Thermodynamics: PV diagram: High temperature adiabat

In summary, the conversation discusses the relationship between temperature and the steepness of an adiabat, as well as the constant in the PV relations and the effect of temperature on the degrees of freedom for a multi-atom molecule. The adiabat is shown to be steeper than the isotherm, and as temperature increases, the degrees of freedom for a multi-atom molecule may also increase, leading to a steeper adiabat. However, this is not always the case as the number of degrees of freedom is limited by geometry. The maximum total degrees of freedom possible is 3N, where N is the number of atoms comprising the molecule. The conversation also mentions that the adiabatic condition assumes an ideal
  • #1
msavg
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0
1. The problem statement, all variables and given/known

Hi, this is my first post on here.

Does an adiabat get steeper at higher temperatures? I think it does, but I wanted to make sure I'm thinking about it in the right way. Also, what is the constant in the PV relations?

Homework Equations



PV=const, for constant temperature.

PVγ=const, for zero heat transfer.

γ=(f+2)/f, where f=degrees of freedom.

The Attempt at a Solution



Using the equations for total thermal energy, the first law, and the ideal gas law, we can derive relationships between pressure and volume that show us what the PV diagram will look like. Since an isotherm comes from
PV=const
and an adiabat comes from
PVγ=const, where γ=(f+2)/f,
we can readily see that the adiabat will be steeper than the isotherm.

However, as temperatue increases, so do the degrees of freedom for a multi-atom molecule. As degrees of freedom increase, so too does the exponent on the V for the adiabatic case. This would lead to a steeper adiabat for non-monatomic molecules at higher temperatures. Furthermore, because the maximum total degrees of freedom possible=3N, where N=number of atoms comprising the molecule, our adiabat would get steeper and steeper for larger and larger molecules at higher temperatures.

Is that correct?

As for the constant, I've looked all over my textbook, but it doesn't describe it at all. Is it some kind of characteristic constant dependent on the kind of gas we're talking about? Are the constants in the isothermal case and adiabatic case the same?
 
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  • #2
msavg said:
Using the equations for total thermal energy, the first law, and the ideal gas law, we can derive relationships between pressure and volume that show us what the PV diagram will look like. Since an isotherm comes from
PV=const
and an adiabat comes from
PVγ=const, where γ=(f+2)/f,
we can readily see that the adiabat will be steeper than the isotherm.
What do you mean by "steeper"? Is this a P-V diagram (P on the vertical axis, V on the horizontal)? What part of the curve are you talking about?
However, as temperature increases, so do the degrees of freedom for a multi-atom molecule.
This is not necessarily true. It depends on the temperature. The number of degrees of freedom are limited by geometry. So when all modes are activated, there is no increase in the number of degrees of freedom with further temperature increases.

Furthermore, because the maximum total degrees of freedom possible=3N, where N=number of atoms comprising the molecule, our adiabat would get steeper and steeper for larger and larger molecules at higher temperatures.

Is that correct?
The adiabatic condition assumes an ideal gas obeying PV=nRT. As you increase the number of atoms in the molecule, the atoms tend to lose their ideal gas behaviour.

AM
 

Related to Thermodynamics: PV diagram: High temperature adiabat

1. What is a PV diagram?

A PV diagram, also known as a pressure-volume diagram, is a graphical representation of the relationship between pressure and volume in a thermodynamic system. It is a useful tool for visualizing and analyzing the changes in pressure and volume during a process.

2. What is meant by "high temperature adiabat" on a PV diagram?

A high temperature adiabat is a line on a PV diagram that represents a process where the temperature of the system remains constant (adiabatic) while the temperature is kept at a high level. This can be achieved by insulating the system from its surroundings to prevent any heat exchange.

3. How is the slope of a high temperature adiabat related to the system's internal energy?

The slope of a high temperature adiabat on a PV diagram is directly related to the system's internal energy. The steeper the slope, the higher the internal energy of the system. This is because the slope represents the rate at which the system is able to do work, and a higher internal energy means the system has more energy available to do work.

4. Can a high temperature adiabat intersect with a low temperature adiabat on a PV diagram?

No, a high temperature adiabat and a low temperature adiabat cannot intersect on a PV diagram. This is because the temperature of the system must remain constant along an adiabat, and if two adiabats were to intersect, it would mean that the temperature of the system is both high and low at the same time, which is not possible.

5. What information can be determined from a PV diagram of a high temperature adiabat?

A PV diagram of a high temperature adiabat can provide information about the changes in pressure, volume, and internal energy of a system during a process where the temperature is kept constant and at a high level. It can also be used to calculate the work done by the system and the heat exchanged during the process.

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