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We know that dQ=nCdT. Since the amount of heat exchanged and temperature are both state functions and depend only on the process, we can also say that ΔQ=nCΔT. Thus
C=n1ΔTΔQ=0.51227−2715000−0=150J/K
If the gas undergoes the process PVx=k, then heat capacity for the process is given by
Easy Math Editor
This discussion board is a place to discuss our Daily Challenges and the math and science related to those challenges. Explanations are more than just a solution — they should explain the steps and thinking strategies that you used to obtain the solution. Comments should further the discussion of math and science.
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to ensure proper formatting.2 \times 3
2^{34}
a_{i-1}
\frac{2}{3}
\sqrt{2}
\sum_{i=1}^3
\sin \theta
\boxed{123}
Comments
We know that dQ=nCdT. Since the amount of heat exchanged and temperature are both state functions and depend only on the process, we can also say that ΔQ=nCΔT. Thus
C=n1ΔTΔQ=0.51227−2715000−0=150J/K
If the gas undergoes the process PVx=k, then heat capacity for the process is given by
C=R(γ−11+1−x1)
For TVn=k, we have PVn+1=k and thus
150=R(35−11+−n1)⟹n1=23−R150
What is the unit of heat supplied?
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Yes, you are right R=325 which yields correct result. Thanks :)
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@Tapas Mazumdar But a doubt still persists, that when the process is coming out to be in the form of PVx=k isn't it adiabatic?
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Source: Wikipedia
As you can see from the above table only when x=γ, the process is adiabatic. In general any process of this from is a polytropic process*.
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