Another contradiction in thermodynamics?

[Amin2014]

Consider an ideal gas operating in a quasi-static (very slow) cycle that is identical to the heat engine version of the carnot cycle in every aspect, except that friction is present. So even though the cycle is quasi-static, it is irreversible due to friction.

Now the question is: How does the efficiency of this quasi-static cycle compare to ideal carnot efficiency? Let η_rev be the efficiency of the carnot cycle and η_irrev be the efficiency of the quasi-static cycle:
Is η_irrev=η_rev?

 

[mfb]

Its efficiency is worse. You convert mechanical work to heat with a 1:1 ratio instead of the thermodynamic optimum.

 

[Amin2014]

You convert mechanical work to heat with a 1:1 ratio.

I'm guessing you're talking about work lost due to friction, correct?
But how does this affect our equations? Take the adiabatic step for instance. Since the process is quasi-static, we could still use dW=-PdV with p referring to the system's pressure. dq=0 right? It's an ideal gas, so dU=C_vdT. I'm taking the gas confined in the cylinder as my system. Where does friction between piston and cylinder come into the picture? If C_vdT = -PdV, then we're going to get the same PV^gamma= Const equation.

 

[Chestermiller]

I can help you work this out. There are two ways of doing this, but the easiest way is to treat the piston and cylinder as a combined system. Assume that all the "frictional heat" goes into the gas. To get things started, let F be the frictional force acting on the piston by the cylinder wall. Do a free body diagram on the piston, and then write a force balance on the piston. Don't forget the supplemental force you need to apply to the piston to keep the conditions quasistatic. What do you obtain?

Chet

 

[Amin2014]

I can help you work this out. There are two ways of doing this, but the easiest way is to treat the piston and cylinder as a combined system. Assume that all the "frictional heat" goes into the gas. To get things started, let F be the frictional force acting on the piston by the cylinder wall. Do a free body diagram on the piston, and then write a force balance on the piston. Don't forget the supplemental force you need to apply to the piston to keep the conditions quasistatic. What do you obtain?

Chet

Thnx Chet. I attached a diagram with three forces/pressures acting on the piston: internal pressure of the gas P, external pressure P_ext, and f_k due to kinetic friction. I've assumed the gas is undergoing expansion. I'm not sure about the supplemental force that you've mentioned though. I'm also confused about your choice of system.

treat the piston and cylinder as a combined system

Is it gas + piston, with the cylinder as surroundings? or is it piston+ cylinder?

Assume that all the "frictional heat" goes into the gas

Why all of the heat?

And what ratio are we trying to calculate here?

 

[Chestermiller]

Thnx Chet. I attached a diagram with three forces/pressures acting on the piston: internal pressure of the gas P, external pressure P_ext, and f_k due to kinetic friction. I've assumed the gas is undergoing expansion. I'm not sure about the supplemental force that you've mentioned though. I'm also confused about your choice of system.

Yes. The diagram is correct. I see that you had the cylinder sitting in a bath. I was assuming you were going to be taking the system to be adiabatic when you wrote PV^γ=const.

The "supplemental" force I was referring to is what you called P_ext. So the force balance on the piston is, as you indicated,

$PA - F = P_{ext}A$

Is it gas + piston, with the cylinder as surroundings? or is it piston+ cylinder?

Sorry. I meant to say, treat the gas and piston as a combined system, and adiabatic cylinder as part of the surroundings.

Why all of the heat?
And what ratio are we trying to calculate here?

To do this problem, you have to decide where the frictional heat is going. If it all somehow goes into the surroundings, then the gas experiences exactly the same treatment as in an adiabatic reversible expansion, and your PV^γ is correct. On the other hand, if part or all of the heat goes into the gas, it experiences a different treatment, equivalent to a non-adiabatic reversible expansion. I was assuming that you wanted to consider the case in which all the frictional heat goes into the gas.

Chet

 

[Chestermiller]

Continuing: If we multiply your force balance by dx (the displacement of the piston) we obtain:
$$PdV-\frac{F}{A}dV=P_{ext}dV=dW$$
where dV = Adx and dW is the work done by the system on the surroundings. If you combine this equation with the differential version of the first law and assume that the cylinder is adiabatic, what do you get?

Chet

 

[Amin2014]

Yes. The diagram is correct. I see that you had the cylinder sitting in a bath. I was assuming you were going to be taking the system to be adiabatic when you wrote PV^γ=const.

The "supplemental" force I was referring to is what you called P_ext. So the force balance on the piston is, as you indicated,

$PA - F = P_{ext}A$Sorry. I meant to say, treat the gas and piston as a combined system, and adiabatic cylinder as part of the surroundings.To do this problem, you have to decide where the frictional heat is going. If it all somehow goes into the surroundings, then the gas experiences exactly the same treatment as in an adiabatic reversible expansion, and your PV^γ is correct. On the other hand, if part or all of the heat goes into the gas, it experiences a different treatment, equivalent to a non-adiabatic reversible expansion. I was assuming that you wanted to consider the case in which all the frictional heat goes into the gas.

Chet

So what ratio do you have in mind as efficiency? Are you considering the Work done by P_ext as the numerator? But what if we choose the gas as our system, then it should be work done by the gas (PdV), no?

 

[Amin2014]

Continuing: If we multiply your force balance by dx (the displacement of the piston) we obtain:
$$PdV-\frac{F}{A}dV=P_{ext}dV=dW$$
where dV = Adx and dW is the work done by the system on the surroundings. If you combine this equation with the differential version of the first law and assume that the cylinder is adiabatic, what do you get?

Chet

I understand you're writing the wok-energy theorem for the massless piston.
PdV-P_extdV-f_kdx=dk_pist=0

dU=dW+dq+dW_*= -P_extdV-Fdx

 

[Amin2014]

where F= (P-P_ext)A
Substituting for f yields:
dU= -P_extdV+ (P_extdV-PdV)= -PdV

 

[Chestermiller]

So what ratio do you have in mind as efficiency? Are you considering the Work done by P_ext as the numerator? But what if we choose the gas as our system, then it should be work done by the gas (PdV), no?

Let's not worry about the efficiency yet. If we chose the gas as our system, then, yes, this would be the work. We'll do the problem that way after we do it this way, OK?

 

[Chestermiller]

I understand you're writing the wok-energy theorem for the massless piston.
PdV-P_extdV-f_kdx=dk_pist=0

dU=dW+dq+dW_*= -P_extdV-Fdx

I don't know exactly what you did here, but the result should be with a plus sign in front of the F and it should be P, not P_ext:
$$dU=\frac{F}{A}dV-PdV$$

Now, the next step is to substitute the ideal gas relationships into this.

Chet

 

[Amin2014]

I don't know exactly what you did here, but the result should be with a plus sign in front of the F and it should be P, not P_ext:
$$dU=\frac{F}{A}dV-PdV$$

Now, the next step is to substitute the ideal gas relationships into this.

Chet

my equation is dU= -P_extdV - Fdx. The first term on the right side of my equation equals the entire right side of your equation, i.e. -P_extdV= F/AdV - PdV.
The difference between my equation and yours is that I have added the term -Fdx, which is the work done by the cylinder on the piston. Considering that the cylinder is part of the surroundings and the piston is part of the system, therefore the force of friction, F, is external to our system, and since its point of application is moving, we must include a term for its work.

I added -Fdx because I believe it's part of the boundary work for our choice of system.

 

[Amin2014]

dW is the work done by the system on the surroundings

Remember that our system is working against TWO forces, not one. dW = P_extdV is only PART of the the work done by the system on its surroundings. The other half is done against friction.

 

[Chestermiller]

my equation is dU= -P_extdV - Fdx. The first term on the right side of my equation equals the entire right side of your equation, i.e. -P_extdV= F/AdV - PdV.
The difference between my equation and yours is that I have added the term -Fdx, which is the work done by the cylinder on the piston. Considering that the cylinder is part of the surroundings and the piston is part of the system, therefore the force of friction, F, is external to our system, and since its point of application is moving, we must include a term for its work.

I added -Fdx because I believe it's part of the boundary work for our choice of system.

How many times do you want to include it? We already included it once.

The cylinder is stationary, so our system does no work on the cylinder. The cylinder is considered part of the surroundings, so our system does no work on that part of the surroundings.

Chet

 

[Chestermiller]

Remember that our system is working against TWO forces, not one. dW = P_extdV is only PART of the the work done by the system on its surroundings. The other half is done against friction.

No, P_extdV is all the work done by our system on its surroundings.

 

[Amin2014]

No, P_extdV is all the work done by our system on its surroundings.

You are right, the piston does no work on the cylinder as the cylinder isn't moving. So P_extdV is the only work done BY the system ON the surroundings. So I made a mistake here. But I don't think you should use the engineering convention of the first law of thermodynamics here. Start with dU=dW +dq, where dW is the work done by the surroundings on the system. This I believe is a generalization of conservation of mechanical energy, and is consistent with the conventions used there.

 

[Amin2014]

In other words, in this particular problem, the work done on the surroundings by the system is not equal to the negative of the work done on the system by surroundings, and thus you cannot use dU= dq-dW where dW is the work done by the system as a valid form of the first law.

 

[Chestermiller]

You are right, the piston does no work on the cylinder as the cylinder isn't moving. So P_extdV is the only work done BY the system ON the surroundings. So I made a mistake here. But I don't think you should use the engineering convention of the first law of thermodynamics here. Start with dU=dW +dq, where dW is the work done by the surroundings on the system.

Actually, the version of the first law that I am accustomed to is dU = dq - dW, where dW is the work done by the system on the surroundings. So, from that perspective, what I said was OK.

So, it's a bit paradoxical, huh? But I am confident that I can resolve the paradox for you, so that we are both in agreement. But, for sure, handling the friction effect at the interface between the piston and the cylinder wall is a bit tricky.

I am going to analyze the friction effect fusing a different approach. Are you familiar with viscous fluids and Newtonian viscosity?

Please stay tuned. But right now, my wife an I are going out to dinner. So, see you later.

Chet

 

[Amin2014]

Actually, the version of the first law that I am accustomed to is dU = dq - dW, where dW is the work done by the system on the surroundings. So, from that perspective, what I said was OK.

So, it's a bit paradoxical, huh? But I am confident that I can resolve the paradox for you, so that we are both in agreement. But, for sure, handling the friction effect at the interface between the piston and the cylinder wall is a bit tricky.

I am going to analyze the friction effect fusing a different approach. Are you familiar with viscous fluids and Newtonian viscosity?

Please stay tuned. But right now, my wife an I are going out to dinner. So, see you later.

Chet

Ok take your time thank you and I hope you have a great time.

 

[Amin2014]

Are you familiar with viscous fluids and Newtonian viscosity?

Two solid objects, grinding against each other, no lubrication. What does this have to do with fluid mechanics? There was a time when I appreciated this branch of physics but I definitely need to refresh my memory.

 

[Amin2014]

I think we need to clarify something here. The cylinder wall is adiabatic right? That means no heat can cross the wall. But the rubbing is occurring between the piston and INNER surface of the wall, which means any heat produced will be confined within the cylinder. So even though the cylinder wall is adiabatic, depending on our choice of system, we may or may not have heat flow to the system.

If we choose our system to be just the gas and piston, that means the heat produced from friction will cross the boundary of our system. All of it, since it can't escape the adiabatic cylinder. So we have to account for dq=Fdx as well : dU= dW + dq= -P_extdV +Fdx -Fdx= -P_extdV, where dW= =P_extdV +Fdx.

On the other hand, if we had taken the boundary of our system to include the frictional force, then dq would be zero, and the frictional work would become internal. So in this case our equation would be dU=dW + dq= -P_extdV. Am I correct?

 

[Chestermiller]

I think we need to clarify something here. The cylinder wall is adiabatic right? That means no heat can cross the wall. But the rubbing is occurring between the piston and INNER surface of the wall, which means any heat produced will be confined within the cylinder. So even though the cylinder wall is adiabatic, depending on our choice of system, we may or may not have heat flow to the system.

Yes.

if we had taken the boundary of our system to include the frictional force, then dq would be zero, and the frictional work would become internal. So in this case our equation would be dU=dW + dq= -P_extdV. Am I correct?

Yes. This is the case I was trying to get us to consider. The equations for this were presented in posts #9 and #12:
$$dU=-PdV+\frac{F}{A}dV$$

If we choose our system to be just the gas and piston, that means the heat produced from friction will cross the boundary of our system. All of it, since it can't escape the adiabatic cylinder. So we have to account for dq=Fdx as well : dU= dW + dq= -P_extdV +Fdx -Fdx= -P_extdV, where dW= =P_extdV +Fdx.

No. If were going to do this type of thing then we would choose as the system the gas. The heat generated at the piston interface with the cylinder would flow into the piston, and then into the gas. So the heat flow into the gas would be dq = Fdx. The surroundings in this case (as reckoned by the gas) would be the piston, and the work done by the gas on the piston (its surroundings) would be dW=PdV, where P is the gas pressure (i.e., the pressure at the interface between our system, the gas, and its surroundings). So, in this case, the first law would give us:
$$dU=dq - dW=Fdx-PdV=\frac{F}{A}dV-PdV$$
Note that both methods give us exactly the same result.

Chet

 

[Amin2014]

Thanks Chet, I understand what you are saying, your analyeses and everything. But they aren't quite addressing my own personal source of confusion. For one, the frictional force DOES do work on the moving piston after all. So there has to be some choice of system where this becomes external work. I was thinking we could choose the system as either gas alone (which you analyzed above), or gas + piston, or somehow, gas + piston + friction. That's how I tried to view the problem. As you see, there is still some source of confusion for me; I can't quite "visualize" everything here.

Why can't we just consider the microscopic details of friction as another "unit" and decide to include or exclude it in our system?

 

[Andrew Mason]

Just a comment here: if the friction results in heat flow into the system, the cycle will not be a Carnot cycle. The Carnot cycle operates between two reservoirs each at different temperatures, Th and Tc. The cycle requires all heat flow to occur where the surroundings and the system are infinitesimally close to thermal equilibrium. Heat flow from the hot reservoir at Th occurs with the system at temperature Th. In order to have heat flow from the system to the cold reservoir the system temperature has to change from being infinitesimally close to Th to infinitesimally close to Tc. This change in temperature has to occur, therefore, without any heat flow occurring (adiabatic). If friction causes heat flow into the system during the adiabatic expansion, it ceases to be adiabatic. So it is not a Carnot cycle.

AM

 

[Chestermiller]

Thanks Chet, I understand what you are saying, your analyeses and everything. But they aren't quite addressing my own personal source of confusion. For one, the frictional force DOES do work on the moving piston after all. So there has to be some choice of system where this becomes external work. I was thinking we could choose the system as either gas alone (which you analyzed above), or gas + piston, or somehow, gas + piston + friction. That's how I tried to view the problem. As you see, there is still some source of confusion for me; I can't quite "visualize" everything here.

Why can't we just consider the microscopic details of friction as another "unit" and decide to include or exclude it in our system?

OK. Let's consider the microscopic gap between the piston and the cylinder as an additional "unit" in the picture. The outer surface of this unit is stationary, since it is the inner surface of the cylinder. The inner surface of this unit is moving with the velocity of the piston. The unit has negligible mass, so there are no changes in its internal energy. From the frame of reference of the laboratory, since the outer surface is not moving, no work is done by the "unit" on the cylinder at this surface; but the inner surface is moving, and the work done by the unit on the piston at this surface is -Fdx. If we apply the first law to this "unit," we obtain:

$-dq=-Fdx$

where dq is the heat flow into the piston from the unit at the piston interface with the "unit" (there is no heat flow at the cylinder surface of the unit).

Now, we can either include the "unit" as part of our gas/piston system as a third element, or we can omit it from our gas/piston system. I think that the case you are interested in is if we don't include it as a third element. If we do this, then the work done by the gas/piston system on its surroundings is:

$P_{ext}dV+Fdx$

where Fdx is the work done on the "unit" (which is now outside our system). There is also heat transfer into the gas/piston system from the unit. So, with this choice of system,

$dW=P_{ext}dV+Fdx=PdV-Fdx+Fdx=PdV$

$dq = Fdx$

And so, from the first law, $dU=Fdx-PdV$

If we were to include the "unit" as part of our system, then no work is done at the cylinder surface by this system, since the cylinder is stationary. And no heat enters this system from the surroundings, because the cylinder is insulated. So, for this choice of the system, we have

$dW = P_{ext}dV$

$dq = 0$

And so, from the first law, $dU=-P_{ext}dV = - PdV + Fdx$

So we get the same answer either way.Chet

 

[Amin2014]

if the friction results in heat flow into the system, the cycle will not be a Carnot cycle.

Yes thankyou. I never implied the cycle is carnot. If friction exists, the cycle is not carnot, period. Friction causes irreversibility, while the carnot is defined to be a reversible cycle between two (constant temperature) reservoirs.

In other words, reversibility is embedded in the definition of carnot cycle; there's' no such thing as an irreverible carnot.

 

[Amin2014]

OK. Let's consider the microscopic gap between the piston and the cylinder as an additional "unit" in the picture. The outer surface of this unit is stationary, since it is the inner surface of the cylinder. The inner surface of this unit is moving with the velocity of the piston. The unit has negligible mass, so there are no changes in its internal energy. From the frame of reference of the laboratory, since the outer surface is not moving, no work is done by the "unit" on the cylinder at this surface; but the inner surface is moving, and the work done by the unit on the piston at this surface is -Fdx. If we apply the first law to this "unit," we obtain:

$-dq=-Fdx$

where dq is the heat flow into the piston from the unit at the piston interface with the "unit" (there is no heat flow at the cylinder surface of the unit).

Now, we can either include the "unit" as part of our gas/piston system as a third element, or we can omit it from our gas/piston system. I think that the case you are interested in is if we don't include it as a third element. If we do this, then the work done by the gas/piston system on its surroundings is:

$P_{ext}dV+Fdx$

where Fdx is the work done on the "unit" (which is now outside our system). There is also heat transfer into the gas/piston system from the unit. So, with this choice of system,

$dW=P_{ext}dV+Fdx=PdV-Fdx+Fdx=PdV$

$dq = Fdx$

And so, from the first law, $dU=Fdx-PdV$

If we were to include the "unit" as part of our system, then no work is done at the cylinder surface by this system, since the cylinder is stationary. And no heat enters this system from the surroundings, because the cylinder is insulated. So, for this choice of the system, we have

$dW = P_{ext}dV$

$dq = 0$

And so, from the first law, $dU=-P_{ext}dV = - PdV + Fdx$

So we get the same answer either way.Chet

This is an awesome analysis Chet! And I'm glad that we're both saying the same thing (I had come to dU= -P_extdV in each case as well). A few things come to mind though: First of all, If we take the "unit" as our system, I believe the fist law leads to dq= -Fdx, which means that the heat is flowing out of this unit (into the gas))
Secondly, in order to clarify the problem further more, we should state that the piston itself is also adiabatic, so no heat can flow into the piston, which means all the heat created will flow directly into the gas. In this case, dq for gas is the negative of dq= -Fdx calculated above.
Again thanks for your patience and depth of analysis.

 

[Amin2014]

If we apply the first law to this "unit," we obtain:

$-dq=-Fdx$

where dq is the heat flow into the piston from the unit at the piston interface with the "unit" (there is no heat flow at the cylinder surface of the unit).
Chet

This is also correct since you are taking dq as heat flowing OUT of the "unit".

 

[Andrew Mason]

Yes thankyou. I never implied the cycle is carnot. If friction exists, the cycle is not carnot, period. Friction causes irreversibility, while the carnot is defined to be a reversible cycle between two (constant temperature) reservoirs.

In other words, reversibility is embedded in the definition of carnot cycle; there's' no such thing as an irreverible carnot.

You can have a Carnot cycle with friction. It is just that you can't have the friction causing heat flow into the system.

The reversibility of the Carnot cycle relates to the thermodynamic cycle. It does not depend on how the work output of the engine is used.

AM