Calculating Change in Enthalpy of Constant Volume Process

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In a constant volume process, the change in specific enthalpy can still be calculated using the formula Δh = Cp*Δt, despite Cp being defined for constant pressure processes. Enthalpy is a property of the gas that depends only on temperature and pressure, allowing for its calculation between two equilibrium states. The relationship between enthalpy and heat capacity is established through experimental measurements at constant pressure, which provide the necessary data for enthalpy tables. Thus, while the process is isochoric, the change in external pressure requires energy input, affecting the enthalpy. Understanding these concepts clarifies the applicability of Cp in constant volume scenarios.
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I was asked to find the change in specific enthalpy of constant volume process.

Mass of 10 kg of a gas is heated to a pressure of about 2 times the initial pressure. The initial temperature was 20°C.

The process is a reversible, non-flow, constant volume process.

I found out the final temperature which is 40°C

Change in enthalpy Δh=Cp*Δt

My question is, is it correct to use Cp which is defined for a constant pressure process in a constant volume process?

If it's correct then how it is correct?
 
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How can the gas be compressed if its volume is constant?

Chet
 
Sorry it's is heated not compressed.
 
You need to look at the formal definition of enthalpy on Wikipedia to understand.

At some point you will find the following equation:

c25908f7c6c63ac4b7422cd7d91b2c16.png


The left part is the definition of enthalpy. The first two terms of the right part are the internal energy dU and the third term is the work done.

The second term of the right part is the internal work done (which affects the internal energy and the enthalpy) and the third term could be seen as the total work done (I'm not sure it's the proper terminology).

The thing is that the pdV term is also included in the d(pV) term (= pdV + Vdp). This is why we end up with:

8e15be705c669a27bdd04c2882bf26bc.png


In an isochoric process, TdS is the internal energy because there is no internal work done, but dp is not equal to zero so the enthalpy is still higher than the internal energy.

The way to think of it is, even though there is no volume change, that change in exterior pressure to keep the volume constant requires some energy from an exterior source.
 
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ajayguhan said:
I was asked to find the change in specific enthalpy of constant volume process.

Mass of 10 kg of a gas is heated to a pressure of about 2 times the initial pressure. The initial temperature was 20°C.

The process is a reversible, non-flow, constant volume process.

I found out the final temperature which is 40°C

Change in enthalpy Δh=Cp*Δt

My question is, is it correct to use Cp which is defined for a constant pressure process in a constant volume process?

If it's correct then how it is correct?
There is an important point that, in my opinion, is always omitted, or at least, under-emphasized in thermodynamics texts. Enthalpy represents a physical property of the particular gas, and is not intrinsically related to the characteristics of any particular process. It is a function only of the temperature and pressure of the gas. So, for example, if you tell me the temperature and pressure of a particular gas in two different equilibrium states, I can tell you the change in enthalpy (per unit mass) between these states. All I need to do this is a table of enthalpy (per unit mass) as a function of temperature and pressure. For an ideal gas, things are even simpler. At low pressures, where ideal gas behavior prevails, the enthalpy is a function only of temperature.

So where does this constant pressure business come into play? Well, this is how we experimentally measure the enthalpy values that go into the table (once and for all). By doing an experiment at constant pressure, the change in enthalpy between equilibrium state A and equilibrium state B is equal to the amount of heat we have to add in the process to get from state A to state B. But, once these measurements have been performed, they never have to be performed again.

What we call the heat capacity Cp is simply equal to the partial derivative of the enthalpy with respect to temperature.

Hope this helps.

Chet
 

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