Derive the expression for isothermal change in Constant Volume Heat Capacity

In summary, Isothermal change in constant volume heat capacity is the measure of the amount of heat required to raise the temperature of a substance by one degree Celsius at a constant volume. The expression for this change is derived by considering the first law of thermodynamics, with various assumptions made such as the substance being in a closed system and an ideal gas. It differs from isobaric change, and has practical applications in various industrial and scientific processes, as well as in the study of thermodynamics and heat transfer.
  • #1
eagerbeaver92
3
0

Homework Statement


Derive the following expression for calculating the isothermal change in Constant Volume Heat Capacity:

(dCv/dV)T = T(d2P/dT2)V


Homework Equations





The Attempt at a Solution



I have no idea, please help
 
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  • #2
How about this?

assuming ideal gas:

P=nrt/V

then

(dP/dT) = R/V , ignoring moles

and

(d2P/d2T) = 0

so (dCv/dV)=T*0=0
 
  • #3
.

Sure, I can help you with this problem. The isothermal change in constant volume heat capacity, also known as the isochoric heat capacity, is defined as the change in heat capacity at constant volume with respect to temperature. Mathematically, it can be expressed as:

Cv = (dQ/dT)V

where Cv is the constant volume heat capacity, dQ is the change in heat, and dT is the change in temperature. Now, let's take the derivative of this equation with respect to volume at constant temperature:

(dCv/dV)T = (d/dV)(dQ/dT)V

Using the chain rule, we can rewrite this as:

(dCv/dV)T = (d/dT)(dQ/dV)T * (dT/dV)T

Since we are considering an isothermal process, the change in temperature (dT) is equal to zero. Therefore, the last term becomes zero and we are left with:

(dCv/dV)T = (d/dT)(dQ/dV)T

Now, we can use the Maxwell relation for the change in pressure with respect to temperature at constant volume, which is given by:

(dP/dT)V = (d2Q/dT2)V

Substituting this into our equation, we get:

(dCv/dV)T = (d/dT)(dQ/dV)T = (d/dT)(dP/dT)V = (d2P/dT2)V

And there you have it, we have derived the expression for calculating the isothermal change in constant volume heat capacity. I hope this helps! Let me know if you have any further questions.
 

1. What is the definition of isothermal change in constant volume heat capacity?

Isothermal change in constant volume heat capacity is the measure of the amount of heat required to raise the temperature of a substance by one degree Celsius at a constant volume.

2. How is the expression for isothermal change in constant volume heat capacity derived?

The expression for isothermal change in constant volume heat capacity is derived by considering the first law of thermodynamics, which states that the change in internal energy of a system is equal to the heat added to the system minus the work done by the system. By rearranging this equation and considering the definition of heat capacity, the expression for isothermal change in constant volume heat capacity can be derived.

3. What are the assumptions made when deriving the expression for isothermal change in constant volume heat capacity?

The assumptions made include: the substance is in a closed system, the volume remains constant during the process, the process is reversible, and the substance is an ideal gas.

4. How does isothermal change in constant volume heat capacity differ from isobaric change?

Isothermal change in constant volume heat capacity differs from isobaric change in that isobaric change occurs at a constant pressure, while isothermal change occurs at a constant volume. This means that the work done in an isobaric process is not zero, while the work done in an isothermal process is zero.

5. What are some practical applications of the expression for isothermal change in constant volume heat capacity?

The expression for isothermal change in constant volume heat capacity is used in various industrial and scientific processes, such as in the design of engines and refrigeration systems. It is also used in the study of thermodynamics and heat transfer, and in the determination of the specific heat capacity of substances.

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