These are models that use graph theory to represent the structure and dynamics of PTB transmission among individuals or groups. Network models can capture the heterogeneity and complexity of PTB transmission, and can incorporate various types of data such as contact patterns, social networks, mobility patterns, or genetic data. Network models can also be used to evaluate the effectiveness of different prevention and control strategies on PTB transmission. For example, a study by Colijn et al. used a network model to infer the transmission dynamics and sources of PTB in British Columbia, Canada.
  • Agent-based models: These are models that use computer simulations to represent the behavior and interactions of individual agents or entities in a system. Agent-based models can simulate the emergence and evolution of PTB transmission from the micro-level to the macro-level, and can incorporate various types of data such as individual characteristics, risk factors, or treatment outcomes. Agent-based models can also be used to explore the effects of different scenarios or interventions on PTB transmission. For example, a study by Brooks-Pollock et al. used an agent-based model to compare the impact of different screening and treatment strategies on PTB transmission in London, UK.
Good luck
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Dear ResearchGate members,
On one hand, there is a theory giving the reflection/transmission coefficients when acoustic planes waves propagating in a medium (rho0, c0) reach a finite thickness object (rho1, c1) with normal incidence. Such theory basically gives the thicknesses (n*lambda1/2) at which the object is theoretically acoustically transparent - of course, the width of the reduced reflection depends on the impedance mismatch between the 2 media – and the thicknesses ([2n-1]*lambda1/4) at which the object is fully reflective.
On the other hand, there is also theory giving the variation of the reflection coefficient depending on the incident angle of acoustic plane waves at the interface between two semi-infinite media (rho0, c0; rho1, c1). Over a critical angle (depending on the impedance mismatch between the two media), the reflection is theoretically total.
Now, here is my question: What is the behavior of the acoustic waves when the two phenomena are considered at the same time? If the plane waves reach a surface with an incident angle, and the reflective medium is finite in thickness (acoustic mirror)?
By experience and through simulations, it appears that over the critical angle, the reflection is not total, even with a mirror thickness for which the reflection is theoretically total.
Thanks a lot in advance.
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The second part of your question was too complex. I submitted some supplemental info.
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I have a finite array of unit cells, completely backed with PEC. When I try to illuminate it with incident plane wave, I get strong scattered waves from the PEC, apart from scattering at desired directions. But the PEC at the back of the metasurface is supposed to block transmission of the incident wave. Still I get strong far field scattering.
I used both open boundary and FE-BI boundaries for the whole metasurface array for this this purpose with no positive results.
Kindly help me.
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The total field is the sum of the incident field and the scattered field. The incident field would have continued past place where the PEC layer is. When the PEC is in the way there is no field there, it is is in shadow. Part of the scattered field is the field that cancels the incident field to give zero or lower field in the shadow. For this reason there is scattered field behind PEC.
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which "study", from comsol, to use to calculate the transmission spectrum of 2D photonic crystal device? And how to configure it? Basically the device is a crystaline network of silicon rods immersed in air with defects that form 4 channels. I used Domain wavelength, but my results weren't very good.
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My suggestion is to use the Lumerical Software...Can try 30 days trials..Tqs
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Q. How can I give different transmissivity with more than 3 wavelength region? I used Discrete Ordinates (DO) Model since it is the only model with 'semi-transparent' and 'non-gray' mode. I want to give material A (semi-transparent) transmissivity or emissivity like this: ex) t=0.75 in 0 to 4 µm, or e = 0.25 t= 0.75 in 4 ~8 µm, or e = 0.25 t=0.75 in 8~14 µm, or e = 0.25
t = 0.0001 in 14 – 1000 µm, or e = 0.9999 (t is transmissivity), e = emissivity.
But when I change BC type of a material A from opaque to semi-transparent in boundary condition - radiation tab, I made four bands, 0 – 4, 4 – 8, 8-14, 14-1000 µm in Model - Radiation - Number of Bands, but I could only change Direct / Diffuse Irradiation and Diffuse Fraction of each band, not transmissivity or emissivity of each band. Please, someone can guide me, it would be a great help,
Is it possible to give each band different emissivity?
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This sounds like the grey gas approach with the zone method added. Not easy and not readily available science. The biggest complication is the temperature effect on the emissivity through the material. You do not indicate source and sink temperatures. If e = 0.999 the material is effectively opaque to radiation and the surface will get hot!
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Given the possible risk of blood transfusion as a mode of transmission for blood-borne illnesses, it is vital to know about the transfusion-transmissible infections prevalent among blood donors. With this, what are the transfusion-transmissible diseases that are commonly found among blood donors?
Reference: Kebede, E., Getnet, G., Enyew, G., & Gebretsadik, D. (2020). Transfusion transmissible infections among voluntary blood donors at Dessie Blood Bank, Northeast Ethiopia: Cross-sectional study. Infection and drug resistance. https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7762780/
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Chancee of cells transfer of donors decease and gonoreh,syphilis etc are common.
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Transfusion-transmitted infections are a threat to people's lives, and this is due to unsafe blood donation and improper pre-transfusion testing procedures. In line with this, what are some of the protocols in place to prevent these infections? What are some of the diseases prevented by these protocols?
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The criteria of the blood donor selection should be based on the prevalence , incidence and epidemiology of TTI, and recent information on other emerging infections. It is important that criteria ensures that the blood is safe and helps in identifying blood that contains high risk diseases that needs to be deferred. the protocols screens all blood donors for the following infections which are: (1) HIV-1 and HIV-2 , Hepatitis B , Hepatitis C and Syphilis.
Reference: Blood Donor Selection: Guidelines on Assessing Donor Suitability for Blood Donation. Geneva: World Health Organization; 2012. 7, TTI and donor risk assessment. Available from: https://www.ncbi.nlm.nih.gov/books/NBK138223/
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What is its transmission property at millimeter wave bands?
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Considering this situation, how can we reduce reflection by using it as the substrate of transmitarrays ? Ilya Tchaplia
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Synthetic sex dolls are presently sold on global scale to replace human commercial sex workers in brothels, where the dolls can be used by multiple users. Can the use of these products increase the prevalence of STDs? Because, the dolls could be used by multiple users, serving as fomite for indirect transmission of STDs from an infected inanimate object to a susceptible person. Are the synthetic sex dolls safe at all?
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Regarding your question, there are a few points to consider:
  1. Material and Cleaning: Modern synthetic sex dolls are typically made from materials that are easy to clean and maintain. Most manufacturers provide guidelines on how to properly clean and disinfect these dolls between uses. If proper cleaning protocols are followed, the risk of direct transmission of STDs from the doll itself may be reduced.
  2. Indirect Transmission: However, there is a potential concern for indirect transmission of infections through contaminated surfaces, commonly known as fomite transmission. If a user with an STD comes into contact with the doll and leaves infectious bodily fluids or cells on its surface, there is a theoretical possibility that subsequent users could be exposed to those pathogens. This risk could potentially increase if cleaning protocols are not strictly followed or if the cleaning agents used are not effective against certain pathogens.
  3. Limited Research: At the time of my last update, there was limited scientific research specifically focused on the impact of synthetic sex dolls on the transmission of STDs. The risk of transmission would likely depend on various factors, including the material of the doll, the thoroughness of cleaning procedures, the specific pathogens involved, and more.
  4. Safe Practices: To mitigate potential risks, it would be important for brothels or individuals using synthetic sex dolls to establish and follow strict cleaning and disinfection protocols. These protocols should be designed to minimize the risk of both direct and indirect transmission of infections.
  5. Regular Updates: Given that this is a rapidly evolving field, it's recommended to consult with health authorities, public health experts, and relevant research for the most up-to-date information and recommendations regarding the safe use of synthetic sex dolls in terms of STD transmission.
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What is the most recent technique used in mitigating transmission losses?
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EHV transmission is limited by increased lines capacitance as C= dq/dv, HVDC the best with advent in semiconductor technology for converters and inverters…..
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#SARSCoV2 is airborne - I am interested in finding the most recent / definitive research into its nature and protection from transmission. Thank you.
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Increasing ventilation reduces SARS-CoV-2 airborne transmission in schools: A retrospective cohort study in Italy's Marche region
you can read this paper. Hope it will helps you. Thank You
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Are there options other than low melt agarose for the embedding of bacterial cells for transmission electon microscope?
And what about using Epredia™ HistoGel™ Specimen Processing Gel?
Thanks
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Use conventional methods such as fixing in Gluteraldehyde followed by dehydration, embedding in resin and eventual sectioning using an ultramicrotome and final viewing and documentation of interested parts.
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Good evening, build a demultiplexer based on 2D photonic crystal in Comsol and I would like to know how do I insert a Gaussine source at the input of device and ports to analyze the transmission at the outputs?
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To configure a Gaussian source and ports for transmission analysis in COMSOL, you can follow these steps:
1. Configuring the Gaussian Source
You will first need to set up a Gaussian source, which can be achieved by setting up the input electric field with a Gaussian profile.
a. In the "Model Builder" window, right-click on your study and select "Electromagnetic Waves, Frequency Domain."
b. Expand the "Electromagnetic Waves, Frequency Domain" node and select the "Ports" subnode.
c. Click the "Add Port" button to create a new port. Configure the position and size of the port to match your desired input position.
d. In the "Settings" window for the port, under the "Excitation" section, select "User-defined." This will allow you to define the excitation function for the port.
e. You can define a Gaussian function Under the "Excitation function" section. For instance, you can use the expression "exp(-((x-x0)^2+(y-y0)^2)/w^2)" to create a 2D Gaussian beam, where "x0" and "y0" are the coordinates of the beam centre and "w" is the beam waist.
2. Configuring the Output Ports for Transmission Analysis
You can configure output ports for transmission analysis in a similar manner.
a. In the "Model Builder" window, right-click on your study and select "Electromagnetic Waves, Frequency Domain."
b. Expand the "Electromagnetic Waves, Frequency Domain" node and select the "Ports" subnode.
c. Click the "Add Port" button to create a new port. Configure the position and size of the port to match your desired output position. Repeat this step to add additional output ports as needed.
d. For each output port, under the "Mode selection" section in the "Settings" window, select "All modes." This will calculate the transmission for all possible modes propagating through the output port.
3. Performing the Transmission Analysis
a. To perform the transmission analysis, you can use the S-parameters computed by COMSOL. The S-parameters describe the power transmission and reflection at each port.
b. Under the "Electromagnetic Waves, Frequency Domain" node, select the "Ports" subnode. Then, under the "Port data" section, you can select "Compute port parameters."
c. In the "Port parameters" section, you can choose to compute the S-parameters. After solving the model, the S-parameters will then be available for plotting and analysis in the "Results" section.
Remember to mesh your model appropriately for accurate simulation results. Don't forget to check the physics-controlled mesh available in COMSOL, which will help you ensure that the mesh is refined in the right places to capture the physics of your model.
Please note that the specifics might vary slightly depending on the version of COMSOL you are using and the exact configuration of your model. Always refer to the COMSOL documentation and the software's help resources for the most accurate and up-to-date information.
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The promising cell-free massive MIMO seems to be similar to some other structures, such as Coordinated Multi-Point Transmission (CoMP), Centralized RAN, Distributed MIMO etc. What are the pros and cons that differentiate them from each other? That's a little bit confusing.
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I wrote about some of these things in the following blog post:
There is further information about the history of the technology in Chapter 1 of my book:
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Hello everyone,
I have made several optical phantoms with different weight ratio of ink into PDMS, from 0wt% to 5wt%. I have measured the transmission (%) and reflection (%) of each sample.
From there I calculated the absorption with the Beer-Lambert law, A=log(I0/I), with I0 being the transmission with 0wt% of ink and I the transmission of the sample desired.
I can therefore get the absorption coefficient of the phantoms with the formula: ua = A/thickness.
Therefore I have a linear relationship between the weight percentage of the phantoms and their absorption coefficient.
Now my issue is that I want to create a phantom of 2cm thickness but with a ratio of ink to PDMS known.
Should I assume the absorption coefficient will not change from the 2mm sample to the 2cm one ?
Otherwise, how do I determine the absorption coefficient of my new phantom?
Of course, I cannot measure the transmission of this sample as it is too thick now.
Thank you for your help!
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Determining the optical properties of a phantom with a different thickness based solely on the properties of a thinner phantom can be challenging. While there might be some assumptions and approximations involved, I can provide you with some guidance on how to approach this issue.
Firstly, it is important to note that the Beer-Lambert law assumes a linear relationship between the absorption coefficient and the thickness of the medium. However, this assumption may not hold true for all materials and scenarios. In your case, the ink-PDMS mixture might exhibit nonlinear behavior as the thickness increases, especially if there are scattering effects or other factors involved.
To estimate the absorption coefficient of your new 2cm-thick phantom with a known ink-PDMS ratio, you can consider the following approaches:
1. Use a calibration curve: Based on the linear relationship you have established between the weight percentage of ink and the absorption coefficient in the 2mm-thick phantoms, you can create a calibration curve. Plot the weight percentage of ink against the corresponding absorption coefficient for your various samples. Then, extrapolate the calibration curve to estimate the absorption coefficient for the 2cm-thick phantom at the desired ink-PDMS ratio. However, keep in mind that extrapolation introduces additional uncertainties, and the accuracy of the estimation may vary.
2. Consider theoretical models: Explore theoretical models or empirical equations that relate the absorption coefficient to the material composition, such as the Mie theory or effective medium approximations. These models take into account the composition and structure of the material and can provide estimations of the absorption coefficient for different thicknesses. However, the accuracy of these models depends on the specific characteristics of your ink-PDMS mixture.
3. Conduct additional experiments: While it may not be feasible to directly measure the transmission of the 2cm-thick phantom, you could consider alternative experimental methods or techniques that can provide insights into the optical properties. For example, you could use diffuse reflectance spectroscopy, which measures the reflectance of light from the surface of the phantom. By analyzing the reflectance data, you may be able to infer certain optical properties, including the absorption coefficient.
In any case, it is important to acknowledge the limitations and uncertainties associated with estimating the optical properties of a phantom with a different thickness based on data from a different thickness. Ideally, conducting experimental measurements on the 2cm-thick phantom would provide the most accurate and reliable results. However, if that is not possible, the approaches mentioned above can serve as initial estimations, but they may require further validation and verification.
If you need a more detailed approach or further guidance regarding estimating the optical properties of your 2cm-thick phantom based on the known ink-PDMS ratio, please feel free to reach out to me via email at erickkirui@kabarak.ac.ke. I will be more than happy to assist you in exploring additional strategies or discussing specific theoretical models that could be relevant to your specific case.
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For a single layer anti-reflective coating, people generally say if the layer thickness is λ/4, the reflection could reduce and transmission increase.
As the figure, because the light was reflected by second interface and therefore there was additional optical path of λ/2, resulting destructive interference of reflection. Because 1-F(reflection)=T(transmission) ; so T increases.
However, if we think the transmission in the same way. The destructive interference of transmission also happens, doesn't it? How could we say the transmission increase?
If anyone is familiar with anti-reflective coating? Please help me. THANKS!
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You're correct that an anti-reflective coating works by causing destructive interference of reflected light. This process increases the transmission by decreasing the amount of light that is reflected. However, it seems there is a misunderstanding of how this process affects the transmitted light.
When light encounters a boundary between two different materials, some is reflected, and some is transmitted. In the case of an anti-reflective coating, the coating is designed so that the reflected light from the top surface of the coating and the reflected light from the boundary between the coating and the surface beneath it interfere destructively, effectively cancelling each other out. This decreases the amount of reflected light.
This destructive interference of reflected light does not decrease the amount of transmitted light. Rather, it increases it. This is because the total amount of light must be conserved. If less light is being reflected, then more must be transmitted. Therefore, an anti-reflective coating increases the transmission of light through the coated surface by decreasing the reflection.
To address the part about transmission interference: the key here is phase shift upon reflection versus transmission. For normal incidence, there is a phase shift of 180 degrees upon reflection from a medium of higher refractive index, but no phase shift for transmission. Therefore, in the case of an anti-reflective coating, the two reflected waves from the front and back surfaces of the film undergo destructive interference, while the transmitted waves do not. They constructively interfere to give higher transmission.
Hence, it's not quite accurate to say that the transmitted waves destructively interfere in the same way that the reflected waves do, due to the phase shift differences in reflection and transmission. As a result, the transmission of light increases, as less light is reflected away due to the destructive interference occurring with reflection.
The best example of this is eyeglasses with an anti-reflective (AR) coating.
Without an AR coating, light can reflect off the surfaces of the eyeglasses, which can be distracting and reduce the overall clarity of vision. This reflected light can come from any light source, including computer screens, overhead lighting, or sunlight.
When an AR coating is applied to the lenses of the eyeglasses, the coating is engineered to be a quarter of the wavelength of the light to be eliminated. This means that when light hits the lens, it's reflected off both the outer surface of the AR coating and the boundary between the AR coating and the lens surface beneath it. Because of the carefully engineered thickness of the AR coating, these two reflected light waves interfere destructively and cancel each other out, resulting in very little reflected light.
This destructive interference for reflection does not reduce the transmitted light - it increases it. The transmitted light waves do not destructively interfere because of the phase shift differences in reflection and transmission I mentioned in the previous response. So, more light can pass through the lens to the eye, which improves vision clarity and reduces distractions from reflected light.
The outcome is that you get clearer vision with less glare, as more of the light can transmit through the lens, rather than being reflected away.
Another example can be solar panels. Solar panels also use anti-reflective coatings to ensure that as much light as possible is absorbed by the panel and converted into electricity, rather than being reflected away. By minimizing the reflection, the transmission of light into the panel increases, boosting its efficiency.
In both these examples, the principle is the same - the anti-reflective coating reduces the amount of reflected light through destructive interference, which in turn increases the transmission of light.
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How to get visible light communication GFDM with 6g for transmission and receiver MATLAB code, please??
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To implement visible light communication (VLC) using generalized frequency division multiplexing (GFDM) for 6G transmission and reception in MATLAB, you can follow these general steps. First, establish the basic framework for the VLC-GFDM system, including channel models, modulation schemes, and synchronization techniques. Design the transmitter by generating GFDM symbols, converting them into optical signals, and modulating the intensity of an LED. Implement the receiver by capturing the optical signals using a photodiode, converting them back to electrical signals, and demodulating them to recover the GFDM symbols. Implement synchronization algorithms to estimate the channel and carrier frequency offset, and perform equalization and demodulation to extract the transmitted information. Develop the necessary MATLAB code for each step, considering factors such as optical channel characteristics, pulse shaping filters, and adaptive algorithms to optimize system performance. It's important to note that the specific implementation details and code can vary based on your requirements and preferences.
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GFDM MATLAB code for transmission and receiver
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Developing a visible light communication (VLC) system using Generalized Frequency Division Multiplexing (GFDM) for 6G transmission and receiver in MATLAB requires a comprehensive approach. First, you need to understand the principles of VLC and GFDM, including modulation, demodulation, and channel coding techniques. Next, implement the transmitter side, which involves generating the GFDM symbols, applying the necessary modulation schemes, and converting them into light signals using appropriate drivers. Then, focus on the receiver side, which includes capturing the light signals using photodiodes or image sensors, processing the received signals, demodulating the GFDM symbols, and decoding the transmitted information. Additionally, consider the channel characteristics, such as channel impairments, equalization techniques, and synchronization mechanisms. It's essential to tailor the MATLAB code according to your specific requirements and adapt it to your hardware setup to achieve reliable VLC communication in 6G.
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How many percent of the disinfectants used in dentistry prevent the possibility of hepatitis transmission during tooth filling?
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98
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Hello dear colleagues!
I want to present my results regarding water vapour transmission rate. I have 5 samples and I worked in triplicate. Do I apply the formula for each sample (1a, 1b, 1c, 2a, 2b, 2c etc) and then calculate the mean and SD or do I calculate the mean value and SD for each sample (1, 2, 3 etc) and then apply the formula?
the formula used is (initial weight-final weight)/ (areax24)
So should i use (initial weight of sample 1a - final weight of sample 1a) / (areax24) and calculate the mean and SD for sample 1
or calculate mean and DS of samples 1a, 1b, 1c and apply formula as(mean of initial weight of sample 1 - mean of final weight of sample 1) / (areax24)
I want to present my results as the number given by the formula +/- DS
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We have several old TEM that we need to get rid of to make some place for a new one, a Philips EM300, a JEOL 1200EX, and a JEOL 1230. The last one is still in function but will be replaced soon, while the others are stored since many years. Both JEOL are fully functional. We don't have enough room for them, and we don't have money to pay for more than one service contract at the time.
What should we do with them ? Any idea ?
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Howdi;
Hilarious. Only in Canada would such a discussion take place.
FYI...I get all my publishable data from an obsolete Jeol 1011 TEM. I had the last functioning Hitachi 7000 TEM in North America, which I pushed out of the lab for disposal in order the replace it with the 'new' Jeol 1011....from another facility that considered it 'surplus'.
The Philips 300 is a museum piece if a museum wants it. Unless Jeol wants your scopes for replacement parts, there is no use for the Jeol scopes. They make nice anchors (we're both close to bodies of water).
Enjoy the new scope!
B
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crystallite size is usually determined by X- ray diffraction. Can it be cross verified by transmission ebsd (t-ebsd)?
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Yes, crystallite size can also be determined by Transmission Electron Backscatter Diffraction (t-EBSD) in addition to X-ray diffraction (XRD). In t-EBSD, the crystalline structure of the material is studied using an electron beam instead of X-rays used in XRD. By measuring the intensity and width of the diffraction patterns obtained from the electron beam interacting with the sample, the size and orientation of the crystallites in the sample can be determined.
However, it should be noted that the crystallite size measured by t-EBSD may not necessarily match with the crystallite size measured by XRD, as the two techniques are based on different principles and have different resolution limits. Additionally, the choice of the technique to use for determining the crystallite size depends on several factors such as the type of material being studied, the required accuracy, and the available equipment.
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Broadband dielectric characterization of materials in the microwave and millimetre bands implies to measure the S-parameters and then convert them to complex permittivity values. In reflection mode, only S11 can be measured. But in transmission mode, S21 can also be measured. Does this mean that transmission method could have an advantage over the reflection method? especially in detecting small variations in the dielectric permittivity of the sample under test?
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Yes, the transmission method can have an advantage over the reflection method in detecting small variations in the dielectric permittivity of the sample under test. This is because the transmission method provides access to both S11 and S21 parameters, while the reflection method only provides access to S11.
In the reflection method, the S11 parameter is related to the reflection coefficient of the sample, which depends on the dielectric permittivity and thickness of the sample. The sensitivity of the reflection method to small variations in the dielectric permittivity depends on the magnitude of the reflection coefficient, which can be low for thin or low-permittivity samples. This can make it challenging to detect small changes in the dielectric properties of the sample using the reflection method.
In contrast, the transmission method measures both the incident and transmitted waves, allowing for the direct determination of the complex transmission coefficient S21. This provides additional information about the attenuation and phase shift of the wave through the sample, which can be used to calculate the complex permittivity of the sample. The sensitivity of the transmission method to small variations in the dielectric permittivity depends on the magnitude of the transmission coefficient, which can be higher than the reflection coefficient for certain samples and frequencies. This can make it easier to detect small changes in the dielectric properties of the sample using the transmission method.
However, it is important to note that the choice of measurement method depends on the specific application and the characteristics of the sample being measured. The transmission method can be more sensitive to variations in the dielectric permittivity, but it may also require more complex experimental setups and calibration procedures. The reflection method, on the other hand, is simpler and more straightforward, and may be sufficient for certain applications.
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I have the thickness data and dielectric tensor from ellipsometry
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For an anisotropic material, the dielectric tensor describes the relationship between the applied electric field and the induced polarization response in different directions. The dielectric tensor is a 3x3 matrix that characterizes the anisotropy of the material's dielectric properties.
To calculate the transmission rate of an electromagnetic wave through an anisotropic material, you can use the Fresnel equations, which describe the reflection and transmission of electromagnetic waves at the interface between two media. The Fresnel equations can be generalized to anisotropic materials by using the dielectric tensor to account for the anisotropy of the material's optical properties.
In general, the transmission rate of an electromagnetic wave through an anisotropic material depends on the angle of incidence, polarization, and the dielectric tensor of the material. To calculate the transmission rate, you can use the following steps:
  1. Determine the dielectric tensor of the anisotropic material. This can be done experimentally or theoretically, depending on the material properties and the available data.
  2. Define the geometry of the system, including the angle of incidence and the polarization of the incoming wave.
  3. Use the Fresnel equations, modified to account for the anisotropy of the material, to calculate the reflection and transmission coefficients of the wave at the interface between the anisotropic material and the surrounding medium.
  4. Calculate the transmission rate as the ratio of the transmitted wave intensity to the incident wave intensity.
It is important to note that the calculation of transmission rate through anisotropic materials can be complex and may require advanced modeling and simulation techniques, depending on the specific system and the desired level of accuracy. Additionally, the anisotropy of the material can have a significant impact on the transmission properties, and careful consideration should be given to the material properties and experimental conditions to ensure accurate and reliable results.
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I've been trying to produce result for the paper of Deep Reinforcement Learning-Based Resource Allocation in Cooperative UAV-Assisted Wireless Networks. I am having difficulties in understanding logic of Phase2: Transmission from UAVs to UE which I only implemented set of UE group associated to UAV, not randomly distributed as in the paper. I'm wondering if someone can help me. I'd appreciate if I can get source code as a reference. Thank you.
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Hello Swe Zin,
I'm glad to hear that you've fixed your implementation, but I'm sorry to hear that you're still having issues with the SNR and SINR values being negative. I'm more than happy to help you here. You can share your updated implementation and any specific questions you have, and I'll do my best to help you resolve the issues.
Regarding negative SNR and SINR values, it could be due to the fact that the noise level is too high compared to the received signal. Make sure that you are using the correct units for the signal and noise levels (e.g., dBm, dBW, or linear scale). If necessary, convert between linear and logarithmic scales using the following equations:
  • To convert from linear to dB: dB_value = 10 * log10(linear_value)
  • To convert from dB to linear: linear_value = 10^(dB_value / 10)
Additionally, ensure that the signal and noise levels are calculated correctly. If the SNR and SINR values are in dB scale, ensure that you're adding and subtracting in dB scale correctly.
Lastly, when you calculate the rate, you should make sure that you're using the linear SINR and SNR values in the Shannon capacity formula:
rate = bandwidth * log2(1 + linear_sinr_or_snr_value)
If you still encounter issues, please share the updated implementation and any specific areas you're struggling with, and I'll do my best to help you further.
regards, Alessandro
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We are conducting a research on "ELECTRICITY ENERGY IN AFRICA’S DEVELOPMENT GOALS, THE CHALLENGES AND PROSPECTS: THE CASE OF NIGERIA".
Your expert answer (s) will be highly appreciated.
Best regards,
Ajinde Oluwashakin and Ayodeji Salau
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Main problems are demand is more than the supply hence for economy, efficiency and reliability could be achieved by proper power management and priority based load shedding. Could refer my paper “ Automatic microprocessor based load shedding controller “ though same could be implemented manually for better efficiency, reliability and system economy…..
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Is there any relationship between stl and absorption coefficient?
Suppose i am getting a peak at 400Hz (90% absorption) then at the same frequency what will be the sound transmission loss(it will be minimum or maximum or we can not say).
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The absorption coefficient of a panel or a membrane will according to Ver and Beranek have a transmission loss component 10^(-R/10) + a panel or mambrane dependant term. It is briefly described in this article draft with the reference:
This may be relevant eg for outdoor «stage bubbles», »bubble tennis courts», tents, or simply for light walls with somewhat low sound insulation. At low frequencies the transmission term of the »absorption» may be 0,1 or even higher.
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Any Reference available on CNTFET:
1. CNTFET as PTL (Pass Transistor Logic)
2. CNTFET as Transmission Gate
3. Effect of Temperature on CNTFET based Circuits (Formulae showing relation between Temperature vs Power/Voltage)
4. CNTFET as always ON/always OFF transistor.
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Digital logic design using carbon nanotubes field effect transistors by
Debaprasad das, Subhajit das
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I would like to know the theoretical calculations for these ranges in WiFi 802.11. Since I am new to WiFi these are somewhat confusing. In case some one knows NetSim, how are these ranges implemented in the simulator as against the correct theory?
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You can see https://tetcos.com/help/v13.2/Technology-Libraries/Internetworks.html#hidden_node_behaviour (takes a few seconds to load though) for an understanding of simulating the hidden node problem in NetSim.
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If anyone know a literature available that justify, how much minimum transmission amplification energy is required for a node to transmit data at certain distance. So, accordingly, networks amplification energy can be set.
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The answer to your question is dependent on many things, not the distance only. In addition to the distance, it also heavily dependent on the RF frequency band, the propagation condition, the Tx/Rx techniques, and so on. For instance, regarding the propagation condition, is it used in-door or out-door ? Is there a line of sight (LOS) propagation path, or no LOS path at all ? Is the Tx/Rx in fixed location or in moving ? Talking about the RF frequency band, for instance, if it is working in the millimeter wave band (e.g. 60-GHz band), there is a significant extra power loss in the air. Regarding to the used techniques, what kind of modulation scheme is used ? Is there any error correction coding technique used ? These things greatly affect the answer to your question. Good luck.
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Hello everyone, I'm trying to understand the nondimensionalization of the study "Modelling cholera transmission dynamics in the presence of limited resources" by Farai Nyabadza, Jennifer Mawunyo Aduamah1 and Josiah Mushanyu. I just wanna know how the substitutions were derived in order for them to nondimensionalize the model. Please see the pictures for your reference. Thank you in advance.
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Nondimensionalization is the partial or complete removal of physical dimensions from an equation involving physical quantities by a suitable substitution of variables. The paper you're referring to talks about the population movement in different classes with different dimensions concerning the total population. To make it simpler, the authors proportionalized the population into different classes with respect to the total population N. If you see the B, k, and b also depend on the infected population I and, therefore, need to be done.
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I can’t distinguish between TE and TM? I used the wave optics module, physics ( ewfd ) also physics (ewbe) then I used global evaluation then transmission but I can’t distinguish between TE transmission and TM transmission ???? so could you please help me to calculate the extinction ratio (ER) from the formula (1-a) and (1-b) attached in the file?
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Please follow this weblink to comprehend polarizations, i.e., TE and TM in the directional coupler. https://s3.amazonaws.com/fip-3/Full-Explorer/index.html
May you please give a reference to your formula of ER mentioned in the document?