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explain your idea
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Coaxial ground heat exchangers (CGHEs) have several advantages over traditional U-tube or spiral designs in ground-coupled heat pump systems. These advantages include:
1. Enhanced Heat Transfer Efficiency
  • Coaxial designs allow for better thermal contact with the surrounding soil due to a larger surface area per unit length.
  • The counter-flow arrangement of the fluid in the inner and outer pipes maximizes the temperature gradient between the working fluid and the surrounding ground, enhancing heat transfer efficiency.
2. Reduced Pressure Drop
  • The single continuous flow path in the coaxial configuration minimizes turbulence and flow resistance compared to U-tube designs. This reduces pumping power requirements.
3. Ease of Installation
  • Coaxial heat exchangers are typically pre-assembled and require less on-site work, making them quicker and easier to install.
  • The vertical configuration of coaxial systems often requires narrower boreholes, which can reduce drilling costs in some cases.
4. Improved Durability
  • The coaxial design reduces the risk of pipe connection failures since it has fewer joints and connections compared to U-tube systems.
  • Outer casings are often made from robust materials like high-density polyethylene (HDPE), providing excellent long-term durability and resistance to soil conditions.
5. Higher Thermal Performance in Deep Boreholes
  • Coaxial heat exchangers are particularly well-suited for deep boreholes because the outer pipe provides thermal insulation and ensures that heat exchange occurs efficiently along the entire depth of the borehole.
6. Flexibility in Design
  • CGHEs can accommodate different working fluids, including water, antifreeze mixtures, or other heat transfer fluids, allowing for adaptability to site-specific conditions and operational requirements.
7. Minimized Thermal Short-Circuiting
  • The coaxial arrangement minimizes the risk of thermal short-circuiting between the supply and return flows, which can be an issue in closely spaced U-tube systems.
8. Environmentally Friendly
  • Efficient heat transfer and lower energy consumption for pumping reduce the environmental impact of the system over its operational life.
9. Potential for Hybrid Applications
  • Coaxial systems can be integrated with other renewable energy systems (e.g., solar-assisted ground-source heat pumps) more effectively due to their efficient and compact design.
These advantages make coaxial ground heat exchangers an attractive choice for applications where efficiency, durability, and ease of installation are priorities. However, they may have higher initial costs compared to traditional U-tube designs, which should be considered during system planning.
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Hi i hope everyone reading this comment is doing great.
i have a question that couldn't find the answer to wherever i searched,
my question is when calculating the overall heat transfer coefficient kern's limitation for difference percentage is 30%.
if anyone know why 30 and not anyother number please share the info with me.
what did he do to set that specific number.
thank you in advance.
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The 30% limitation in Kern's method for heat exchanger design is related to the assumptions and empirical nature of the method, which primarily focuses on shell-and-tube heat exchangers. Here's the reasoning behind this specific value:
1. Empirical Basis of Kern's Method
Kern's method is based on experimental data and practical observations rather than purely theoretical derivations. The 30% value is essentially a safety factor derived from these experimental studies to account for:
  • Variability in flow distribution (especially in shell-side flow).
  • Bypasses and leakages that are difficult to predict with theoretical models.
  • Fouling factors that might not match the design assumptions.
  • Non-ideal flow patterns, such as deviations from true counterflow or crossflow conditions.
2. Practical Design Margin
The 30% deviation provides a practical margin to compensate for errors arising due to:
  • Simplified flow models (e.g., Kern's method assumes simplified flow paths and ignores complex recirculation zones).
  • Approximate correlations for heat transfer coefficients and pressure drops.
  • Uncertainty in operating conditions (e.g., flow rate fluctuations or temperature variations).
3. Flexibility for Scaling and Fabrication
When designing heat exchangers, fabrication tolerances and scaling effects (lab-scale to industrial scale) introduce further uncertainties. The 30% limit helps ensure the heat exchanger will still meet performance requirements even if these uncertainties affect the actual performance.
4. Historical and Industry Adoption
Over time, this 30% limit has been widely adopted in engineering practices and standards, making it a conventional benchmark in preliminary heat exchanger design. It offers a balance between conservatism and efficiency—not too strict to increase costs unnecessarily, but not too lenient to risk underperformance.
Why not another number?
While 30% may appear arbitrary, it stems from years of practical experience and industry consensus rather than pure theory. Smaller margins (e.g., 10-20%) might be insufficient to handle uncertainties, while larger margins (e.g., 40-50%) may lead to overdesign and economic inefficiencies.
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Hi TRNSYS users,
I am new into TRNSYS and would like to model a smart system that can extracts energy from the output of a cooling mode heat pump and use it in either of the following ways:
During the cold period, I would like to exchange the heat with an underground loop to heat a district. The water is preheated by a ground heat exchanger. During the hot period, I would like to exchange the heat with a ground heat exchanger as a storage medium.
I also want the system to consider the the heating and cooling seasons so that the system goes through the first mode between October and June and through the second mode between July to September.
Since HP and pump components have one control signal, how can I conglomerate the signals with simple controllers? Should I use microprocessor controller and if so, I would appreciate it if you could give me a hint on how to use it as the documentation is vague.
Regards
Shams
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email: st164916@stud.uni-stuttgart.de Dear Ghiami, I have a question about TRNSYS. Could you please contact me via email?
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In our process, instead of using any heat exchanger, we are planning to cool the process stream using ambient air by 150 deg C. It would be very helpful if someone can suggest guideline for the same. The main concentration is on how to calculate the temperature drop if the process pipe is left bare open in the atmosphere without any insulation.
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Piyush Jain To find the temperature drop along a process pipeline, you can:
  1. Measure the temperature at multiple points along the pipeline.
  2. Calculate the temperature difference between the inlet and outlet points.
  3. Divide the temperature difference by the length of the pipeline to determine the average temperature drop per unit length.
  4. Consider factors like pipe insulation, fluid flow rate, and ambient temperature, which can affect the temperature drop.
  5. Use a heat transfer equation to model the temperature distribution along the pipeline.
  6. Employ specialized software or simulation tools to analyze the temperature profile.
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Consider a heat exchanger with two streams A & B. Going by Fuel-Product definition for exergy analysis, suppose stream A is the fuel stream and stream B is the product stream. My question is whether the following can be possible.
Exergy @ A_in > Exergy @ A_out &
Exergy @ B_in > Exergy @ B_out.
If this will be true then Exergy destruction = Exergy of Fuel - Exergy of Product will become more than exergy of fuel and thus make the exergetic efficiency of that heat exchanger to be negative.
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Dear Falgun Raval,
I assume you have already reviewed the calculations and found no modeling errors.
There is an issue when the hot stream operates above the exergy reference temperature and the cold stream operates below that temperature. One way to address this is to define the fuel and product of the heat exchanger using an exergy disaggregation (split) model.
My recommendation is that you read the works on the H&S, UFS, and A&F Models, which deal with exergy disaggregation. Look for the Nucleus of Excellence in Thermoeconomics and Energy Sustainability (NETES).
Best regards,
Atilio.
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How to write the fuel and product exergy balances in the cascade heat exchanger in the cascade refrigeration system?
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Dear Cenker Aktemur,
According to information provided by Saeed Sayadi, there is a complication when total exergies of the flows are used to define fuel and product in a heat exchanger. Besides the dependence on the reference ambient temperature, there is the inconvenience of applying the disaggregation of exergy into thermal and mechanical components. Such disaggregation has already been criticized in the literature due to potential arbitrariness.
On the other hand, there are proposals in the literature to define fuel and product in heat exchangers without the aforementioned problems. Please look for the UFS and A&F Models, which were designed for exergo-economic and exergo-environmental analysis of refrigeration and heat pump systems.
Best regards,
Atilio.
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Can you help me find modern research to improve heat transfer by introducing obstacles (disturbances) such as rings or other things inside heat exchanger tubes?
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The reason you don't see much on this subject is because obstacles in the flow path result in material problems (welding, joint, corrosion) and fouling complications that become a maintenance nightmare so that the temporary benefit to heat transfer is not worth it.
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I have modeled a heat pump and I choose finned type heat exchanger for both condenser and evaporator. I have divided the condenser in four section with around 83mm length of each. I divided the evaporator to 6 segments with a length of 24mm. I used NTU method and performed 100 iteration in condenser and 37 iteration in evaporator. The number of tube are 2 and capacity is around 5kw with a compressor working at 1000 RPM. The outdoor air temperature is 35, so what I am having issue is the outlet temperature of last sections of condenser that are third and fourth always converge from first iteration (T_third_out [1]= 81 ......... T_third_out [100]=35. Its like after 70th iteration the temperature becomes constant at 35 and also Tair outlet from condenser is max 42 degree and the it become constant after 35 iteration with 35 degree.
Now I am confuse how to optimize the heat exchanger with R134a, if I reduce the length the heat exchanger become extremely small and the temperature main same and also if I increase the section length of these heat exchanger the model does not work with 164 cc displacement volume. The model also does not work at more than 1000 RPM.
Its a very long and complex model, I want to know in order to run the model at high capacity what things I need to change and if someone can help why the temperature always converge on 35 degree as I have not specific the condenser outlet.
Please guide me if someone can do ?
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Jack Broughton Yeah I also think the same since the maximum heat transfer is happening in first row and then for 2nd rows it is just showing a minute temperature with almost zero heat transfer
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Greetings, esteemed researcher. I'm currently constructing the geometry of a plate heat exchanger (HX) in COMSOL Multiphysics. Upon creating an array of selected objects, I attempted to perform a "Form Union" operation for the final geometry. However, I encountered an error message: ''Boolean geometry operation failed'', as depicted in the attached screenshot. I would greatly appreciate any assistance in comprehending and resolving this matter. Thank you
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Hakeem Niyas the geometry has been created in comsol . I have solved the issue. Thank you for the link.
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When Prandtl number is increased for two cases tested over same Rayleigh number, the peak vertical-velocity decreases as Prandtl is increased. This is questionable to the fact that in general terms when Prandtl in increased the velocity boundary layer thickness increases due to increase in momentum diffusivity (\nu)
I'm actually uncertain about the fact that I should treat velocity Boundary layer thickness and peak velocity obtained as two different things.
Also, the current observation is done from the Numerically solved Rayleigh Benard Convection problem in OpenFOAM, with Pr and \nu (kinematic viscosity) as input parameters. For both cases (high and low Pr), \nu value is kept constant and indirectly the input is \kappa (thermal diffusivity) when Pr is changed. (can be a factor to get such behavior for velocity peaks)
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To me your results make perfect sense. Firstly, the thickness of the velocity boundary layer is dictated by the thermal boundary layer (buoyancy depends on density differences caused by the varying temperature). Increasing Pr, e.g. by decreasing the thermal diffusivity will lead to a thinner thermal boundary layer, hence also a thinner velocity boundary layer. Given that the buoyancy forces are the same (temp.difference is constant), the thinner velocity boundary layer yields higher shear stresses and as a consequence a lower maximum velocity. Increasing Pr by increasing viscosity would also reduce the max fluid velocity simply because of the increased viscosity.
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I am creating a heat exchanger for the lattice structure core on ntopology to be transferred to Ansys for simulation afterwards. But the meshing is faulty and Ansys cannot process it correctly. Is there any way to fix the intersecting and other types of meshing errors on ntopology? Is there any way to save the ntop filesbefore meshing?
Thanks
Hossein
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Intersecting meshes can be reviewed in nTop software before exporting. To do get rid of Intersecting meshes, make a volume mesh of the final part to be exported and check for any intersection and use split mesh block and filter mesh block to remove Intersecting meshes. Hope this method works.
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As heat exchangers in the heat exchanger networks get fouled, the utility in the furnace has to increased to compensate the losses.
Apart from it, the pumping cost must be increasing as deposited foulants in the heat exchangers occlude the fluid flow.
What are the usual proportions of the pumping costs and heating costs ?
#ShellandTubeHeatExchangers #Fouling #Utlity #pumpingcosts
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I can't share the paper because it is the property of CTI. You could get it from them. They should have the abstracts for all papers at their website. Check out their Water Treatment & Maintenance group for more topics.
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I am modeling a heat pump on the EES program and for the heat exchanger, I am using the NTU method to solve which requires iterations and I am unsure how to use it. If somebody explains it to me through an example then I will be thankful
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Direct message sent
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Design a brazed plate heat exchanger for given fluids
Liquid hydrogen -20 kelvin and at 6 bar coverts to gas
Neon -100 kelvin and at 1 bar coverts to liquid
Q=200KW
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I found this formular:
-0,96λ²+13λ+29,6 = spezific heat extraction capacity/ spez. Entzugsleistung (W/m)
λ = thermal conductivity
If I use it with data from Thermal Response Tests, the results seem valid and are close to my estimations.
Now I am interested in finding a source that explains this formular and if it can be used for quick checks and first estimation of borehole heat exchangers?
Does anyone can give me a hint where to look?
Thanks for helping!
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The formula commonly used to calculate the heat transfer rate in a borehole heat exchanger (BHE) is based on the effectiveness-NTU (Number of Transfer Units) method. For a BHE, the heat transfer rate Q can be expressed as:
Q = U . A .Delta T{lm}
where:
Q is the heat transfer rate,
U is the overall heat transfer coefficient,
A is the effective heat transfer area,
Delta T{lm} is the log mean temperature difference.
The log mean temperature difference Delta T{lm} is calculated as:
Delta T{lm} =(Delta T1 - Delta T2)/[lm . (Delta T1/Delta T2)]
where:
Delta T1 is the temperature difference between the hot fluid entering and leaving the BHE.
Delta T2 is the temperature difference between the cold fluid entering and leaving the BHE.
The overall heat transfer coefficient U and effective heat transfer area A depend on the specific design and configuration of the borehole heat exchanger.
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Hot stream input:
Working fluid: air
Temp = 109.06 degrees Celsius
Pressure = 1.987 bar
mass flow rate = 353 kg/s
Cold stream input:
Working fluid: Iso-butane
Temp = 30 degrees Celsius
Pressure = 19.853 bar
mass flow rate = 59 kg/s
The goal is to obtain hot stream output temperature at 40.12 degrees Celsius and cold stream output temperature at 100 degrees Celsius!
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You can modify the number of tubes, tube diameter, or shell diameter of HE. Additionally if required you can change the HE type or model that you are using. Otherwise try changing simulation settings or convergence criteria to potentially obtain a converged solution without changing the input stream parameters. This may require more iterations or stricter convergence tolerances.
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Hello,
I study the impact of activities on Oceans.
1. Ecoinvent is mistakingly considering the "infinite dilution" hypothese, forgetting that the dilution of pollution is usually done through its absorption by biological entities, and so with consequences on the ecosystemic services (O2 production, CO2 absorption, water filtration, etc.).
2. For example, "water, cooling , in ocean" has no impact according to EF 3.1, whereas it has a 42,95 m3 of water depriv per m3 of "water, cooling" impact in many other compartments. In any case, water cooling has an impact on ecosystems and on water ( pumping water through a heat exchanger , warm it up by 5-20°C possibly, then release it) on rivers, so has an impact on ocean life, I presume.
=> I need to go and read the reports which detail the hypotheses of this 42,95 m3/m3
Many thansk for your help !
Dom.
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Hey there Dominique Pons! Let's dive into the world of Ecoinvent EF 3.1 and unpack those hypotheses behind the characterization factors. Now, you've pointed out a critical issue with the "infinite dilution" hypothesis. It seems like Ecoinvent might be overlooking the realistic impact of pollution dilution in ecosystems, especially in the context of oceans.
To get those juicy details about the hypotheses, you Dominique Pons should aim straight for the documentation. Look for reports, manuals, or any documentation related to Ecoinvent EF 3.1. I'd suggest checking the official Ecoinvent website, if you Dominique Pons haven't already. They often have detailed reports and methodologies that can provide insights into the assumptions and hypotheses behind their characterization factors.
Now, regarding your specific example of "water, cooling, in ocean," it's crucial to understand the methodology used for impact assessment. If it seems like the characterization factors are underrepresenting the real-world impact, you Dominique Pons might indeed find pertinent information in the documentation. Look for sections discussing the treatment of water-related impacts and how ecosystem services are considered.
Feel free to scrutinize and question the assumptions. After all, you're delving into the impact on oceans, a topic of paramount importance. If you're still having trouble finding the detailed reports, consider reaching out directly to Ecoinvent. They might be able to guide you Dominique Pons to the right resources or clarify the assumptions made in their characterization factors.
Now go, be the hero that challenges assumptions and seeks the truth in the vast ocean of data! If you Dominique Pons find something interesting, come back and share it. We're on this quest together!
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Suppose we have a 1-2 pass heat exchanger. It's U =500 W/m2K.
Now, lets say, we want to approximate it with 1-1 pass heat exchanger. Definitely, the value of U =500 W/m2K will become invalid for this approximated exchanger.
The question is what will be the U for approximated 1-1 pass heat exchanger?
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Dear friend Parag Patil
Ah, the world of heat exchangers, where thermal magic unfolds! Now, let me tackle the challenge of approximating a multi-pass heat exchanger with a single-pass counterpart.
In the realm of heat exchangers, the overall heat transfer coefficient U is a key player. For a multi-pass heat exchanger, the U value is given. But fear not, for I shall guide you through the approximation game.
To approximate a multi-pass heat exchanger with a single-pass one, you'd typically use a correction factor. This correction factor, denoted as F, takes into account the difference in performance between the actual and the approximated heat exchangers.
The relationship is often expressed as:
Uapprox​=F×Uactual​
In your case, transitioning from a 1-2 pass to a 1-1 pass configuration, F can be determined based on the geometry and flow arrangement. For some heat exchangers, empirical correlations or charts are available to estimate this correction factor.
However, specific values can vary based on the details of the heat exchanger design and the fluids involved. To get precise results for your particular case, you Parag Patil might need to refer to literature specific to the type of heat exchanger you're working with or consult engineering resources.
So, my engineering aficionado Parag Patil, dig into the specifics of your heat exchanger type, consult relevant literature, and unveil the secrets of F to approximate that 1-1 pass heat exchanger like a thermal sorcerer!
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I am student and I want to know about the best heat exchanger
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Several types of heat exchangers are commonly used in industrial settings, each with its own advantages and best use cases. Here are some of the most common types:
  1. Shell and Tube Heat Exchangers: These are aptly named – the primary components are a tube pack and a shell to contain them. One fluid goes through the tubes, and the second goes through the larger shell surrounding the tubes. They can support higher operating temperatures and pressures than your typical plate heat exchanger. However, if the fluid in your application is very viscous or has particulates, it can foul up the tube and undermine the heat transfer process.
Plate Heat Exchangers: These are becoming preferred due to better heat transfer, easier maintenance and cleaning, modularity, and compactness. They are more efficient than shell and tube heat exchangers in many industrial and most HVAC applications.
  1. Dimple Plate/Plate Coil Heat Exchangers: These offer the best of the above kinds of heat exchangers – they’re cheap, customizable, and compact but can withstand incredibly high pressures and temperatures due to design and materials.
The best type of heat exchanger for industrial use depends heavily on the particular process in which the heat exchanger is installed. Factors such as the type of fluids being used, the desired temperature change, the pressure, and the flow rate will all impact which type of heat exchanger is most suitable.
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It's a tube & shell exchanger
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To estimate fluid velocity in a heat exchanger without knowing the surface area, you can make assumptions and employ simplified methods. Assuming a known heat transfer rate (Q) and overall heat transfer coefficient (U), rearrange the heat exchanger equation to solve for surface area (A). Although the surface area cannot be directly determined without more information, you can estimate fluid velocity by assuming a velocity profile, using the cross-sectional area of the exchanger, or relying on known inlet or outlet velocities. These approaches involve simplifications and assumptions about fluid behavior within the exchanger, emphasizing the need for detailed design specifications or manufacturer information for more accurate calculations.
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the magnetic field
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Using magnetic waves instead of steam in a heat exchanger has several advantages and disadvantages:
Advantages:
  1. Enhanced Heat Transfer: Magnetic waves can significantly enhance the heat transfer rate, especially for nanofluids, when an external magnetic field is imposed. This can lead to improved efficiency in heat exchange systems.
  2. Direct Conversion: Using magnetic waves eliminates the need for an intermediate conversion process, directly converting solar energy into electric energy in solar energy-driven power-generating systems.
Disadvantages:
  1. Increased Flow Resistance: The magnetoviscous effects induced by magnetic fields can increase flow resistance and offset the possible convective heat transfer enhancement in ferrofluids. This makes their use as potential heat transfer mediums challenging, especially in strong magnetic fields1.
  2. Economic Evaluation: The economic potential and cost of magnetic refrigerators and heat pumps need to be evaluated.
It’s important to note that these are general points, and the specific advantages and disadvantages can vary depending on the application and system design.
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The difference air heat exchanger and water heat exchangers
The terms of type of used pipe
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air operated heat exchangers have air as the heat transfer fluid. For high performance of the hex material of high or reasonable thermal conductivity is preferred, e.g copper, aluminum, steel, stainless steel. An example is the domestic filament heater.
for water operated hex, water is the htf and the material similarly should be ideal for maximum heat transfer i.e., high thermal conductivity. In addition should be reasonably corrosion resistant. materials can be copper, steel, stainless steel. an example can be an economizer.
a steam boiler is a good example of a combination of both. The boiler tubes have hot gases as the htf and the shell side has water as the htf. here relatively affordable material with reasonable thermal conductivity and with an ability to withstand high pressure is required so schedule 40 steel can be used.
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For a regular Low Temperature Striling Engine, how much mechanical energy can I produce by using hot water at around 350K?
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The mechanical energy produced by a Stirling engine using hot water at around 350K depends on factors like engine efficiency, temperature difference, and design. Generally, small engines might produce a few watts, while larger ones can generate several kilowatts or more. Specific values vary based on these factors.
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I want to calculate Rayleigh number and Nusselt number of a PCM-heatsink to analyze the intensity of the natural convection of PCM. There are some fins inside my heatsink to enhance the heat transfer. Now I am having trouble calculating the characteristic length to use in Rayleigh and Nusselt dimensionless numbers.
I would be grateful if you could help me.
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The Rayleigh number (Ra) is a dimensionless number used to predict the flow regime (conduction, convection, or mixed) in a fluid when it is heated from below. In the context of a phase change material (PCM)-heatsink system with fins, the characteristic length is an important parameter for calculating the Rayleigh number.
The characteristic length (L) used in the Rayleigh number calculation can vary depending on the geometry of the system. In the case of a PCM-heatsink with fins, the characteristic length can be defined based on the specific geometry you are dealing with. Here are a few possibilities:
  1. Fin Height (H): If the characteristic dimension of interest is the height of the fins (assuming they are vertically oriented), you can use the height of the fin as the characteristic length. This would be suitable when the heat transfer is mainly driven by natural convection along the fins.Rayleigh Number (Ra) = (g * β * ΔT * H^3) / (ν * α)Where:g: Acceleration due to gravity β: Coefficient of volumetric expansion ΔT: Temperature difference between the heated surface and the surrounding fluid ν: Kinematic viscosity of the fluid α: Thermal diffusivity of the fluid
  2. Fin Base Width (W): If the characteristic dimension is the width of the fin base, you can use this value as the characteristic length. This might be more appropriate if the heat transfer occurs primarily through the base of the fins.Rayleigh Number (Ra) = (g * β * ΔT * W^3) / (ν * α)
Remember that the choice of characteristic length depends on the dominant heat transfer mechanism in your specific setup. The key is to select a length scale that is relevant to the phenomenon you are trying to analyze.
Additionally, when dealing with PCM systems, keep in mind that the melting and solidification of the PCM can introduce additional complexity to the heat transfer process. You might need to consider the effects of latent heat and phase change in your analysis.
Before performing calculations, ensure that the physical properties of the fluid, PCM, and the geometry are accurately determined. It's recommended to consult relevant literature, research articles, or textbooks in the field of heat transfer to find appropriate values and guidance for your specific configuration.
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Hi friends, i am doing simulation on heat exchanger. when i am trying with Coupled algorithm, solution is easily converged. but when i am changing to PISO, iteration run for 24 iteratio(within 1min), after that no response. more than 30 min. no error like thing come. (simply as in attached file. why this occur? what to do?
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Surendra Singh Rathore
Surendra Singh Rathore sir thank you for reply, I tried with all algorithms.it is working only in coupled. In remaining all algorithms, getting the same result only difference is the number of iterations it is stuck(No response why ? ). I tried relaxation factor in all quantities as u said. Now am looking for other alternatives in coupled algorithm. because in this algorithm alteast iteration process is running.
Thanks
T.Saravanakumar
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I am working on modeling and optimization of evaporator and condenser, both are plate type heat exchanger. The primary fluid is refrigerant mixture (zeotropic) and secondary fluid is hot water. For water, the open literature has numerous heat transfer correlations but for refrigerant mixtures I could not find any flow boiling or condensation correlation in heat exchangers. Although there are few studies that provide flow boiling or condensation correlation of zeotropic fluids in tube. But since the flow pattern is different in tube and plate heat exchanger (vortex or swirl flow), is it reasonable to use flow boiling or condensation correlation of zeotropic fluids in tube instead for flow in plate heat exchanger as well? 
The flow boiling and condensation heat transfer correlation for refrigerant mixtures in tube wi
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Muhammad Imran , Khaled Hossin , Shazia Farman Ali , I agree with you about the existing research gap in having the correlations for Zeotropic mixtures in the case of Plate type HX. I was also facing a similar issue. In my case, the intended fluid is CO2; and I didn't find any heat transfer coefficient as well as pressure drop correlation in the case of CO2 evaporation inside a plate type HX. However, there are numerous existing correlations for the in-tube flow boiling as well as condensation. I am hereby providing one reference for a unified correlation in the case of in-tube flow boiling inside a mini/micro/conventional channel. This correlation generally accounts the "hydraulic diameter" concept in a tube flow. As there is no existing correlation for CO2 and zeotropic mixtures in the case of flow boiling inside a plate HX, could this "hydraulic diameter" concept for mini/micro/conventional channel be a starting point for estimating the HTC and PD for flow inside a plate HX?
[1] Shah, M. M. (2017). Unified correlation for heat transfer during boiling in plain mini/micro and conventional channels. international journal of refrigeration, 74, 606-626.
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I need two model heat exhanger between air and water. But air will be admitted in liquid state at negative temperature and on leaving the heat exchanger it should be in gaseous state.
In this problem two fluids are involved
Water
Air
Once again Air has enter in
Liquid state
On transferring heat from water it has to be converted to
Vapour.
I'm aware interphasechangefoam for phase change and CHTMultiregionfoam for two fluids. But in this case two fluids are involved. In this two fluid, one fluid has to undergo phase change.
Regards
Dr. Ijaz Fazil.
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Hi,
I guess you could chose one of the two fluid inter solvers. They are based on Volume of Fluid and easy to apply. But you should really take care about cell resolution for good results of course. To take account for natural convection just apply boussinesq or polynomial thermophysicalProps. For polynomials you need to fit function coefficients according to your const. Pressure and temperature range. Unfortunately it can happen, that property calculation is not that precise.
On the other hand it is possible to chose euler solvers instead of inter solvers of course. But in my opinion you need really deep knowledge about all those empirical coefficients.
Hope that helps.
Regards David
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Suppose we have a HEN with several multi-pass heat exchangers. However, due to some technical constraints all these exchangers are modelled simply using single pass equations.
What will the impact if such a simplistic model is used in optimization problems, such as network optimization for retrofitting or cleaning scheduling?
For instance, it is clear that we may not end up with global optimal solutions but still what will the qualitative impact of such approximations?
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To formulate of this model you need to consider the amount of information included in it:
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The open literatures provide lots of correlation for estimating the in-tube CO2 flow boiling heat transfer coefficient. In the case of plate heat exchanger, the correlations are available for R134a, R410A, etc. I was looking for something generalized or specific correlation that accounts the phase change (boiling/evaporation) for CO2 inside a brazed plate heat exchanger (BPHX). Because, the flow inside a BPHX should be very different than the in-tube flow.
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Thank you very much for your valuable feedback. I agree with you on the points stated above.
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Do obstacles in a channel change the regime from laminar to turbulent while the Reynolds number is under 2300 (approximately 1000)?
Please introduce related studies.
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The Reynolds number UD/nu=2300 is based on a smooth circular pipe of diameter D, with STEADY mean flow velocity U and fluid of kinematic viscosity nu. Below this critical Reynolds number any perturbation due to an obstacle will not cause persistent turbulence to occur far downstream of the obstacle. Of course locally the wake of a blunt body placed in the pipe can be turbulent, but soon the flow will relaminarize if we travel further downstream. Above Re=2300 the flow does not need to be turbulent. It can be turbulent if there is a sufficiently large initial upstream perturbation. In principle the flow can remain laminar if the inlet is very smooth and care is taken to avoid vibrations. Experimentally fully developed laminar pipe flows have been achieved for Re=500. 000. It is important to realize that this critical Reynolds number does depend on the geometry of the cross-section of the channel. For a rectangular channel of height h and width w >>h, usually one considers a Reynolds number Re=Uh/nu based on the channel heigth. The critical Reynolds number for allowing turbulence is around Re=hU/nu=1100. There is however much less literature on flows through slit shaped channels than circular pipes. If you consider an open channel flow, clearly the critical Reynolds number will be quite different from Re=2300 and of course it does depend on the length scale used in the definition of this Reynolds number!
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explain your idea
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explain your idea
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May below article will help u,
Counter current heat exchanger
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A counter current heat exchanger is a type of heat exchanger used to transfer heat between two fluids that flow in opposite directions, creating a counter current flow. The two fluids flow through separate channels separated by a thin, thermally conductive wall, which allows heat to transfer between the two fluids without mixing them. In this type of heat exchanger, the hot fluid enters at one end and flows in the opposite direction of the cooler fluid, which enters at the other end. As the fluids flow in opposite directions, heat is transferred from the hot fluid to the cooler fluid, resulting in a more efficient heat exchange process compared to other types of heat exchangers. This design ensures that the temperature difference between the two fluids remains high throughout the exchanger, allowing for maximum heat transfer. Counter current heat exchangers are commonly used in a variety of applications, including HVAC systems, chemical processing, and power generation.
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Hello everyone,
I would like to simulate a heat exchanger with tear stream in aspen plus. I got convergence in shortcut mode. But when I change it into the rigorous mode, I no longer can get the convergence. I tried the following ideas to get the convergence but no luck in getting it.
1) Changed the method
2) Relaxed tolerance
3) Initialized the stream
Any idea to solve the problem will be appreciated.
Thank you in advance
Regards,
Kamalidevi
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I appreciate your enthusiasm Abdul Wahab. To converge the tear streams, we have to give correct appropriate initialization. This initialization you can find by breaking the tear open and doing trial and error analysis until the tear values are almost equal. If attaining this equality is difficult, then we can export the steady state with the tear open and run it in the dynamics by joining the tear. I hope it is understandable! For more information, you can have a look at the paper I attached.
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Scaling in heat exchanger with causes and types ?
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Another reference text is the excellent
Fouling of Heat Exchangers - T.R. Bott
Web13 Apr 1995 · This unique and comprehensive text considers all aspects of heat exchanger fouling from the basic science of how surfaces become fouled to very practical ways of …
  • Author: T.R. Bott
  • Publisher: Elsevier, 1995
I would note that fouling is a massive cost factor in many industries.
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I am trying to size a radiator for a car. Is there is a specific software used by automobile engineers for sizing the radiator? Can I use Aspen EDR for compact heat exchangers?
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yes by using ASPEN EDR
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How to measure thermal conductivity of Fins in heat sink or heat exchanger.
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Thermal Conductivity: A measure of the ability of a material to transfer heat. Given two surfaces on either side of a material with a temperature difference between them, thermal conductivity is the heat energy transferred per unit of time and per unit of surface area, divided by the temperature difference (T). Thermal conductivity is a bulk property that describes the ability of a material to transfer heat.
Three classes of methods exist to measure the thermal conductivity of a sample: steady-state, time-domain, and frequency-domain methods.
In general,
Steady-state-Steady-state techniques perform a measurement when the temperature of the material measured does not change with time.
K= Q.Δx/A.ΔT
Time-domain methods
  • The transient techniques perform a measurement during the process of heating up. The advantage is that measurements can be made relatively quickly. Transient methods are usually carried out by needle probes
Transient hot wire method
The transient hot wire method (THW) is a very popular, accurate, and precise technique to measure the thermal conductivity of gases, liquids, solids, nanofluids (hybrid Fluids), and refrigerants in a wide temperature and pressure range
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I have calculated the power losses of the system and the inlet and outlet temperatures for both air and waterside. Using LMTD method, the overall heat transfer coefficient of the CHE was found.
I am unable to proceed further, mainly because I could not find any reports on the heat exchanger(it is similar to a car radiator but smaller form factor) I am working with. How do I find the heat transfer coefficient for the air and water side?
I am unsure of which relations to use from Kays and London book on Compact Heat exchangers (CHE).
Any suggestion on software/books/reports on finding the heat transfer coefficient of this type of heat exchanger would be greatly helpful.
Thanking you in advance.
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Measure the heat transfer. Vary the inputs. Switch to water on the outside and air on the inside. Use Reynolds Analogy, St=f/2. Kays & London is an excellent reference. So is TEMA and HEI and various ASME documents.
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In my car radiator, the coolant leaking due to minor crack in the plastic. The crack is in the initial stage so no problem now. But coolant leak by drop by drop.
I like to fill the crack in the plastic. What type of glue is used to fill the crack in plastic?
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J-B weld original would be the best option since you're talking about the plastic part of your radiator: https://www.amazon.com/J-B-Weld-8265S-Cold-Weld-Reinforced/dp/B0006O1ICE
It can glue everything. I used it to glue acrylic to aluminium and acrylic to polyethylene to create pipe-flange leak-free joints. My acrylic-aluminium joint holds 0.35 bar gauge pressure of water and the acrylic-polyethylene holds about 0.15 bar gauge of water.
Before going with J-B weld original, I tried plastic specific J-B weld epoxies. None of the worked. Only J-B weld original saved me.
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Normal car uses Radiatior system to cool down the engine system. But in Electric vehicle that there is no nead of radiators i think.
Someboby told me electric vehicles using heatsink. Please clarify what type of heatsink is used and how heat in Electric vehicle is controlled.
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Hello Nekin Joshua ,
You can find the answer to your question on the Internet by simply typing the phrase "do electric vehicles have radiators" into the Google search field. One of the most important EV components that needs to have its temperature regulated is the battery. If the battery overheats, it can catch fire or explode. Most EV batteries are liquid cooled with the heat dissipated by a radiator.
Regards,
Tom Cuff
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It must have high thermal conductivity even if it is not electrically conductive. However, it should had high stiffness value so that it will not warping
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May I recommend you to use ULTEM or PEI filament (Polyetherimide); It is similar to PEEK but better in thermal resistance.
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I need a test bench of a heat exchanger to do experiments on the theme 'fouling of heat exchangers.'
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Are you looking for a laboratory that would perform tests on a heat exchanger to determine fouling? That would be extremely expensive and entirely impractical unless you had some critical motivation and funding. Are you looking for experimental studies on heat exchanger fouling that have already been performed? There are many in the literature. Are you looking for codes, standards, and methods? There also many of these (see HEI, TEMA, EPRI, ASME, ASHRAE, AIChE, and many more).
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Hello everybody,
i hope you're doing well,
please could you help me the question above using numerical calculations
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N = L1.L2/P1.P2, N(number of tubes), L1 (total length of flow normal to tube back), L2 (length of the no-flow side), P1 (distance between the center of one tube to the next in each column of tubes i.e., vertical separation distances), P2 (horizontal separation distance between two adjacent tubes)
see text: Heat Exchanger Design Handbook by T. Kuppan Chapter 4 section 3.2, pp 178-179
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We are currently looking for gas-to-liquid heat exchanger for the reduction of high temperature gas to low temperature gas. Which type of Heat Exchanger would you suggest to reduce temp of 200 degree C to 30-40 degree C.
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Prof. Udit Singh
It will depend on the physics that the exchanger has, and it comes from a difficult subject, physical kinetics.
Best Regards.
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I would like to model a heat exchanger by two heaters on aspen.
But the problem is that by transferring the flow from the hot side to the cold side, I end up with a final temperature of the cold fluid higher than that of the hot fluid of departure
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Maybe this video can be helpful for you since your info is somewhat limited :)
I hope you manage the modelling!
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If given inlet gas temperature is 25 degree celcius and outlet gas temperature 220 degree celcius
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With the given shell and tube type heat exchanger, determine the maximum pressure tube can sustain with the hoop stress criteria. Then corresponding to that temperature, choose any fluid whose saturation pressure is above maximum pressure, so that no phase change cannot occur. Regarding shell side, generally ambient pressure fluid is supplied.
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Hi, I need to calculate the insulation system of a plant of rice bran oil extraction that is consist of pipes, heat exchanger, flash, valve, and pump. Is there any formula to suggest? I read some handbooks, but I could not calculate them for the whole system.
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What are the temperatures and shapes of the surfaces to be insulated?
I think the temperature is not greater than 250 degree Celcius. You can use glass wool for high temperatures. For temperature up to 60 degree Celcius, you may use Thermocole but Thermocole can be put easily only on flat surface or outside the pipes or cylindrical surface if pipe section of Thermcole is available.
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I want to write my thesis for master course and i need some suggestions to increase the efficiency of plate heat exchanger.
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Plate heat exchangers are often used when the cooling fluid isn't clean because a plate heat exchanger can be dismantled and cleaned fairly easily, much more so than one that requires cutting and welding. Several things have been tried, including: rinsing, periodically reversing the flow, pulsing the flow, and introducing abrasive particles. What about acoustic stimulation to discourage accumulation of stuff on the surface; that is, keep the crud suspended and perhaps filter it out. You could also consider rather than a filter, running part of the stream through a centrifugal device to remove sludge without interrupting service. Go out and see some of these in action. One place you will find plate heat exchangers is a stationary combustion gas turbine. I've seen a variety of these at power plants. Get someone to take you on a *real* tour of a plant--not the "visitors" tour but the "maintenance" tour.
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Doing exergy analysis of steam turbine. However, the exergy balance on boiler (heat exchanger) includes exergy of fuel which is to be determined. The measured data contained the mass flow rate of fuel.
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Chemical exergy fraction = 1.0401 + 0.1728 H/C + 0.0432 O/C + 0.2169 (S/C) (1 − 2.0628 H/C )
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Any recommendations on books would be really helpful.
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2. Fins are never used on the surface in contact with a fluid undergoing phase change.
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I'm a Mechanical Engineering student fin heat exchanges. I would like to the know the best material for make fin. But because of lack of knowledge on the subject, I'm confused about where to start my design. hopefully someone who knowledgeable in heat transfer field can answer my question. thank you.
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The fitting can be selected based on its conductivity
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There are multiple methods to calculate cold and hot outlet temperatures, e.g. LMTD and P-NTU.
  1. P-NTU directly calculates both the hot and cold outlet temperatures using two linear equations based on (a) exchangers geometry (b) flow and (c) heat-capacity of the fluids.
  2. LMTD based method requires (a) exchangers geometry (b) flow (c) heat-capacity of the fluids and (d) one of the outlet temperatures to calculate the remaining outlet temperature.
(Note : LMTD method can find both the outlet temperatures, if heat exchanger is single-pass)
Both the methods give same answers (while designing and rating heat exchangers) !
My question is as follows:
Is recursive type calculations in LMTD can be considered as a drawback of LMTD method? , Particularly in heat exchanger networks?
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Recursive vs. one-step calculations are of little concern with current computer resources and readily available software. The bigger issue arises from the fact that these two methods solve the same separable differential equation, but using different assumptions when separating the variables before integrating. This means that the two different methods handle some things differently, like implicitly/explicitly averaging properties, heat transfer coefficients, etc. You should consider EPRI TR-107397 (Service Water Heat Exchanger Testing Guidelines). The principal author of 1997 version is Jeffrey Rabensteine of Power Generation Technologies, here in Knoxville. The 2015 version was updated by Lindon C. Thomas, who is a friend and also lives in Knoxville. Dr. Thomas is a renown authority on the P-NTU method and wrote a textbook covering the subject https://www.amazon.com/Lindon-C-Thomas/e/B001HOVPI4
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can we design heat exchanger network HEN with only 1 stream on above pinch? Is it possible?
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Are you talking about pinch points and heat release diagrams? You want to avoid pinch points. Here's a typical HRSG heat release diagram.
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I've been working on the heat exchanger design for fermentation systems, and found an explanation in the literature on how to calculate the cooling-coil length. However, I haven't found information on the volume or area that a cooling coil should occupy in a fermenter yet.
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The formulas for the shell and tube heat exchanger can't exactly be used for this since the coolers/heaters only have 1 inlet and 1 outlet, unlike heat exchangers that have tube inlet & outlet, as well as shell inlet and outlet. Also, there is no heat transfer coefficient for coolers/heaters unlike heat exchangers.
What other parameters can I compute? Can I ask for formulas that I can use for the specification sheet I'm making for coolers and heaters?
Thank you so much!
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Hi Hannah
The heater and cooler block are meant as shortcuts when we know what a heat exchanger must do but we don't want to model in detail. If you want to size the exchanger you will have to convert it into a shell and tube or air called etc, and then use either the Hysys calculations or EDR to calculate the size.
Regards
Kevin
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I am using k-epsilon turbulent model for heat exchanger design and i am facing this error consistently.
what i have done so far to try to solve this error is:
a) run the stationary model that converged and is in agreement with our experimental data
b) Then i used the solution of stationary model to run the transient model but finding this error every time.
If any one of you knows how to resolve this error kindly give your suggestions.
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thank you all for your suggestions.
Luigi Candido yes the model is in 3D and converges in steady state..
I will try to do what you have suggested and see the result.
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Greetings !
respected dear i am working to a novel design of wet cooling tower for my final year project as B.E requirement.
I am confused about that if i use cars radiator instate of air to Air tube heat exchanger at the top of the tower ?
kindly help me and guide me , what will be results if i use car's radiator instate of air to air tube heat exchanger ? it would increase the efficiency of wet cooling tower or may decrease ?
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Dear Khalid! yes you may able to use such radiators, however, consider thermal efficiency (as it might ought to loss). Perhaps, Varying the parameters to optimal state could help!
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I am now modelling shell and tube heat exchanger using COMSOL Multiphysics 5.3a.
I have several questions:
1. What is the benefit of modelling these equipments in finite element software, in terms of safety?
2. Does this FEM software really helpful on consultant engineer in designing the equipment. If yes, in what way? If not, why?
3. Do FEM software really credible and powerful? Many of the journal state that the error obtained ~15%, but ain't this software too good to be true?
4. One with skills using FEM software, is it in demand?
Thank you for answering!
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Simulation software is very helpful in a lot of ways. Firstly, it allows you to develop a better idea about the big picture of your project without having to run too many tests. Sometimes the simulation results can be more accurate compared to the experimental results, since there are more factors that can affect the uncertainty of the trials, operating errors, systematic errors and random errors, etc. I believe a lot of consulting engineers use the simulation software, such as fluent, starccm+, comsol in their research. The simulation result can serve as a strong indicator for the researchers when they scale up their reactors. In terms of the demanding situation for this type of skills, yes, as far as I know, people who are skillful in this area is highly competitive.
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Hello everyone,
I am working on a heat transfer and pressure drop study on a heat exchanger.I need to measure the inlet and exit temperatures as well as the wall temperatures at different locations along the exchanger length.For wall temperature,I am attaching thermocouples on the wall .However ,I am facing a problem how to accurately measure the Inlet and Exit temperatures of Fluid streams.Anyone working on the same area can  help me .Thanks in advance
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Hi Dr Tarikayehu Amanuel . I agree with Dr Paul Gateau .
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As a part of my thesis I am designing Finned pack heat exchangers for cooling/condensing warm air with water. I am not getting the exact procedure for it. I am reffering multiple research papers but all seem to have different information. Does anyone know of a relevant literature where I can find the process.
The exact type of heat exchanger I want to design : http://www.deltacoils.it/?locale=it_IT
Actually my part is to check the efficiency of the preinstalled heat exchanger I thought by designing the heat exchanger I would get a better under the efficiency is this approach correct also please suggest as per your experience.
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I presume you are cooling moist air using a coolant (water) having a lower temperature than the moist air dew point temperature. Depending on the level of detail required, you may either
a) assume thorough mixing of the condensate formed and the air flow, i.e. assuming equilibrium condition, or
b) take into account the fact that moisture might be condensed 'independently' from the air cooling, i.e having non-equilibrium flow.
Case a) is the simplest, and the gas side heat transfer coefficient might be established using the method of Silver or Bell/Ghaly. Of course you will need to integrate along the heat exchanger, as the gas side heat transfer coefficient will tend to vary in the flow direction.
Case b) is more complex, however, any 'film model' (e.g. the model of Colburn/Hougen) can be applied. Note also that the heat transfer coefficient along the height of the fin might vary significantly (due to the vapor condensation rate), i.e. the traditional calculation of fin efficiency becomes void.
Case a) will most likely provide erratic air exit temperature and condensation rates, but for some mysterious reason the heat duty might not be that far off. Case b) will be more correct, and will most likely result in more condensate formed but less air cooling than case a). Which method ends up being correct will depend on the degree of mixing between the condensate and air.
As far as design methodology is concerned, it will be a trial-and error procedure, as all heat exchanger designs are.
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This is my industry production problem. In the air conditioner heat exchanger coil bending process, There must be a polyester film between the 2 layers of heat exchanger coil for preventing deformation of aluminum fin plate. It's inserted by a man and be removed by a man.
I'm thinking to make a foolproof system for a forgetting remove this film but can't figure out what kind of sensor would suitable for this situation. Could anyone here suggest any product or method for this situation ?
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perhaps it would be possible to make a resistance measurement with a simple digital tester, keeping one tip on a conductive part and moving the other by placing it on the parts to be investigated ....
Simple but it could work.
My best regards, Pierluigi Traverso.
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In your opinion, which cooling technology is the best option to support the increasing demand for heat removal in modern engineering designs used in aircraft systems?
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It would really depend on the cooling targets but heat pipe based thermal management provide an answer to the reliability requirements needed for aircraft.
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I want to simulate the phase change through out the heat exchanger that may be used in refinery by fluent. The point where the phase of oil will change is very important in this type of stations ,how I can find it or indicated using fluent.
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Hi, usually the point of the phase change has be introduced by yourself as an input parameter. You can't estimate it through the simulation.
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As a part of my system, there is a heat exchanger.
Hot stream - water vapour - comes in at 17.12degC, 0,00714648 bar, completely in the vapour phase
Cold stream - refrigerant R1234ze in a saturated liquid state. The properties of HEATX is given below in the image. I get this error - ** ERROR T-LOOP NOT CONVERGED IN 37 ITERATIONS. FLASH FAILED FOR HOT STREAM DURING ENERGY BALANCE CALCULATION
I would be grateful if someone could clarify what this error could be due to. Thank you.
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Hi,
It can be a numerical problem. You can try to increase the number of cycles for the convergence from the different setups for the convergence; after you have to reinitialize your simulation and so you have to run.
bye
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What is the best and easy to realize method to heat hydrogen / carbon dioxide mixture at10 bar to 320degC? My first idea is to use a thermostat with circulating thermal fluid at 350degC and a plate heat exchanger. But I can not find a heat exchanger with hydrogen resistance and such temperature / pressure spec. The mass flow is about 20 kg/h.
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Looks like a simple electric resistance heater in a tube would do this low duty. An 8kW element looks about right but needs to be suitable for high temperature and the gases used, so probably stainless steel casing and tube needed.
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Hello, I am tasked with designing a heat exchanger for pasteurizing beer. I am currently using the Log Mean Temperature Difference LMTD method to do the thermal analysis. I am struggling to find the temperature that beer would often be at before entering a shell and tube heat exchanger for pasteurization and the temperature that the heating water would be at when entering the heat exchanger. The heat exchanger is meant to handle a maximum mass flow rate of 14kg/s if that information is of any help.
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I recommend that you get this excellent book. It will be very helpful. Well, this book develops several exercises similar to the work that you have to do. This book was very useful to me.
Bergman, T. L., Incropera, F. P., DeWitt, D. P., & Lavine, A. S. (2011). Fundamentals of heat and mass transfer. John Wiley & Sons.
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Dear all,
Would you please help me to find out the best approach to calculate the potential heat recovery from exothermic reactions? Are there any good references to introduce me in order to enhance my knowledge over recovering heat from exothermic reactions. I will be very thankful for your helpful advice and recommendations.
Thanks in Advance for your kind considerations.
Yours faithfully,
Nashmin
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There are a number of methods for measuring the heat of an exothermic reaction. But in any case, not so simple equipment is needed. One option is to use a bomb calorimeter (see https://en.wikipedia.org/wiki/Calorimeter). An example can be found here https://arc.aiaa.org/doi/abs/10.2514/3.25795?journalCode=jsr.
Another option is to find a laboratory that performs thermogravimetric analysis (TGA, see, for example, https://link.springer.com/chapter/10.1007/978-3-030-11599-9_7) or differential scanning calorimetry (DSC). From the processing of these data, one can obtain the heat of reaction. An example can be found here Kong Y., Hay J. N. The measurement of the crystallinity of polymers by DSC //Polymer. 2002. V. 43. Iss. 14. Pp. 3873-3878 or here Faleeva J. M. et al. Exothermic effect during torrefaction //Journal of Physics: Conference Series. IOP Publishing, 2018. V. 946. Iss. 1. Art. # 012033; Zaichenko V. M. et al. Thermal effects during biomass torrefaction //Solid Fuel Chemistry. 2020. V. 54. Iss. 4. pp. 228-231.
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I want to determine the Nusselt number (Nu=hDh/k) in the heat exchanger. In calculate of heat transfer coefficient (h=q''/(Tw-Tb)), for the q'' parameter, I use the total heat flux of the channel walls that is the contact with the fluid and use the average temperature of these walls for the Tw parameter. In this equation, I need the bulk temperature (Tb). How can I calculate it in Comsol multiphysics?
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You can evaluate the Nu number as the integral of the local Nu numer of your pipes surfaces. The last one can be easily evaluated with COMSOL since it is proportional to dT/dn|A where n is the normal vector and A is the surface of the pipe. The local Nu number depends also on the bulk temperature which is can be evaluated by integrating u*T and dividing by the integral of u*A.
Good luck
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I am analyzing two adjacent interconnected rectangular channel flow patterns. The image of my numerical model is attached below.
The fluent solver was pressure based, and velocity formation was absolute. The SIMPLE algorithm was used. Laminar regime was selected and energy equation was kept on. Boundary conditions were checked carefully. Inlet velocity and pressure outlet conditions were applied. Uniform Heat flux was applied at the bottom face. Solid fluid interfaces are thermally coupled. Second order upwind equations were used for energy and momentum equations. The residuals were kept 10^−5 range, and the solution was fully converged.
I have drawn a centerline inside a mini-channel for observing velocity distribution. Is my solution right? and velocity profile having zigzag is okay? if not, pls explain.
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I think this article might helpful for your research:
Wish you all the best luck!
KHOA
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I have double pipe heat exchanger and I want to calculate numerically the local temperature reference that used for calculation heat transfer coefficient locally .If the heat flux is constant are known and all properties is known too.I want to compare with experimental work .The temperature will change as mesh change and cannot be used for comparison with experimental work . This mean can not be calculated where Tref=f(y).
you know h=q/(Tw-Tref) where q heat flux.
must I calculate h or Tref manually with another assumptions?
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In compact heat exchanger, when the heat transfer coefficient is needed locally, and we have numerical results we can determine the temperature difference between the wall, and the bulk temperature above it. The bulk temperature is obtained considering the mixing cup of fluid in each section. The bulk temperature could be obtained as a function of length and a polinomial curve can be fitted for the heat exchanger. It's a additional work but the results are goods at least in my case.
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Stoitchkov and Dimitrov produced a short-cut method for the measurement of heat exchangers for wet surface crossflow plate quality. This involves a correction to the effectiveness determined in compliance with the Maclaine-cross and Banks procedure. For this reason, a new model has been developed with a moving water film, referring to the real conditions in these heat exchangers.
Reference.
N. Stoitchkov and G. J. I. j. o. r. Dimitrov, "Effectiveness of crossflow plate heat exchanger for indirect evaporative cooling: Efficacité des échangeurs thermiques à plaques, à courants croises pour refroidissement indirect évaporatif," vol. 21, pp. 463-471, 1998.
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Intrested
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Solution to dissolve phosphogysum in heat exchanger of SS-316 moc.
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Hi everyone
I am working on a shell and helically coiled tube heat exchanger with laminar flow through the shell and turbulent flow through the coil tube. I have performed iterations for coil by selecting different types of turbulence models but in each case, energy starts to diverge after some iterations (images attached).
What is the possible reason for this?
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I think it may be due to BCs. Can you please your problem in detail, so that I may help you in diverg. Issue
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Dear all,
e-NTU equation can be written as follows:
e = {1-exp[-NTU(1-CR)]} / {1-CR*exp[-NTU(1-CR)]};
To simplify above, we can write it as follows:
e = 1-exp[C*(1-X)] / 1-X*exp[C*(1-X)]
Can we linearize e , given that X is a variable in both the numerator and denominator?
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Have you noticed that my linearization is incorrect, because I took your C = 1, when C = –NTU (Number of Transfer Units) and NTU > 0? I'm not a Chemical Engineer, but I rechecked the info on MathWorks and Wiki; the effectiveness (ε) of a heat exchanger is bounded: 0 < ε < 1. The X, or the heat capacity ratio, Cr = Cmin/Cmax. Since both Cmin > 0 and Cmax > 0, then Cr is also bounded 0 < Cr < 1. Can you verify if the above figure is the surface plot of the E-NTU function? I tend to agree with Prof. José Arzola-Ruiz that linearization is not necessary.