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Emission - Science topic
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May 14, 2025
This section formulates the ECM-based mechanical interpretation of electrical conduction through massive charge carriers, primarily electrons, in conductive media. Unlike photons, electrons possess positive matter mass (Mₑ), and their kinetic behaviour under applied electric potential reveals the presence of an associated negative dynamic mass component (−Mₐₚₚ), consistent with ECM's mass-energy coupling. The ECM force law is thus adapted for charged particles as:
Fₑ𝚌ₘ = (Mₑ + (−Mₐₚₚ))·aₑ𝚏𝚏,
where Mₐₚₚ = ΔMₑ represents the negative apparent mass arising from the electron’s motion-induced kinetic energy. The applied potential establishes an effective acceleration field across the conductor, leading to the directed flow of electrons, photon emission (as kinetic energy release), and field induction—especially enhanced in coiled geometries. Further, the saturation of outermost or free electrons with absorbed photon energy limits additional energy absorption, redirecting incoming energy into motion and electromagnetic emission. This ECM perspective provides a unified dynamic explanation for charge flow, energy transfer, and electromagnetic field generation in conductive systems, rooted in mass-energy redistribution rather than abstract field formalism.
Regards,
Soumendra Nath Thakur
I am writing to invite you to submit a chapter to an edited monograph, titled The End is Nigh: Climate Anxiety in the Classroom, that explores the multiple ways in which climate anxiety permeate and serve to disrupt students’ and teachers’ mental health within kindergarten to grade 12 classrooms.
The monograph book is a contemporary examination of the state of climate anxiety within the field of education. Climate change is one of the most pressing issues of our time. While some continue to deny its existence and question human’s contributions to its effects, climate change is an undeniable fact (e.g., IPCC, 2018; IPCC, 2022). Media addresses climate change by describing it using doomsday language such as catastrophic, urgent, irreversible, and devastating. Popular climate change advocate Greta Thunberg (2019) reinforces the fear by stating, "I don’t want you to be hopeful. I want you to panic. I want you to feel the fear I feel every day. And then I want you to act. I want you to act as you would in a crisis. I want you to act as if our house is on fire. Because it is." (para. 20)
With extensive exposure to the negative impact climate change can have on individuals, their family, community, and the world, it is not surprising that individuals are experiencing climate anxiety (Albrecht, 2011; Clayton, 2020; Maran & Begotti, 2021; Ojala, 2015; Reyes et al., 2021, Weintrobe, 2019). The impact of climate change on mental health is not limited to those who have lived through a natural disaster associated with climate change (Howard-Jones et al., 2021). Within schools, classroom discussions and analysis of the effects of climate on one’s country and across the global may affect students’ and teachers’ mental health in the form of climate anxiety (Helm et al., 2018; Maran & Begotti, 2021). As schools play a key role in the educating students about climate change it is essential that we understand the presence of climate anxiety within our classrooms and its impact on teachers and their students.
As such, this book will offer a global dialogue, critically scrutinizing academic and practical approaches to address the universal challenges associated with climate anxiety within elementary, middle, and high schools. Authors from a variety of nations, will illustrate that climate anxiety is a world-wide phenomenon, that is often neglected from climate change dialog.
Within our call for chapters, we invite contributions that explore the following three themes:
Theme 1: Climate Anxiety within Schools
• Theoretical foundations of climate change education and anxiety
• Intersectionality of culture and climate anxiety within the classroom
• Theoretical foundations of climate change education and anxiety
• Principles of sustainable education, mental health, and climate anxiety
• Pedagogical perspectives of anxiety, sustainable education, and climate change education
Theme 2: The Impact of Climate Anxiety on Students and Teachers
• Evaluation of student and teacher experiences related to climate anxiety.
• Exploration of the psychological manifestation of climate anxiety in students and teachers.
• Critical examination of how climate anxiety impacts students’ learning and development.
• Description of how climate anxiety occurs within the classroom.
• Critical examination of how curriculum generates climate anxiety.
• Critical examination of the impact of climate anxiety on teaching praxis
Theme 3: Addressing Climate Anxiety
• Description of innovative and creative approaches to address climate anxiety in school settings.
• Description of pedagogical strategies to address students’ climate anxiety.
• Exploration of how climate anxiety should be addressed within schools.
• Rebuilding a cohesive learning environment after climate change induced disasters.
• Lessons learned from the challenges and successes of combating climate anxiety.
• Examining the need of policy and administrative support for addressing climate anxiety.
The editors are interested in a range of submissions and encourage proposals from a variety of practitioners within the field of education including, academics, educators, administrators, and graduate students. Submissions should include theoretical stances and practical applications.
Audience:
The book will be useful in both academic and professional circles. The intended audience for this book includes school administrators, educators, and advocates of climate change and reform, all of whom may find this book to be a useful teaching resource. In addition, the book can be used in a variety of courses graduate and undergraduate courses, including, but not limited to: educational psychology, curriculum development, current issues in education, methods and pedagogy, international education, and education law.
Proposals:
All submissions must be written in English.
Please submit as a PDF file for compatibility.
Prospective contributors should submit a 1000-word overview (excluding abstract) of their proposed chapter, including:
• Title
• Abstract – 250 words
• Contact information including name(s), institutional affiliation(s); email and phone number.
• A description of the chapter’s central argument that includes how your chapter addresses one of the central themes of the book.
• A clear explanation of the research underpinning any assertions, as well as the main argument, purpose and outcomes presented in the chapter.
• Where chapters will draw on specific research projects, we’d expect some detail in relation to the type of research, period, data set and size, and of course, the findings.
• 3-5 key words/phrases.
Font: Times New Roman size 12 font, double-spaced.
Please adhere to APA, 7th edition formatting standards.
Contributors will be sent chapter format and guidelines upon acceptance. Full manuscripts will be sent out for blind peer review.
Final Chapters:
Final papers should be approximately 7000 words, not including references.
Review Process:
Each author will be asked to review one chapter from the book and provide feedback to the author(s) and editors.
Important dates
Submission of title, abstract, and author(s) to editors - June 1, 2023
Notification of acceptance to authors - Sept 1, 2023
Submission of full manuscript to editors - January 8, 2024
Feedback from editors to authors - March 1, 2024
Submission of revised manuscripts to editors - May 1, 2024
Please send your submissions to: juliec@nipissingu.ca
Please feel free to contact the editors directly with any questions/queries:
Dr. Julie K. Corkett juliec@nipissingu.ca
Dr. Wafaa Abdelaal w.abdelaal@squ.edu.om
References:
Albrecht, G. (2011). Chronic environmental change: Emerging ‘psychoterratic’ syndromes. Climate Change and Human Well-being. New York. Springer. pp 43-56.
Clayton, S. & Karazsia, B. (2020). Development and validation of a measure of climate anxiety. Journal of Environmental Psychology, 69, 101434. https://doi.org/10.1016/j.jenvp.2020.101434
Helm, S.V., Pollitt, A., Barnett, M.A., Curran, M.A., & Craig, Z.R. (2018). Differentiating environmental concern in the context of psychological adaption to climate change. Global Environmental Change, 48, 158–167. https://doi.org/10.1016/j.gloenvcha.2017.11.012
IPCC (2018). Annex I: Glossary In Masson-Delmotte, V., P. Zhai, H.-O. Pörtner, D. Roberts, J. Skea, P.R. Shukla, A. Pirani, W. Moufouma-Okia, C. Péan, R. Pidcock, S. Connors, J.B.R. Matthews, Y. Chen, X. Zhou, M.I. Gomis, E. Lonnoy, T. Maycock, M. Tignor, and T. Waterfield (eds.) Global Warming of 1.5°C. An IPCC Special Report on the impacts of global warming of 1.5°C above pre-industrial levels and related global greenhouse gas emission pathways, in the context of strengthening the global response to the threat of climate change, sustainable development, and efforts to eradicate poverty. In Press https://www.ipcc.ch/sr15/chapter/glossary/
IPCC. (2022). Climate Change 2022 Impacts, Adaptation and Vulnerability: Summary for Policymakers. Working Group II contribution to the Sixth Assessment Report of the Intergovernmental Panel on Climate Change. [H.-O. Pörtner, D.C. Roberts, M. Tignor, E.S. Poloczanska, K. Mintenbeck, A. Alegría, M. Craig, S. Langsdorf, S. Löschke, V. Möller, A. Okem, B. Rama (eds.)]. Cambridge University Press. https://www.ipcc.ch/report/ar6/wg2/downloads/report/IPCC_AR6_WGII_FinalDraft_FullReport.pdf
Maran, D. A. & Begotti, T. (2021). Media exposure to climate change, anxiety and efficacy beliefs in a sample of Italian university students. International Journal of Environmental Research and Public Health, 18, 1-11. https://doi.org/10.3390/ijerph1879358
Ojala, M. (2015). Hope in the face of climate change: associations with environmental engagement and student perceptions of teachers’ emotion communication style and future orientation. The Journal of Environmental Education, 46(3), 133-148. https://doi.org/10.1080/00958964.2015.1021662
Reyes, M. E. S., Carmen, B. P. B., Luminarias, M. E. P., Mangulabnan, S. A. N. B., Ogunbode, C. A. (2021). An investigation into the relationship between climate anxiety and mental health among Gen Z Filipinos. Current Psychology. 1-9. https://doi.org/10.1007/s12144-021-02099-3
Thunberg, G. (2019, January 25). 'Our house is on fire': Greta Thunberg, 16, urges leaders to act on climate. The Guardian. https://www.theguardian.com/environment /2019/jan/25/our-house-is-on-fire-greta-thunberg16-urges-leaders-to-act-on-climate
Weintrobe, S. (2012). The difficult problem of anxiety in thinking about climate change. In S. Weintrobe (Ed.). Engaging with Climate Change: Psychoanalytic and Interdisciplinary Perspectives (pp 33-47). Routledge.
Dear all,
I hope you are doing well.
I am currently working with WRF-Chem, and I have a locally developed emission inventory specifically prepared for my study area. The dataset is in NetCDF format, but it does not conform to the standard structure required by WRF-Chem emission pre-processing tools (such as the anthro_emis utility).
I would like to ask for your guidance on the following:
- How can I properly reformat or convert my local NetCDF emission inventory so that it can be ingested by the anthro_emis utility or any other available tool for WRF-Chem?
- Are there any recommended workflows, scripts, or guidelines for adapting a custom emission inventory (especially one that is not initially designed for WRF-Chem) to the required format?
- What are the key structural aspects (variables, dimensions, units) that my NetCDF file must have to be correctly processed?
Any advice, references, or examples would be greatly appreciated.
Thank you very much in advance for your support.
Best regards,
When I measure the fluorescent emission intensity, there appears two peaks very close and with similar peak hight. I checked with different solvents, but it still the same. Is it ok to continue like this?
Dear All,
What actually causes the dioxin and furan concentration from MSW incineration to raise?
I thought with proper combustion (aiming for perfect combustion) whilst maintaining combustion chamber temperature high enough (approximately 1100 degree Celcius and its stack temperature around 800 degree Celcius, also sufficient retention time could minimize its formation. Am I missing something ?
Really appreciate any feedback from you.
Regards
I am synthesizing blue-emitting perovskite nanoparticles using 1-octadecene as a solvent, oleic acid, and oleylamine as a ligand. After synthesis, I centrifuge the nanoparticles at 12000 RPM and then disperse them in 15 mL of hexane followed by sonication. However, to remove excess organic solvents and ligands, I attempted washing with ethyl acetate, which is commonly used for perovskite purification. Unfortunately, this process shifts the emission from blue to green, indicating a possible phase transformation or change in surface chemistry.
Since I need to retain the blue emission for LED applications, I am looking for an alternative method to efficiently remove excess organic solvents and ligands without affecting the optical properties of the perovskite nanoparticles.
Has anyone successfully purified blue-emitting perovskite nanoparticles while maintaining their emission stability? Any suggestions on alternative solvents or purification techniques would be highly appreciated.
Thank you!
I am working with PS-DVB microsphere and have observed a luminescence in this wavelength range. Could this be related to impurities, structural defects, or specific effects associated with DVB crosslinking? I would appreciate any references or insights.
Link to the procedure of synthesized microsphere:
Choi, J., Kwak, S.-Y., Kang, S., Lee, S.-S., Park, M., Lim, S., ...Hong, S. I. (2002). Synthesis of highly crosslinked monodisperse polymer particles: Effect of reaction parameters on the size and size distribution. J. Polym. Sci., Part A: Polym. Chem., 40(23), 4368–4377. doi: 10.1002/pola.10514
I came across an article about an instrument that emits electrons at ambient pressure through corona discharge. The number of emitted electrons is amplified using a special material and light. This technique is called Photon Mediated Electron Emission (PMEE).
Does anyone know anything about PMEE?
Are you familiar with the patents mentioned in the article?
This is the work of an Indian researcher (Dr. Rajah Vijay Kumar), but I can't find anything on the subject.
Thanks a lot!
I am doing a test on LED coating for phosphors powder.
I am using an old 310 nm LED which is oxidized, it produces an emission peak at ~430nm and the emission spectrum of my phosphors is in the range of 400-600 nm, there is a spectral overlap between the oxidized part of the LED and my phosphors spectrum.
How can i calculate the quantum efficiency of the phosphors in this experiment? If possible, please give me the formula and explanation
The South African(SA) government is planning to shift the countries energy systems away from coal and towards renewable energy sources. The government has come up with a program called Just Energy Transition(JET-P) that aims to mitigate climate change impact, reduce carbon emissions towards a net-zero level, job creation, develop local skills, access to affordable energy, promote sustainable economic growth and development and to ensure fairness, equity and social justice.
The big economies of the world like US,UK Germany, France and the EU have committed to supporting South Africa's decarbonization efforts through their agreement in the long-term Just Energy Transition Partnership. These countries have committed financing through grants, concession loans and investments and risk sharing instruments worth $8.5billion for the first phase. This partnership is expected to prevent up to 1.5 gallstones of emission over 20 years. The partnership is more concerned about acceleration of the transition of South Africa to a low emission climate resilient economy.What does this mean to SA, in terms of economic growth?
I am interested to understand how the shift will affect jobs and business around the coal mining areas and SA. I want to determine the number of skills and the type of the job opportunities that will be available during and after the transition. I want to determine how an low emission climate resilient economy grows. I want to use comparison as well of South Africa and other countries that have taken the similar shift from coal to renewable energy sources.
Dear forum users!
I have a question about the temperature in the Ideal gas equation when calculating the GHG flux, e.g. CO2 measured with LiCOR or Gas chromatography from the static chamber method.
I have found differences in the literature between them. So, my question is, what temperature should be used to calculate the flux?
Is it Air temperature, Inside chamber temperature, soil temperature, Laser temperature for LICOR/GC, or Laboratory ambient temperature for GC?
Thanks in advance.
Dear Friend,
It is well-known that when there is a single emission peak in the PL spectrum, the maximum emission wavelength corresponds to the wavelength of that peak. However, when multiple emission peaks are present, how should the maximum emission wavelength be defined? Should it correspond to the peak with the longest wavelength or the one with the highest emission intensity? Are there any references or literature that support this definition? Additionally, how should this be addressed in the context of absorption spectra?
I look forward to your insights on this matter.
Sincerely
Robin King

Hello,
I am trying to check the status of the optical system in an atomic absorption spectrometer by using it in emission mode.
The model i am working with is a XplorAA Dual (GBC Scientific) system. Currently, we do not have a hollow cathode lamp to test the equipment, but i was told that it could be used in emission mode to check the status of the burner and/or optics before acquiring a HC lamp. The problem is i can't seem to find the information regarding the configuration of the equipment for its use in emission mode. The manual provided doesn't seem to include this information, although i was able to find the configuration option for emission mode in the software.
We also have problems with the installation of the flame shield, it seems some parts are missing or there is something we are not seeing.
GBC Scientific doesn't have an official representative in my country (Argentina) anymore. I have tried to make contact with the technical service in Australia and other Latin american countries to no avail.
If someone familiar with this brand and/or model can help me solve these issues, it would be greatly appreciated.
Best regards,
Dr. Juan Manuel Ostera
Universidad Nacional de Moreno - República Argentina
Exploring the Role of Small Modular Reactors in Achieving Net Zero Emissions for Merchant Vessels by 2050
EDS: energy dispersive spectroscopy
XFS: X-ray Fluorescence spectroscopy
PIXE: proton induced X-ray emission
- I am working on phthalocyanine molecules and recorded photoluminescence absorption and emission in the range 345-700 nm. The compound is in both solid thin film as well as solution form I want to see the non radiative relaxation which proves the mono disperse and aggregated conditions

When Er-doped materials are pumped by 980nm laser, they can emit the light at 1550nm as well as green light due to the energy transfer between different energy level. When all the emission energy come from the pump light, the up-conversion green light should be suppressed in order to maximize the emission energy at 1550nm which is the important for optical amplification at telecommunication wavelength. The question is thus that, how to suppress the up-conversion emission in Er-doped materials and therefore most of the pump energy can be converted into 1550nm?
low R-value is probably related to the higher symmetrical site occupied by Eu3+ ions, supporting the highest emission intensity.
Hello. I am working on ROS production of two systems:
system A is cerium oxide and hydrogen peroxide, system B is cerium oxide nanoparticle, hydrogen peroxide and potassium bromide. I did some antibacterial tests before and the bacteria(e.coli) cultivate in LB broth later mixed with these two systems were killed up to 100%. The results were obtained by plate couting and the plate with system B can kill all E.coli every time, while system A can kill most of them, so I want to go further and investigate the ROS production: singlet oxygen and hydroxyl radical.
singlet oxygen: excitation 488nm, emission 528nm;
hydroxyl radical: excitation 476nm, emission 516nm.
I used a clear-bottom black 96 well plate and add 100ul probe in each well to mix with the systems as below, then incubate them under room temperature for 30 min in dark before using the microplate reader:
system A(CeO2+H2O2)+E.coli
system B(CeO2+H2O2+KBr)+E.coli
system A(CeO2+H2O2)
system B(CeO2+H2O2+KBr)
The result was strange, fluorescence of system A+E.coli sometimes even bigger than system B+E.coli, and the result of system A or B without E.coli addtion were negative values, or bigger than with E.coli addition.
I think there must be some contamination in the process, and I am not familar with all the setting of the microplate reader.
Please help me........
Meadows, D. (1997). Places to Intervene in a System. Whole Earth, 91(1), 78-84.
On P7, it reads:
"In 1986 the US government required that every factory releasing hazardous air pollutants report those emissions publicly. Suddenly everyone could find out precisely what was coming out of the smokestacks in town. There was no law against those emissions, no fines, no determination of "safe" levels, just information. But by 1990 emissions dropped 40 percent. One chemical company that found itself on the Top Ten Polluters list reduced its emissions by 90 percent, just to "get off that list."
This is an exciting story, and I am thinking of using this example to illustrate the effectiveness of information policy instruments in my Environmental Policy course teaching. However, I am wondering, the Clean Air Act was enacted in 1970, and by 1986, there was still no law against emission? No fines? No determination of safe level in the US?
Who can provide a quick answer so that I do not have to dive into the legal documents?
Hi,
I have a question about emission factors for passenger cars based on the EMEP/EEA air pollutant emission inventory guidebook 2023, in the link that I used to calculate the CO2 emission per vehicle per household for a dataset of 2016- 2017: https://efdb.apps.eea.europa.eu/?source=%7B%22query%22%3A%7B%22bool%22%3A%7B%22must%22%3A%5B%7B%22term%22%3A%7B%22code%22%3A%221.A.3.b.i%20Road%20transport%2C%20passenger%20cars%22%7D%7D%2C%7B%22term%22%3A%7B%22Fuel%22%3A%22Petrol%22%7D%7D%2C%7B%22term%22%3A%7B%22Pollutant%22%3A%22CO2%22%7D%7D%2C%7B%22term%22%3A%7B%22Type%22%3A%22Tier%202%20Emission%20Factor%22%7D%7D%5D%7D%7D%2C%22display_type%22%3A%22tabular%22%7D
the emission factors are like 0.398 g/km much smaller than the 118.1 gram/km in 2016 based on the: https://www.eea.europa.eu/en/analysis/indicators/co2-performance-of-new-passenger
so, my average CO2 emission from private cars in the dataset is much lower than expected, suppose that the emission factor of 118.1 g/km, and an average km driven of around 13000km the CO2 is is 1,535,300 g/km and my average is about 173 g/km so this is a factor 10 different
could you please explain these two different emission factors? i mean the 0.398 g/km and the 118.1 g/km?
Do we have to use kg N or kg organic fertilizer multiply by emission factor of organic fertilizer production?
Could anyone suggest me what is effect of electron donating and withdrawing group on fluorecence emission or intersystem crosssing.
Thank you
I am studying the interaction between carbon dots and fluorescent organic dyes like Rhodamine 6G, which have an overlap between the emission of the CDs and absorption of the dyes.
In spectroscopic analysis, as I increase the concentration of the dyes in the CDs solution, the emission peak quenches, while the fluorescence lifetime increases as the concentration of the dye increases. Additionally, the emission intensities of the dyes increase. In a typical FRET (Förster Resonance Energy Transfer) process, the emission of the carbon dots is expected to decrease, and the emission of the dye is expected to increase. This is happening with my samples, but the fluorescence lifetime of the CDs is expected to decrease. However, in my CDs sample, the lifetime increases as I increase the amount of the quenching dyes.
Can you please share suggestions to understand this anomalous observation?.
Hello Everyone,
I have done UV-Vis absorbance and PL emission of 3 samples. When plotted, there is a clear correlation between UV-Vis absorption and PL emission spectrums, where the sample with the highest absorbance possesses the lowest excitonic emission. Is there any reason behind it, or is it just a coincidence? Or should I repeat the measurements?
I appreciate your time. Thanks.
Thermal emission is temperature dependent. Non-thermal emission is not temperature dependent such as synchrotron emission.
In order to proceed with the quantification of an Azide Alkyne Cycloaddition reaction efficiency by using a fluorogenic probe with Cy5-DBCO, I first need to construct a calibration curve. The problem is that water gives me fluorescence intensity values as well at an excitation wavelength of 647 nm and emission of 668 nm (excitation and emission that correspond to Cy5). I observe this using just water as a background control and it shows really high values. I am using a TECAN infinite 200 instrument and the samples are prepared in a black polystyrene 96-well plate.
I performed calculation using Gaussian to obtain the fluorescence emission of some organic molecules. The following lines are the data of the optimized singlet state geometry. why does the first excited state has lower wavelength emission than the second excited state ?
Excited State 1: Singlet-A 1.9113 eV 648.69 nm f=0.0008 <S**2>=0.000
85 -> 89 -0.69679
This state for optimization and/or second-order correction.
Total Energy, E(TD-HF/TD-KS) = -1179.74328545
Copying the excited state density for this state as the 1-particle RhoCI density.
Excited State 2: Singlet-A 1.3773 eV 900.19 nm f=0.4216 <S**2>=0.000
88 -> 89 0.70630
Dear Researchers,
I have 100+ existing inland ships' hull lines plans along with their operational data like service speed, capacity, fuel consumption, main engine power, MCR at service condition, etc. I would like to start a research work focusing the reduction of fuel consumption and emission. Any other innovative research idea is also most welcome.
If anyone one shows interest for joint research, please send msg.
Thanks and best regards
Dr S M Rashidul Hasan
Earth’s Carbon cycle and Temperature
Slow Carbon Cycle:
Carbon takes around 100 – 200 million years to move through
rocks, soil, ocean and atmosphere.
10 - 100 million metric tons of carbon move through
Slow Carbon cycle per annum.
10,000 – 1,00,000 million metric tons of carbon move through
Fast Carbon cycle per annum.
Earth naturally absorbs (by oceans and forests) and
emits (undersea volcanos and hydrothermal vents)
around 100 billion metric tons of carbon per annum
(roughly equivalent to 400 billion tons of CO2).
CO2 Emissions from fossil fuels in 2023: Roughly 40 billion metric tons.
Ratio: CO2 Emissions from fossil fuels amounts to just 10% of natural CO2 emission and absorption by earth.
Moral
Overall carbon cycle, over a very long term,
is expected to maintain a balance,
which keeps earth’s temperature
to remain to be relatively stable.
However, over a relatively shorter time period,
earth fluctuates between ice ages and warmer interglacial periods,
where, parts of carbon cycle may even intensify
the short-term temperature changes
(which, we keep experiencing now),
and thereby significantly affecting
the stability of earth’s temperature.
Nature will take care
the balance of
carbon-cycle
as well as
temperature
on its own,
but very slowly.
Leaving aside
altering earth's climate,
Have we understood
the nature
(including the 'coupled' effect of
Milankovitch theory: eccentricity/obliquity/precession;
cirrus clouds effect;
albedo effect;
urban island effect;
El Nino effect)
in a single (human) life span?
Even, if it is so,
whether,
all the fundamental laws
remain valid
for such a complex system?
Even, if smarter one
manages to convince
that the earth's climate system
be modelled precisely,
how will the model results
be validated (in the absence of any future data)??
If not, how do we forecast?
[Only recent temperature data remains to be
satellite based,
while we used thermometers
(which just measures the degrees of hotness)
earlier.
Before 1624??]
Do we have
a well-defined
'Conceptual Model'
and its respective
'Mathematical Model'
(assuming that
we have a super computer
for numerical model)
that forecasts
how exactly climate change
will affect
extreme precipitation events
and sea levels?
Which conceptualization
has led to the prediction that
CO2 emissions from fossil fuels,
particularly from oil & gas industries
have led to the rise
in mean global temperature?
Is there any specific
spatial and temporal scales
over which
these climate models work?
With 428 ppm as on date,
feasible to distinguish
the CO2 emissions
from various sources?
Suresh Kumar Govindarajan
in the synchronous fluorescence measurements, the difference between excitation and emission wavelengths (Δλ) was fixed at 60 nm or 50 nm for Trp or 20 nm/ 15 nm for Tyr residues?
please answer which is the right Δλ for both Trp and Tyr? and Why?
Hello for everyone, I come to you to help me find a solution to my problem in the GC MSD.I reinstalled the external filaments but it does not work normally and an error message is displayed “The filament shows emission current while the filament is off” could you guide me to find a solution to this problem please.
We have grown boron nitride with a monolayer thickness. XRD usually is used to understand the polymorphism of any material. However, due to the minimum thickness of the sample, it won't work for our investigation.
PL is another choice, and a few papers have also demonstrated near-band edge emission to explain polymorphism. However, our research is focused on sub-bandgap emissions.
Which experimental tool can help us to understand the polymorphism of BN?
Hi all,
I'm working on calculations related to electron-phonon interactions during thermionic emission in a 2D material, using ab initio methods. I've come across the electron-phonon coupling constant, a dimensionless parameter commonly used in deriving the superconducting transition temperature. I'm curious about how this parameter can be related to thermal electron emission.
I can calculate the Density of States for my material and I have the Fermi-Dirac distribution at the emission temperature. I'm considering that incorporating the electron-phonon coupling constant might allow me to calculate a term for the emission probability, which could then yield the thermionic emission rate but I don't know the term. Could anyone assist me with this approach? Your help would be greatly appreciated
I have a fluorophore and its emission is quenched on adding analyte compound. The overlapping spectra of compound and analyte make UV-vis absorption analysis unreliable.
The analyte mixture spectra shows larger absorbance value than fluorophore compound.
Although I depend on emission spectroscopy for the quenching constants and etc.
I'm curious to know if there are any possible computing methods to overcome this problem and making the absorption spectrums useful for my purpose (explaining emission quenching)?
THE FATE OF “SOURCE-INDEPENDENCE” IN ELECTROMAGNETISM, GRAVITATION, AND MONOPOLES
Raphael Neelamkavil, Ph.D., Dr. phil.
With the introductory claim that I make here suggestions that seem rationally acceptable in physics and the philosophy of physics, I attempt here to connect reasons beyond the concepts of magnetic monopoles, electromagnetic propagation, and gravitation.
A magnetic or other monopole is conceptually built to be such only insofar as the basic consideration with respect to it is that of the high speed and the direction of movement of propagation of the so-called monopole. Let me attempt to substantiate this claim accommodating also the theories in which the so-called magnetic monopole’s velocity could be sub-luminal.
If its velocity is sub-luminal, its source-dependence may be demonstrated, without difficulty, directly from the fact that the velocity of the gross source affects the velocity of the sub-luminal material propagations from it. This is clear from the fact that some causal change in the gross source is what has initiated the emission of the sub-luminal matter propagation, and hence the emission is affected by the velocity of the source’s part which has initiated the emission.
But the same is the case also with energy emissions and the subsequent propagation of luminal-velocity wavicles, because (1) some change in exactly one physical sub-state of the gross source (i.e., exactly the sub-state part of the gross source in which the emission takes place) has initiated the emission of the energy wavicle, (2) the change within the sub-state part in the gross source must surely have been affected also by the velocity of the gross source and the specific velocity of the sub-state part, and (3) there will surely be involved in the sub-state part at least some external agitations, however minute, which are not taken into consideration, not possible to consider, and are pragmatically not necessary to be taken into consideration.
Some might claim (1) that even electromagnetic and gravitational propagations are just mathematical waves without corporeality (because they are mathematically considered as absolute, infinitesimally thin waves and/or infinitesimal particles) or (2) that they are mere existent monopole objects conducted in luminal velocity but without an opposite pole and with nothing specifically existent between the two poles. How can an object have only a single part, which they term mathematically as the only pole?
The mathematical necessity to name it a monopole shows that the level of velocity of the wavicle is such that (1) its conventionally accepted criterial nature to measure all other motions makes it only conceptually insuperable and hence comparable in theoretical effects to the infinity-/zero-limit of the amount of matter, energy, etc. in the universe, and that (2) this should help terming the wavicle (a) as infinitesimally elongated or concentrated and hence as a physically non-existent wave-shaped or particle-shaped carrier of energy or (b) as an existent monopole with nothing except the one mathematically described pole in existence.
If a wavicle or a monopole is existent, it should have parts in all the three spatial directions, however great and seemingly insuperable its velocity may be when mathematically tested in terms of its own velocity as initiated by STR and GTR and later accepted by all physical sciences. If anyone prefers to call the above arguments as a nonsensical commonsense, I should accept it with a smile. In any case, I would continue to insist that physicists want to describe only existent objects / processes, and not non-existent stuff.
The part A at the initial moment of issue of the wavicle represents the phase of emission of the energy wavicle, and it surely has an effect on the source, because at least a quantum of energy is lost from the source and hence, as a result of the emission of the quantum, (1) certain changes have taken place in the source and (2) certain changes have taken place also in the emitted quantum. This fact is also the foundation of the Uncertainty Principle of Heisenberg. How then can the energy propagation be source-independent?
Source-independence with respect to the sub-luminal level of velocity of the source is defined with respect to the speed of energy propagation merely in a conventional manner. And then how can we demand that, since our definition of sub-luminal motions is with respect to our observation with respect to the luminal speed, all material objects should move sub-luminally?
This is the conventionally chosen effect that allegedly frees the wavicle from the effect of the velocity of the source. If physics must not respect this convention as a necessary postulate in STR and GTR and hence also in QM, energy emission must necessarily be source-dependent, because at least a quantum of energy is lost from the source and hence (1) certain changes have taken place in the source, and (2) certain changes have taken place also in the emitted quantum.
(I invite critical evaluations from earnest scientists and thinkers.)
I am using a fluorescence microscope with DAPI filter, here are the specifications:
Excitation wavelength: 360/40 nm
Emission wavelength: 460/50 nm
Dichroic mirror wavelength: 400 nm
I want to label my cells with cyan fluorescent protein. I just want to know if our DAPI filter can detect the CFP. Thanks.
Through my preliminary experiments, it was found that there is an emission of abnormal ultra-high energy electrons downstream of the RF cavity of the electron storage ring, which I theoretically predicted. Therefore, I call on particle physicists to conduct more experiments to fully verify this previously unknown phenomenon with important significance.
What is the Relationship Between Vacuum and Space?
The historical evolution of the concept of "vacuum" [1] can be roughly described as the following.
0) Buddhist Vacuum: the void formlessness, the empty barrier-free. It refers to the place and space where all dharmas exist. There are four meanings: pervasive, immovable, endless, and eternal.
I) Conceptual Vacuum: Aristotle in ancient Greek era believed that " Void separated from the matter does not exist" [2], the void must be filled with matter in order to be able to carry out physical action*. The concept of vacuum at this stage is void, a state of space.
II) Industrial vacuum: Evangelista Torricelli (1608-1647), secretary and assistant of Galileo Galilei (1564-1642), proved the "vacuum" without an atmosphere using a mercury barometer [3]. The concept of vacuum at this stage was static and overlapped with Newton's absolute space.
III) Ether Vacuum: “......, as the recipient of energy, is to regard it as continuously filling all space, and possessing the mobility of fluid rather than the rigidity of a solid. If whatever possess the property of inertia be matter, then the medium is a form of matter. But away from ordinary matter it is, for obvious reasons, best to call it as usual by a separate name, the ether."[4] "The aether is the solitary tenant of the universe, save for that infinitesimal fraction of space which is occupied by ordinary matter."[5]. The vacuum at this stage is the medium through which electromagnetic waves can travel.
IV) Quantum Vacuum: Along with the development of quantum mechanics, numerous vacuum-related concepts have arisen, the ground state, the various excited states, zero point energy, negative energy sea, spontaneous emission, Vacuum polarization, vacuum fluctuations, etc.. "The vacuum is, in fact, precisely the ground state of the fundamental many-field system. "[9]† "In a quantum theory, the vacuum is a very busy place. Particle-antiparticle pairs are constantly produced out of nothing, violating the energy-conservation law by borrowing an amount of energy E from the vacuum for a time t such that Et<ℏ, according to Heisenberg's uncertainty principle. "As the Higgs boson propagates in the quantum vacuum, it feels the presence of virtual particles and interacts with them."[6] and theoretically and experimentally identified the Casimir effect for verifying vacuum energy[7][8], and the Lamb shift. The concept of vacuum at this stage provides a self-consistent ground for quantum field theory, where the vacuum is seen as a separate background for spacetime.
V) Relativity Vacuum: Quantum field theory predicts that a uniformly accelerated particle detector sees the vacuum as a thermal bath with temperature T related to its proper acceleration a, i.e., T =a/2π, as a result of the interaction between the detector and the fluctuating vacuum scalar fields, and this is called the Fulling-Davies-Unruh (FDU) effect. Vacuum and space appear to be separate.
VI) Planck Scales Vacuum: Some of the new physics considers the vacuum to be more complex, with the emergence of Quantum foams [11], Spin foams, Quantum spacetime [12], String Network, Lattice structure, Conformal structure [13], and other concepts [14]. Space is discretized and the Vacuum seems to merge with Space again.
VII) Dark Energy Vacuum: It is believed by some people that the vacuum energy is dark energy, and therefore the vacuum is a place with a certain dark energy density. In this case, the vacuum has the effect of the cosmological constant Λ [15], which is the driving force for the accelerated expansion of space-time.
It appears that the relationship between the various vacuums and space is not consistent. Without a clear definition on this most fundamental issue of physics, it may already be a potential obstacle to progress.
Our questions are:
1) Is the size of the vacuum the same as the size of cosmic space? When cosmic space inflation or expands, is the cosmic vacuum also inflating or expanding?
2) If the vacuum is not empty, is it uniform? Is it affected by the General Relativity Space-Time Metric (Curvature)? Is the vacuum inside a black hole the same as the vacuum elsewhere?
3) In a particle accelerator, does an electron traveling at high speed see the same vacuum as a stationary electron? Do electrons interact with the vacuum only at the moment of collision?
4) Without vacuum energy, is there no possibility of producing any particles in space? How were the initial elementary particles excited‡?
5) Would our conception of the vacuum change if we gave up the dynamical function of the uncertainty principle?
--------------------
Notes
* Aristotle gives an example, if a ball is thrown up, and it continues to fly after it has been released from the hand, it means that something must be holding it up one after the other, otherwise it would have fallen down. Note that this plain view is not necessarily wrong. Without borrowing the notion of conservation of energy-momentum, our explanation must return to the plain description. In fact, the intuitive interpretation of conservation of energy-momentum itself still requires this plain view.
‡ "What relation subsists between the medium which fills the interstellar void and the condensations of matter that are scattered throughout it?"[5] The relation between vacuum energy and visible energy was questioned 100 years ago.
† In the literature [9] the vacuum is specified, the Higgs vacuum, electromagnetic field vacuum, Dirac electron vacuum, the boson vacuum, the QCD vacuum......
--------------------
References
[1] 张天蓉. (2022). 真空. https://blog.sciencenet.cn/blog-677221-1342155.html
[2] Aristotle. (1929). The Metaphysics [物理学] (张竹明, Trans.).
[4] Heaviside, O. (1892). On the forces, stresses, and fluxes of energy in the electromagnetic field. Philosophical Transactions of the Royal Society of London.(A.)(183), 423-480.
[5] Whittaker, E. (1910). A History of the Theories of Aether and Electricity (Vol. Vol. I: The Classical Theories; Vol. II: The Modern Theories, 1900-1926). Courier Dover Publications(1989)极好的早期物理学历史著作。
[6] Kane, G., & Pierce, A. (2008). Perspectives on LHC physics. World Scientific Publishing Co. Pte. Ltd.
[7] Casimir, H. B. (1948). On the attraction between two perfectly conducting plates. Proc. Kon. Ned. Akad. Wet.,
[8] Jaffe, R. L. (2005). Casimir effect and the quantum vacuum. Physical Review D, 72(2), 021301. https://doi.org/10.1103/PhysRevD.72.021301
[9] Aitchison, I. J. R. (1985). Nothing's plenty the vacuum in modern quantum field theory. Contemporary Physics, 26(4), 333-391. https://doi.org/10.1080/00107518508219107
[10] Zhou, W., & Yu, H. (2020). Collective transitions of two entangled atoms and the Fulling-Davies-Unruh effect. Physical Review D, 101(8), 085009.
[11] Misner, C. W., Thorne, K. S., & Zurek, W. H. (2009). John Wheeler, relativity, and quantum information. Physics Today, 62(4), 40-46.
[12] Ashtekar, A., & Singh, P. (2011). Loop quantum cosmology: a status report. Classical and quantum gravity, 28(21), 213001.
Rovelli, C. (2008). Loop Quantum Gravity. Living Reviews in Relativity, 11(1), 5. https://doi.org/10.12942/lrr-2008-5
[13] Penrose, R. (2012). The basic ideas of conformal cyclic cosmology. AIP Conference Proceedings 11,
[14] Addazi, A., Alvarez-Muniz, J., & etl. (2022). Quantum gravity phenomenology at the dawn of the multi-messenger era—A review. Progress in Particle and Nuclear Physics, 125, 103948. https://doi.org/https://doi.org/10.1016/j.ppnp.2022.103948
[15] Peebles, P. J. E., & Ratra, B. (2003). The cosmological constant and dark energy. Reviews of Modern Physics, 75(2), 559.
can anyone give me advise about charge transfer transition of transition metal and rare earth element?
and usually people see the FL and absorption, emission spectra of those materials in glass, and I just want to know how much energy need to ionization the transition metal and rare earth element.
Could you recommend some studying source about it?
As the article reported,
Reaction Yield= mpurified*w%/n*MPb
where mpurified is the mass of the dried quantum dots, w% is the mass
percentage of lead (28.74 %) [by inductively coupled plasma optical
emission spectroscopy (ICP-OES) elemental analysis], n is the number of
CsPbBr3 quantum dot moles, and MPb is 207.
n should be the moles of Pb precursor according to "The reaction yield is assessed in terms of Pb present in the DBSA-QDs compared to the Pb precursor."
Hi there. Can DAPI be excited with 440 nm wavelength? Maybe still a bit of tail is there from the absorption spectrum, yet we are much in the emission spectrum already. Making me think what we get is mainly just stimulated emission. Anyone has experience on a similar test?
I have emission and sink of CO2 from 2060 to 2015 and I use a box model for the troposphere or world to predict a future scenario in excel and SPSS. I also need to make different scenarios I guess on I assumptions, so would you please enlighten me about how to do that? Many thanks.
Looking for thoughts:
(i) How to verify Methodology of GHG Emission for Armed Conflict, considering no clear methodology identified by UNFCC, nor academia use consistent factors as baseline for calculation?
(ii) Why some studies consider emission for destruction of concrete building in addition to reconstruction, while other only consider rebuilding? Is it the significant amount of concrete and release of of CO2 due destruction?
Is there any open-access source where I can find the emission factors for the Scope 3 components of an educational institution?
The components include:
chemical,
glassware,
capital goods,
computer accessories,
electronics and electrical products,
commuting and business travels,
refrigerants,
consumed water
transport
wastes
Is there any weather data morphing tool (for hourly weather data) to predict climate change for future using the IPCC AR5 (assessment report 5) emission scenarios I.e. rcp 2.5, rcp 4.5, rcp 6 & rcp 8?
It should be noted that the synthesized particle has a blue emission
A company produces PP surgical products from granular raw materials by injection. molding technique. They did not find any weight loss after melting. According to the manufacturer policies, they should mention the amount of CO2 emission. How do they measure the amount of CO2 emission?
The History of Reserve Currencies
Lets begin with understanding money as liquid, which is how CHINESE describes MONEY as WATER.
MONEY as WATER & LIQUIDITY
The expression "money is like water" is often attributed to Chinese culture, and it reflects a particular mindset about wealth and its fluid nature. While not everyone in China may use this expression, it does capture a common attitude towards money. Here are some reasons why money is sometimes metaphorically equated with water in Chinese culture:
- Fluidity and Circulation: Water is fluid and can flow easily. Similarly, the idea is that money should not be stagnant but should circulate and flow smoothly through various channels of the economy. This concept emphasizes the importance of keeping money in motion to generate economic activity.
- Adaptability: Water can take the shape of its container and adapt to different forms. Money, too, is seen as something that should be adaptable and flexible. The ability to adapt to different financial situations is valued, and the metaphor highlights the importance of being nimble in financial matters.
- Renewal and Growth: Water is essential for the growth of plants and sustaining life. Money, in a similar sense, is considered crucial for economic growth and development. The metaphor emphasizes the idea that money, like water, is essential for sustaining and fostering prosperity.
- Symbol of Abundance: In Chinese culture, water is often associated with abundance and prosperity. The metaphor of money being like water might convey the idea that there is an abundance of financial opportunities and resources available, and one should tap into them wisely.
- Flowing Fortunes: The phrase could also imply that fortunes, like water, are ever-changing. What may be plentiful today might be scarce tomorrow, emphasizing the importance of being mindful of financial fluctuations and making sound financial decisions.
CO2 as LIQUIDITY
If we conceptualize CO2 as liquidity rather than a gas or vapor, we are essentially considering carbon dioxide as a form of tradable liquid asset that represents environmental impact. This approach adds an additional layer to the integration of CO2 into a financial system. Here's how this could be incorporated into the concept:
- CO2 Liquidity Units: Instead of carbon credits, introduce the concept of CO2 liquidity units. These units would represent a standardized measure of carbon emissions that can be bought, sold, or traded in the market.
- Liquid Carbon Market: Establish a liquid carbon market where entities, including businesses, governments, and individuals, can buy and sell CO2 liquidity units. This market would function similarly to financial markets where liquidity is traded.
- Carbon Liquidity Exchanges: Create specialized carbon liquidity exchanges where participants can engage in the buying and selling of CO2 liquidity units. These exchanges would operate alongside traditional financial exchanges.
- Liquidity Providers: Designate entities, such as environmental organizations or sustainable initiatives, as liquidity providers. These entities would contribute to the market by removing excess CO2 liquidity units from circulation through activities like carbon sequestration or environmental projects.
- Centralized Liquidity Authority: Establish a centralized authority responsible for regulating and overseeing the CO2 liquidity market. This authority would manage the overall liquidity supply, adjusting it based on environmental goals and targets.
- Carbon-backed Liquidity Reserves: Implement carbon-backed liquidity reserves to stabilize the value of CO2 liquidity units. These reserves would function similarly to central bank reserves in traditional financial systems.
- Carbon Liquidity-backed Financial Instruments: Develop financial instruments, such as bonds or loans, that are backed by CO2 liquidity units. This would provide a way for financial markets to support sustainable projects, similar to green bonds.
- Liquidity-based Incentives: Introduce incentives for entities to maintain or increase their liquidity levels. Those who reduce their carbon emissions and maintain a surplus of CO2 liquidity units could benefit financially, while those with deficits would face higher costs.
- Real-time Liquidity Monitoring: Implement advanced monitoring systems for real-time tracking of carbon liquidity levels. This transparency would enable better decision-making and responsiveness to changes in environmental conditions.
- Education and Adoption: Promote education and awareness about the CO2 liquidity system to ensure widespread understanding and adoption. Stakeholders, including businesses and individuals, need to grasp the concept of CO2 as a form of liquid asset.
This conceptualization aims to integrate the idea of liquidity into the carbon economy, treating CO2 as a tradable liquid asset with a value that can be influenced by market forces. It introduces the dynamics of supply, demand, and liquidity management into the broader context of environmental sustainability. As with any innovative financial system, careful planning, regulation, and adaptation are crucial for its successful implementation. Additionally, it's essential to consider potential unintended consequences and continually assess the system's effectiveness in achieving environmental goals.
MONEY & CURRENCIES PEGGED to CO2 as LIQUID SUPPLY & DEMAND
Here's a conceptual approach to a real-world system where money is pegged to CO2 supply and demand:
- Carbon Credits as Tradable Assets: Implement a system where carbon credits become tradable assets, similar to stocks or bonds in financial markets. These carbon credits would represent the right to emit a certain amount of CO2.
- Carbon Pricing Mechanism: Introduce a carbon pricing mechanism, such as a carbon tax or cap-and-trade system. This places a cost on carbon emissions, creating a direct economic incentive for businesses and individuals to reduce their carbon footprint.
- Centralized Carbon Authority: Establish a centralized carbon authority responsible for issuing and regulating carbon credits. This authority would control the overall supply of carbon credits in circulation, adjusting it based on environmental goals and targets.
- Currency Pegged to Carbon Credits: Create a new form of currency that is directly pegged to the supply of carbon credits. The value of this currency would be tied to the overall carbon emissions allowed within a specified period.
- Carbon Reserve System: Implement a carbon reserve system, similar to a central bank's reserve system, to manage fluctuations in carbon credit supply and demand. The reserve would be used to stabilize the value of the carbon-backed currency.
- Incentives for Carbon Reduction: Offer financial incentives for businesses and individuals to reduce their carbon emissions. Those who emit less than their allocated carbon credits could sell their excess credits, while those exceeding their limit would need to buy additional credits.
- International Carbon Exchange: Facilitate an international carbon exchange where countries can trade carbon credits, fostering global cooperation in addressing climate change. This exchange would allow nations to balance their emissions by buying and selling credits on the international market.
- Carbon-backed Financial Instruments: Develop financial instruments such as bonds or loans that are backed by carbon credits. This could encourage investments in sustainable projects and provide a way for financial markets to support environmentally friendly initiatives.
- Carbon Auditing and Verification: Implement rigorous carbon auditing and verification processes to ensure the accuracy and legitimacy of carbon credit transactions. This would prevent fraud and maintain the integrity of the carbon-backed currency.
- Transition Period and Education: Recognize that transitioning to a carbon-backed currency would require careful planning and education. Governments, businesses, and the public would need to understand the new system and its implications.
It's important to note that while this concept provides a real-world approach, it is highly complex and would face numerous challenges, including international cooperation, regulatory frameworks, and the need for a robust infrastructure to manage the carbon credit system.
The CARBON COIN/ DOLLAR
Pegging an international currency to a conception of CO2 reduction involves linking the value of the currency to the success and progress of global efforts in reducing carbon emissions. Here's a conceptual framework for how this might be achieved:
- Creation of a Carbon-Backed International Currency: Develop a new international currency, let's call it "CarbonCoin" for illustration purposes, directly pegged to the global reduction of carbon emissions. The value of CarbonCoin would be tied to the success in achieving predetermined global CO2 reduction targets.
- Global Carbon Reduction Targets: Establish ambitious and scientifically informed global carbon reduction targets. These targets would serve as the benchmark against which the value of CarbonCoin is pegged. The more successful the world is in meeting these targets, the stronger the value of CarbonCoin.
- Carbon Reduction Verification Mechanism: Implement a robust and transparent global mechanism for verifying carbon reduction efforts. This could involve international organizations, technological solutions, and agreements that ensure accurate reporting and accountability for CO2 reductions.
- CarbonCoin Reserve System: Create a global CarbonCoin reserve system that stores CarbonCoins in proportion to the cumulative global CO2 reductions achieved. This reserve would act as a backing for the international currency, similar to gold backing traditional currencies in the past.
- International CarbonCoin Authority: Establish an international authority responsible for managing the CarbonCoin system. This authority would oversee the pegging process, verify carbon reductions, and adjust the supply of CarbonCoins in circulation based on global progress toward emission reduction goals.
- CarbonCoin Exchange Mechanism: Develop a global exchange mechanism for CarbonCoins, where countries and entities can buy, sell, and trade CarbonCoins based on their individual and collective contributions to CO2 reduction. This exchange would influence the value of CarbonCoin in the international market.
- CarbonCoin as a Reserve Currency: Promote the use of CarbonCoin as a reserve currency alongside traditional fiat currencies like the U.S. dollar or the euro. Countries could hold CarbonCoins in their reserves as a way to demonstrate and support their commitment to environmental sustainability.
- Incentives for Carbon Reduction: Offer financial incentives for countries and entities that contribute significantly to global CO2 reductions. This could involve rewarding nations with additional CarbonCoins based on their achievements in emission reduction.
- CarbonCoin-Backed Bonds and Financial Instruments: Introduce financial instruments, such as bonds, loans, or investment products, that are backed by CarbonCoins. This would create a market for sustainable investments and encourage the allocation of funds to projects contributing to CO2 reduction.
- International Cooperation and Agreements: Encourage international cooperation through agreements and treaties that support the CarbonCoin system. Cooperation would be vital to the success of this currency peg, requiring commitments from nations to pursue and maintain effective carbon reduction policies.
Implementing such a system would require significant coordination, cooperation, and commitment from the international community. It would also involve addressing challenges such as varying levels of economic development, differing national priorities, and potential resistance to adopting a new international currency system. Additionally, technological advancements in monitoring and verification of carbon reduction efforts would play a crucial role in the success of this conceptual framework.
How Pegging CO2 as LIQUIDITIES to CURRENCY EXCHANGES can OVERCOME EXISTING INERTIA to CO2 REDUCTION
Pegging CO2 as liquidities to currency exchanges could potentially introduce innovative financial mechanisms to overcome hurdles in CO2 reduction efforts. Here are ways in which this approach might help address challenges:
Market-Driven Incentives:
How it Helps: By pegging CO2 as liquidities to currency exchanges, you create a market for trading carbon assets. This introduces market-driven incentives for businesses and nations to reduce emissions, as they can profit from selling excess carbon liquidities or face costs for exceeding their allocated limits.
Flexibility and Adaptability:
How it Helps: Liquid markets are often more flexible. This flexibility can be harnessed to adapt to varying circumstances, allowing entities to buy or sell carbon liquidities based on changing economic conditions or technological advancements. It provides a dynamic system that can adjust to evolving emission reduction challenges.
Global Collaboration through Trading:
How it Helps: A liquid carbon market could facilitate global collaboration. Countries with a surplus of carbon liquidities can trade with those facing challenges, promoting a more efficient allocation of resources for emissions reduction. This approach encourages a collaborative, international effort to achieve overall reduction targets.
Liquidity-Backed Investments:
How it Helps: The concept of CO2 liquidities as a tradable asset could attract investments in sustainable and low-carbon projects. Financial instruments backed by carbon liquidities, such as bonds or green funds, may become attractive to investors, funneling capital into initiatives that contribute to emission reduction.
Transparent Market Mechanism:
How it Helps: Liquid markets often operate with a high degree of transparency. This transparency could help overcome challenges related to verification and trust. It ensures that the buying and selling of carbon liquidities are conducted with integrity, minimizing the risk of fraudulent activities.
Carbon Liquidity Reserves:
How it Helps: Establishing reserves of carbon liquidities can act as a stabilizing mechanism. During economic downturns or unexpected challenges, entities can tap into these reserves to meet emission reduction targets without facing excessive financial burdens, promoting long-term stability in carbon markets.
Economic Growth with Emission Reduction:How it Helps: Liquid carbon markets could provide a mechanism for balancing economic growth with emission reduction. As economies grow, they may need additional carbon liquidities, which can be acquired through the market. This allows for economic development while ensuring adherence to overall carbon reduction goals.
Private Sector Participation:
How it Helps: Liquid carbon markets could attract greater participation from the private sector. Businesses can actively engage in emissions reduction efforts by buying and selling carbon liquidities, aligning their financial interests with environmental goals and contributing to a more sustainable economy.
Carbon-Backed Financial Instruments:
How it Helps: The creation of financial instruments backed by carbon liquidities, such as carbon futures or options, could provide businesses and investors with tools to manage and mitigate risks associated with emissions. This can enhance financial planning and encourage long-term sustainability.
Public Awareness and Engagement:
How it Helps: A liquid carbon market could be designed to include public participation, allowing individuals to buy and sell carbon liquidities. This engagement can increase public awareness and encourage environmentally conscious behavior, as individuals see a direct link between their actions and the carbon market.
While pegging CO2 as liquidities to currency exchanges introduces potential benefits, it's crucial to recognize that implementing such a system would still require careful design, international cooperation, and ongoing monitoring to ensure its effectiveness in promoting meaningful CO2 reduction. Additionally, considerations for potential market manipulation, regulatory frameworks, and social equity issues should be addressed in the development and implementation of this approach.
The POLITICAL ECONOMY of CARBONCOIN
A political economist would likely analyze the concept of pegging CO2 to currency exchanges from a multidimensional perspective, considering the economic, political, and social implications of such an approach. Here are some aspects a political economist might consider:
Economic Efficiency:
Analysis: A political economist would assess whether pegging CO2 to currency exchanges promotes economic efficiency by creating market-driven incentives for emissions reduction. They might evaluate the efficiency of the proposed carbon market in allocating resources and encouraging innovation in low-carbon technologies.
Distributional Effects:
Analysis: Political economists would scrutinize the distributional effects of the proposed system. They might investigate how the costs and benefits are distributed among different socioeconomic groups, regions, and nations. Consideration would be given to whether the approach exacerbates or mitigates existing inequalities.
International Cooperation:
Analysis: Political economists would study the feasibility of achieving international cooperation through a liquid carbon market. They might analyze the political dynamics and power structures among nations, assessing whether the proposed system provides sufficient incentives for countries to collaborate on emission reduction efforts.
Policy Instruments and Instruments Choice:
Analysis: Political economists would examine the choice of policy instruments within the proposed framework. They might consider the use of market-based mechanisms, regulatory approaches, and the role of government intervention. The analysis would explore how different policy instruments align with political and economic ideologies.
Political Will and Implementation Challenges:
Analysis: Political economists would assess the political will required to implement and sustain such a system. They might analyze potential political resistance, lobbying efforts, and the ability of governments to commit to long-term emission reduction targets, considering the political economy of climate change policies.
Environmental Justice:
Analysis: Political economists would scrutinize the environmental justice implications of the proposed approach. They might assess whether the system disproportionately affects vulnerable communities or if it addresses historical disparities in environmental burdens.
Role of Private Sector and Corporate Influence:
Analysis: Political economists would consider the role of the private sector within the proposed framework. They might analyze how corporations influence policy decisions, whether the approach aligns with corporate interests, and how the involvement of the private sector may impact the effectiveness of emission reduction efforts.
Policy Stability and Long-Term Commitments:
Analysis: Political economists would evaluate the stability of the proposed system over the long term. They might consider the potential for policy reversals with changes in government or economic conditions, assessing the resilience of the system to political volatility.
Global Governance and Institutions:
Analysis: Political economists would examine the global governance structures and institutions needed to support the proposed system. They might explore the role of international organizations, the effectiveness of existing institutions, and the need for new forms of global governance in managing a liquid carbon market.
Public Perception and Democratic Legitimacy:
Analysis: Political economists would consider how the public perceives the proposed approach and whether it aligns with democratic principles. They might assess the level of public engagement, participation, and the legitimacy of decision-making processes in shaping climate policies.
In essence, a political economist would analyze the proposed approach within the broader context of political and economic systems, considering its implications for power dynamics, social equity, and the overall political economy of climate change mitigation. This multidimensional analysis would provide insights into the feasibility, effectiveness, and potential challenges associated with pegging CO2 to currency exchanges.
Image Source: https://www.investopedia.com/terms/c/currency-peg.asp

I am considering planck's equation where Intensity of emission is a function of wavelength and temperature . If we have the intensity value for a particular wavelength (determined through emission spectroscopy) for solid propellant combustion case. Then in planck's equation for grey body emissivity and temperature will be the two unknowns.
As an end result I want to determine temperature in the solid propellant combustion flame by knowing intensity of the emission emitted at a particular wavelength. But since the hot particles which are emitting that intensity in the flame are like grey bodies emissivity has to be known to find out temperature of the hot particles (grey body).
Please help me in determining the emissivity so that temperature can be determined from intensity and wavelength data. Please refer equations given in section 3.2 (Continuous Spectra) of the attached reference paper.
The triplet energy stands as a crucial factor in adjusting the emission of TADF compounds. Discovering how to measure and calculate it using simple techniques is essential.
I understand that ED-XRF or WD-XRF only allows for high energy photon emission. I am wondering if it is possible to obtain emission in the visible region by attaching an external optical fiber to a spectrophotometer (Ocean Optics)? However, I am skeptical about this since the chambers used for XRF are typically sealed. Do you have any other suggestions?
I characterized my materials by PL spectroscopy. I observed some enhancement in my emission intensity. From this data can I calculate Quantum yield? If anybody know the calculation please give the notes.
Hello. I have vehicle specific power (VSP) values I calculated from different speeds and gradients (uphill and downhill), always considering zero acceleration. With these binned VSP values, I have the corresponding CO2 emissions in g/s that I got from the EPA's "Methodology for Developing Modal Emission Rates for EPA’s Multi-Scale Motor
Vehicle and Equipment Emission System", but I would rather have them in g/km.
I'm messing something up, because I have emissions for a downhill slope (<=-2,5%) at 10km/h of 537,66 g/km and for an uphill slope (>2,5%) and speed 120km/h of 214,95g/km.
This makes no sense to me.
What I did to convert the values was consider that, e.g., for an emission of 1,5g CO2/s, and for a speed of 10 km/h (or 2,78m/s), was:
1,5g/s : 2,78m/s = 0,54g/m. So, for a total distance of 1km: 0,54 * 1000 = 540 g/km.
Is this reasoning correct? I'm going absolutely mad with this! Would appreciate any help.
Thank you
Global warming potential is calculated from the sum of CO2-equivalents from N2O and CH4 emissions. Why is carbon dioxide emission NOT included in global warming potential?
GWP (kg CO2 equivalent ha ) = CH4 (kg CH4 ha-1 ) X 28 + N2O (kg N2O ha ) X 265.
CH4 emission is greater 28 times and N2O is 265 times greater than CO2 emission in greenhouse potential, nevertheless total CO2 emission is much greater than CH4 or N2O.
Greeting Researchers
What is the accepted level of CO and NOx gas emission to the atmosphere ????
To whom it may concern,
Does anyone could explain me what is the components of the alpha emission quantity unit : Cph/cm² ?
C is for Coulomn ? ph ? I don't really understand...
Thanks in advance,
Vincent
The study object is a flat diode.
In the Particle Tracking solver, in the emission model settings (Edit Particle Area Source – Tracking emission model – Emission Settings) for Space Charge Limited Emission, Thermionic Emission, there is a Kinetic Settings tab (Fig. 1).
1) If temperature is selected as the kinetic characteristic (for Uniform distribution - Kinetic type: Temperature, for Maxwell distribution - Temperature), then what value should be set, the cathode temperature?
2) Velocity is selected as the kinetic characteristic (for Uniform distribution - Kinetic type: Velocity). The dependence of the emission current on the velocity I(v) is obtained. The emission current decreased with increasing speed (Fig. 2).
Energy is chosen as the kinetic characteristic (for Uniform distribution - Kinetic type: Energy). The dependence of the emission current on the energy I(U) is obtained. The emission current increased with increasing energy (Fig. 3).
How to understand the opposite behavior of the dependencies under consideration if energy and velocity are directly related: U= mv^2/(2*e)?
3) In the Thermionic Emission model settings, the temperature appears in both General and Kinetic Settings (Fig. 4). The temperature value in both General and Kinetic Settings should be the same?
Carbon storage potential of the floral species exhibits significant spatial variation depending on the near-surface atmospheric CO2 level that regulates the leaf thickness.

Dear colleagues,
I am new in the OLED field and just make some research about the field. Therefore I have some questions I want to confirm. I want to investigate the absorption and emission of molecule A.
1) To get the vertical absorption energy, first optimize the molecule at the ground state energy using
# td(nstates=10) opt
From the ground state geometry, perform a single point for first singlet excited state as #td(singlet,root=1,nstates=10)
The difference in the energy is vertical absorption energy. Is it correct?
I wonder if it can produce similar result to optimize molecule at dft and then perform simple td-dft of the ground state since the process also provides energy transition to first excited state?
2) for phosphoresence emission from first triplet excited state, first perform opt geometry as #td(triplet,root=1,nstates=10) opt. From the opt geometry of triplet excited state, perform #td(nstates=10) at ground state. The difference of energy is phosphoresence energy? Is it correct?
The same can be calculated for flouresence.
Thank you very much,
Sincrely,

I want to know how to measure methane emissions in dairy animals at the field level along with what kind of data to be measured .......
both are about excitation , is there same?
Interferences in plasma spectral analysis can certainly occur and can pose challenges when conducting analytical tests. The accuracy and dependability of the results can be seriously impacted by interference in elemental analysis. Plasma spectral analysis, often performed using techniques like inductively coupled plasma-mass spectrometry (ICP-MS) or inductively coupled plasma optical emission spectrometry (ICP-OES), is highly sensitive and capable of detecting trace elements and ions. One of the common types of interference is the Spectral interference. This phenomenon takes place when the analyte's emission or absorption lines and the lines of other elements in the sample cross each other. As a result, the target analyte may not be quantified correctly.
References:
Rosen, V. (2023, July 16). Interferences in ICP-OES/MS: Linkedin. https://www.linkedin.com/pulse/41-note-interferences-icp-oesms-vasiliy-v-rosen-ph-d-?trk=pulse-article
Thermo Fisher Scientific. (2021, September 16). Interferences Explained, ICP-OES Part 1. https://www.spectroscopyonline.com/view/interferences-explained-icp-oes-part-1
Can you briefly calculate carbon dioxide or greenhouse gas emissions from heating loads?
Example: 10 kwh/㎡·a * CO2 emission coefficient (kg/kwh) = ⅹ(kg/kwh·a)
If the transition is instantaneous, the moment the photon appears must be superluminal.
In quantum mechanics, Bohr's semi-classical model, Heisenberg's matrix mechanics, and Schödinger's wave function are all able to support the assumption of energy levels of atoms and coincide with the spectra of atoms. It is the operating mode of most light sources, including lasers. This shows that the body of their theories is all correct. If they are merged into one theory describing the structure image, it must have the characteristics of all three at the same time. Bohr's ∨ Heisenberg's ∨ Schödinger's, will form the final atomic theory*.
The jump of an electron in an atom, whether absorbed or radiated, is in the form of a single photon, and taking the smallest energy unit. For the same energy difference ΔE, jumping chooses a single photon over multiple photons with lower frequency ν, suggesting that a single photon structure has a more reasonable match between atomic orbital structures**.
ΔE=hν ......(1)
ΔE=Em-En ......(2)
It is clear that without information about Em, En at the same time, generating a definite jump frequency ν is impossible. "Rutherford pointed out that Rutherford pointed out that if, as Bohr did, one postulates that the frequency of light ν, which an electron emits in a transition, depends on the difference between the initial energy level and the final energy level, it appears as if the electron must "know" the frequency of light ν. level and the final energy level, it appears as if the electron must "know" to what final energy level it is heading in order to emit light with the right frequency."[1].
Bohr's postulate of Eq. (1)(2) energy level difference is valid [2]. But it does not hold as axiomatic postulate. This is not just because all possible reasons have not been ruled out. For example, one of the most important reasons is that the relationship between the "wave structure" of the electron and the electromagnetic field has not been determined†. Only if this direct relationship is established can the transition process between them be described. It is also required that the wave function and the electromagnetic field are not independent things, and it is required that the wave function is a continuous field distribution, not a probability distribution [5]. More importantly, Eqs. (1)(2) do not fulfill the axiomatic condition of being axiomatic postulate, which is not capable of ignoring the null information‡.
Doing it as a comparison of questions is the same as when we ask how the photon controls its speed [3] and where the photon should reach next. They are both photon behaviors that must rest on a common ground.
Considering the electron transition as a source of light, it is equally consistent with the principle of Special Relativity, and the photons radiated must be at the speed of light c and independent of the speed of the electrons††. However, if the light-emitting process is not continuous, the phenomenon of superluminal speed occurs.
We decompose the light-emitting process into two stages. The first stage, from "nothing" to "something", is the transition stage; the second stage, from something to propagation, is the normal state. According to classical physics, if the light emission is instantaneous, i.e., it does not occupy time and space. Then we can infer that the photon from nothing to something is not a continuous process, but an infinite process, and the speed at which the photon is produced is infinity. We cannot believe that the speed of propagation of light is finite and the speed at which light is produced is infinite. There is no way to bridge from the infinite to the finite, and we believe that this also violates the principle of the constancy of the speed of light.
There is no other choice for the way to solve this problem. The first is to recognize that all light emitting is a transitional "process" that occupies the same time and space, and that this transitional process must also be at the speed of light, regardless of the speed of the source of light (and we consider all forms of light emitting to be sources of light). This is guaranteed by and only by the theory of relativity. SR will match the spacetime measure to the speed of light at any light source speed. Secondly, photons cannot occur in a probabilistic manner, since probability implies independence from spacetime and remains an infinity problem. Third, photons cannot be treated as point particles in this scenario. That is, the photon must be spatially scaled, otherwise the transition process cannot be established. Fourth, in order to establish a continuous process of light emission, the "source" of photons, whether it is an accelerated electron, or the "wave function" of the electron jump, or the positive and negative electron annihilation, are required to be able to, with the help of space and time, continuous transition to photons. This will force us to think about what the wave function is.
Thinking carefully about this question, maybe we can get a sense of the nature of everything, of the extensive and indispensable role of time and space.
Our questions are:
1) Regardless of the solution belonging to which theory, where did the electron get the information about the jump target? Does this mean that the wave function of the electron should span all "orbitals" of the atom at the same time.
2) If the jump is a non-time-consuming process, should it be considered a superluminal phenomenon¶ [4]?
3) If the jump is a non-time consuming process, does it conflict with the Uncertainty Principle [5]?
4) What relationship should the wave function have to the photon to ensure that it produces the right photon?
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Notes:
* Even the theory of the atomic nucleus. After all, when the nucleus is considered as a "black box", it presents only electromagnetic and gravitational fields.
* * It also limits the possibility that the photon is a mixed-wavelength structure. "Bohr noticed that a wave packet of limited extension in space and time can only be built up by the superposition of a number of elementary waves with a large range of wave numbers and frequencies [2].
† For example, there is a direct relationship between the "electron cloud" expressed by the wave function of the hydrogen steady state, and the radiating photons. With this direct relationship, it is possible to determine the frequency information between the transition energy levels.
‡ If a theory considers information as the most fundamental constituent, then it has to be able to answer the questions involved here.
†† Why and how to achieve independence from the speed of light cannot be divorced from SR by its very nature, but additional definitions are needed. See separate topic.
¶ These questions would relate to the questions posed in [3][4][5].
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References:
[1] Faye, J. (2019). "Copenhagen Interpretation of Quantum Mechanics." The Stanford Encyclopedia of Philosophy from <https://plato.stanford.edu/archives/win2019/entries/qm-copenhagen/>.
[2] Bohr, N., H. A. Kramers and J. C. Slater (1924). "LXXVI. The quantum theory of radiation." The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 47(281): 785-802. This was an important paper known as "BSK"; the principle of conservation of energy-momentum was abandoned, and only conservation of energy-momentum in the statistical sense was recognized.
[3] “How does light know its speed?”;
[4] “Should all light-emitting processes be described by the same equations?”;
[5] “Does Born's statistical interpretation of the wave function conflict with ‘the Uncertainty Principle’?” https://www.researchgate.net/post/NO13_Does_Borns_statistical_interpretation_of_the_wave_function_conflict_with_the_Uncertainty_Principle;
When we measure the photoluminescence (PL) emission of some nanoparticles we find sometimes emission bands at energy higher than the optical bandgap. It is normal to observe photoluminescence at energies below the material bandgap as a result to the presence of localized defect states. However PL at energies higher than the optical bandgap it look strange!
Hello research community,
I got CFD simulation results of an internal combustion engine regarding emission in kg unit. For example: 14.5 gram of CO per cycle.
I need to convert this number to g/kW-hr to compare it with standards.
Anyone has any ideas?
In dumping operation of hot wet materials, for example, there is emission of particulate matter together with water vapor, which difficult the measurement of opacity. Is there any way to solve this problem, or other techniques to quantify the PM?
How does stokes shift of nitrogen-doped carbon quantum dots (blue emission) increases with quantum yield?
I am a master's student of environmental science and trying to calculate the GHG emissions from electricity generation industries using the tier 1 method of IPCC guideline and LEAP model. When I searched for some examples through websites and also some papers, I did not find them. So, I am confused about the calculation part, especially for IPCC. Please guide me or give me any suggestions on where I can get the references for that calculation.
I have difficulty when elaborating the positive impact/avoided emission from eliminating plastic/polybag use for tree planting activity. Is there any direct value/rule of thumb reference when eliminating XX kg of plastic?
How to improve the efficiency of the above title!
There exist some basic models for the angle dependence of sigma0. In R.E. Clapp, 1946, “A theoretical and experimental study of radar ground return” three such models are presented:
[1] sigma0(theta) = constant * cos(theta)2 called: “Lambert’s law”
[2] sigma0(theta) = constant
[3] sigma0(theta) = constant * cos(theta)
[3] is actually more complicated since it can also include multiple reflections from deeper layers of the surface. If however one only considers direct reflections the model takes the form as shown above.
In Ulaby, Moore, Fung, 1982, “Microwave Remote Sensing, Active and Passive” vol. II the authors also discuss these models of Clapp.
With models [1] and [3] one cosine(theta) term accounts for the decrease in incident power per unit surface area when the radar measures the ground return under angle theta. With [1] a seccond cosine(theta) term is added in accordance with Lambert’s law: a radiating surface whose angle-dependent emission is according to I = I0 * cos(theta) [Wm-2].
The well-known integral form of the radar equation applied to surface returns is (see for example Ulaby1982):
Prx = Ptx * [ lambda2 / (4 pi)3 ] * integral[ G2 / R4 * sigma0(theta) , dA ]
What I don’t understand is why there is not a cosine term in this equation by default? So
Prx = Ptx * [ lambda2 / (4 pi)3 ] * integral[ G2 / R4 * sigma0(theta) * cos(theta) , dA ]
Because the way I see it: regardless of the scattering properties of any surface the incident power per unit surface area must be rescaled according to cos(theta).
Hello all,
I am performing TDDFT emission spectrum calculation for the first time. I have used below mentioned route section command
%nprocshared=6
%mem=24GB.
# opt td=(singlets,nstates=10,root=1) b3lyp/gen pop=full geom=connectivity
pseudo=read
My molecule have C, H, N O for which I am using 6-31G** and Ge for which I am using LANL2DZ. The molecule comprised of 74 atoms in which one atom is Ge rest 36 are carbon and nitrogen, others hydrogen.
Can anyone please tell me am I going in a right direction or not.
Also, can anyone comment on the time it usually takes to complete the run.
Thanks in advance for the help.
Wondering, if the addition of DEE with biodiesel influences the HC, CO, NO and Smoke emissions. Its a great honor to get answer from expertise answer from the RG community. Kindly provide your valuable answers.
Does anyone know of a fluorescent protein with an emission max greater than 720 nm? Which is the best fluorescent protein with an emission max greater than 700 nm for making a BRET sensor? I have many luciferase mutants which could serve as donors in the 610-630 range provided I find a good acceptor FP in the far red range.
Dear Colleagues,
I want to make a demonstrative experiment on field emission of electrons from metal.
How much vacuum level is sufficient for field emission of electron without any corona discharge ?
Please discuss.
Thanks and Regards
N Das
India’s Green House Gas emissions calculation of livestock specifically enteric fermentation. These queries are related to -
• Methodology used to calculate emission from livestock in India
• What are the parameters used to calculate emissions from livestock – considering different - sub category of cattle and buffalo, breed, non-descript animals, feeding practices and rearing practices across India
• Emission factors – how are these arrived at for different cattle and buffalo breed including non-descript, what were the formula and sub formula used
• Details of various parameters used in the above formula and sub formula to arrive at the emission factor for each category
• Details of any model that is currently being used for emission factor estimation
• State wise enteric fermentation data for the last five years based on the emission factors currently used
• Activity Data – details of the activity data used to calculate the enteric fermentation
• How are we calculating emission for different rearing practices, stall fed, stall fed and grazing, grazing or pastoral and their details
• How are we calculating emission for the non-descript cattle and buffalo
• Are we factoring in the draught power in the emissions
• What are the factors contributing to the Uncertainty as per BUR3, what are the ongoing efforts to reduce these uncertainty
• Details of GHG inventory improvement practices adopted by the country
• Details of the effects of adaptation and mitigation actions related to productivity improvements in the livestock sector is adopted to estimate GHG emissions and its sustainability
is it possible to convert emission concentrations of air pollutants to ambient or atmospheric concentrations? and how many techniques are available for this issue?
Hello everyone.
I am currently deepening my knowledge related to the topic of emission reduction on a global scale. I am confused to find the default emission factor value for land cover/use class in the IPCC Guideline 2006 document, which incidentally is in units of tC/ha. Can anyone provide any clues in this regard?
Thank you.
Renewable source of energy is said to be an environmental friendly alternative source of energy specifically in addressing the emission of Green House Gases
Dear all
I want to set up the technique to assess the neuraminidase antiviral resistance in Influenza viruses, using the MUNANA assay.
I already have a TECAN fluorimeter fluorimeter Infinite 200 Pro. I need to get new filters for this technique.
TECAN offers several filters at the emission wavelength of 4-methylumbellyferone. Could you please tell me which of the available filters are you using?
Thanks
My TD-DFT calculation has been running for 2 days until now. It is converging very slowly. Can anyone check my input if it is correct? there are 102 atoms including Hg for this molecule
%NProcShared=4
%mem=12GB
%chk=1ehg5PCM_td.chk
# pbe1pbe opt td=(nstates=5,Root=1) Gen Pseudo=Read
Title Card Required
(geometry input-102 atoms)
C N H O 0
6-311+G**
****
Hg 0
LanL2DZ
****
Hg 0
LANL2DZ
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Another question, I check the output while it is running. It showed 5 excited states each time it is optimized. Why did the excited state go to 192 while the homo/lumo is 195/196 from Gaussview? it seems like the wavelength is too high at 6889.90 nm. How can I fix the problem?
Excitation energies and oscillator strengths:
Excited State 1: Singlet-A 0.1799 eV 6889.96 nm f=0.0256 <S**2>=0.000
190 -> 192 -0.17151
191 -> 192 1.41420
191 <- 192 -1.23925
This state for optimization and/or second-order correction.
Total Energy, E(TD-HF/TD-DFT) = -2302.89854925
Copying the excited state density for this state as the 1-particle RhoCI density.
Excited State 2: Singlet-A 0.6186 eV 2004.28 nm f=0.1212 <S**2>=0.000
190 -> 192 0.70827
191 -> 192 0.37654
190 <- 192 -0.18014
191 <- 192 -0.33394
Excited State 3: Singlet-A 0.7693 eV 1611.67 nm f=0.0040 <S**2>=0.000
188 -> 192 -0.15400
189 -> 192 -0.68720
191 -> 192 0.19474
191 <- 192 -0.18663
Excited State 4: Singlet-A 0.9019 eV 1374.75 nm f=0.0044 <S**2>=0.000
188 -> 192 0.68953
189 -> 192 -0.15006
Excited State 5: Singlet-A 1.4185 eV 874.08 nm f=0.0774 <S**2>=0.000
184 -> 192 -0.21919
186 -> 192 0.11819
187 -> 192 0.65092
Thank you so much for your help!
I have performed scanning mode of fluorescence measurement at different excitation wavelengths from 310 nm to 410 nm and collected the emission wavelength of each excitation wavelength from 350 nm to 600 nm. The picture below is the obtained fluorescent spectra. However, I am only able to obtain typical scanning-type emission spectra at excitation wavelengths from 310 nm to 340 nm. The rest of the excitation wavelength gives strange spectra (like something missing at the middle region). Can anybody explain this phenomenon? Is it normal or can we fix it if this is abnormal?

I am looking for some studies as regards reporting of greenhouse gas emissions of hospitals in the Philippines?
in fluorescence emission, the shoulder is formed. what is the cause of this phenomenon?
I have a cell that expresses a luciferase protein upon adding substrate. Our luciferase protein has an excitation wavelength of 488 nm and therefore it is supposed to be able to excite a yellow fluorescent protein. Plate reader (in luminescence mode) can be used to check if such a system works. Because of some limitations, I highly prefer other techniques, if it is possible. My question: can I use FACS (flow cytometry) to test the system? Using FACS machine, in our case FACSMelody, I can see if the cell expresses YFP protein by a combination of laser 488 nm (for excitation ) and filter 530 nm (for emission). Now, I want to use our luciferase protein instead of the laser 488 nm to excite YFP. if I use a FACS machine that has laser 488 nm, but (i) laser 488 nm is combined with filter 613 nm (not in the range of YFP emission wavelength), and (ii) laser 561 nm is combined with filter 530 nm,
can I say I am seeing the output of my system in 530 nm histogram graph, although YFP is excited by 488 nm laser (but its emission wavelength can not be detected because there is no detectable filter combined with laser 488 nm in the machine)?