Solving Thermodynamics Problems with Helium

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SUMMARY

This discussion focuses on solving thermodynamics problems related to the Brayton cycle using helium as the working fluid. The key points include calculating heat flow (ΔQ) and net work per kilogram for the cycle, specifically for two moles of helium. The discussion emphasizes that ΔQ for adiabatic processes is zero, while for isobaric processes, it is calculated using the formula ΔQ = n * Cp * ΔT. Additionally, it highlights the importance of using specific heat capacities and specific volumes to derive work and heat flow per kilogram accurately.

PREREQUISITES
  • Understanding of the Brayton cycle and its processes
  • Knowledge of specific heat capacities (Cp and Cv) for helium
  • Familiarity with thermodynamic equations for heat flow and work
  • Ability to convert moles to mass for helium (molar mass of helium)
NEXT STEPS
  • Calculate specific heat capacity (Cp) and specific volume (V) of helium at given temperatures
  • Learn how to apply the equation W = P * V for isobaric processes
  • Explore the relationship between net work and total heat flow in a complete Brayton cycle
  • Study the implications of using specific heat capacities in thermodynamic calculations
USEFUL FOR

Students and professionals in mechanical engineering, particularly those specializing in thermodynamics and energy systems, will benefit from this discussion. It is also valuable for anyone looking to deepen their understanding of the Brayton cycle and its applications using helium as a working fluid.

sportsrules
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thermodynamics!

Another question regarding this question :

The question gives a picture of a brayton cycle with temperature on the x-axis and pressure on the y-axis. It is for the monatomic gas, helium, and we are told that there are two moles of helium. The diagram consists of two adiabatic processes and two isobaris processes. You are given two temparatures and the asked to find the other two. I did that just fine. However, then it asks you to find the heat flow (delta Q) per kilogram of helium for the entire cycle and net work per kilogram for the cycle. I know that delta Q of adiabatic processes are 0, so I would only have to worry about the isobaric processes. I know that for the isobaric parts, the delta Q will be equal to n*Cp*change in temperature. So, to find the heat flow per kilogram, I think that I would just say that since there are 250 moles in 1 kg of helium, I could use 250 moles/kg for n instead of 2 in the equation. For work, for the adiabatic processes, there equation is n*Cv*change in temperature, so again, I could just use 250 moles/kg instead of 2 moles (i think). But for the isobaric processes, workk is equal to P*V. I don't know how to incorporate the 250 moles/kg in order to get J/kg in the answer. Any thought?
 
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also...in a brayton cycle, will the net work and the total change in heat flow, Q, be equal for one complete cycle?
 



To solve this problem, you need to first calculate the specific heat capacity (Cp) and specific volume (V) of helium at the given temperatures. Once you have those values, you can use the equations you mentioned to calculate the heat flow and work for each process.

For the isobaric processes, you can use the same equation for work (P*V), but instead of using the number of moles, you can use the specific volume (V) to get the work per kilogram of helium.

For example, for the first isobaric process, you would use the equation W = P*V = 100 kPa * V (specific volume at the given temperature). Then, to get the work per kilogram, you would divide this value by the mass of one kilogram of helium (250 moles * molar mass of helium).

Similarly, for the adiabatic processes, you would use the equation for work (n*Cv*change in temperature), but instead of using the number of moles, you would use the specific heat capacity (Cv) to get the work per kilogram.

Once you have calculated the work and heat flow per kilogram for each process, you can add them together to get the total work and heat flow for the entire cycle.

I hope this helps. Good luck with your thermodynamics problems!
 

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