First Law of Thermodynamics - Piston

In summary: I get confused sometimes.In summary, a cylinder of cross-sectional Area A is closed by a massless piston. The cylinder contains n mol of ideal gas with specific heat ratio and is initially in equilibrium with the surrounding air at temperature T and pressure P. The piston is initially at height h1 above the bottom of the cylinder. Sand is gradually sprinkled onto the piston until it has moved downward to a final height h2. Find the total mass of the sand if the process is isothermal.
  • #1
rpthomps
182
19
A cylinder of cross-sectional Area A is closed by a massless piston. The cylinder contains n mol of ideal gas with specific heat ratio and is initially in equilibrium with the surrounding air at temperature T and pressure P. The piston is initially at height h1 above the bottom of the cylinder. Sand is gradually sprinkled onto the piston until it has moved downward to a final height h2. Find the total mass of the sand if the process is isothermal

Homework Equations



W=PV

W=mgh

The Attempt at a Solution



##\Delta U=\Delta Q-W\\\\##But the system is isothermal therefore##\Delta U= 0\\\\\Delta Q =W##The Work is being done by gravity ##mg\Delta h=PV\\\\mg(h_2-h_1)=PA(h_2)\\\\m=\frac{PA(h_2)}{(h_2-h_1)g}##Answer in text is##M=\frac{PA}{g}(\frac{h_1}{h_2}-1)##
 
Physics news on Phys.org
  • #2
This is not a 1st law problem. This is an ideal gas law problem.
 
  • #3
Isothermal ≠ adiabatic.
 
  • #4
Sturk200 said:
Isothermal ≠ adiabatic.

Yes, I agree. I thought I had kept that concept in mind in my solution above. Is this not the case?

Thanks again for looking.
 
  • #5
rpthomps said:
Yes, I agree. I thought I had kept that concept in mind in my solution above. Is this not the case?

Thanks again for looking.
No. Your analysis is incorrect. It doesn't even determine the work correctly. Furthermore, the work is irrelevant to the solution of this problem.

What is the initial pressure and the initial volume? What is the final volume? From the ideal gas law, what is the final pressure? Considering the weight of the sand and the initial pressure, what is the final pressure? What do you get if you set your two relationships for the final pressure equal to one another?
 
  • Like
Likes rpthomps
  • #6
rpthomps said:
Yes, I agree. I thought I had kept that concept in mind in my solution above. Is this not the case?

Not quite. Isothermal means that temperature is held constant, whereas adiabatic means that no heat (thermal energy) is exchanged. (Remember that U stands for thermal energy.) If you look at the etymology, adiabatic means literally "not go through," so it refers to some physically intrinsic thing (energy) that is not being allowed to pass a barrier. Isothermal just means "equal temperature" -- no mention of a barrier. Thus energy is allowed to be exchanged in an isothermal process, and indeed the exchange of energy during such a process is often precisely the thing that allows the system to be kept at the same temperature throughout.
 
  • Like
Likes rpthomps
  • #7
Okay..I will look at the problem again but before I do, doesn't the statement ##\Delta U=0## mean that the gas doesn't increase its temperature and that by making ##\Delta Q## not 0 that I am allowing for the possibility of an adiabatic transfer of energy?

Again, thanks for spending your time on this.
 
  • #8
rpthomps said:
Okay..I will look at the problem again but before I do, doesn't the statement ΔU=0\Delta U=0 mean that the gas doesn't increase its temperature and that by making ΔQ\Delta Q not 0 that I am allowing for the possibility of an adiabatic transfer of energy?

Nope, setting U=0 means that you are not allowing any heat energy to enter or leave the system. Under this assumption, if we add mechanical work to the system, for instance, then Q would have to go up and thus the temperature would have to increase. If, on the other hand, we had allowed U to be nonzero, then the input of mechanical work may have been counterbalanced by an output of heat energy, thus allowing the overall Q (and thus temperature) to remain constant.
 
  • #9
Sturk200 said:
Nope, setting U=0 means that you are not allowing any heat energy to enter or leave the system. Under this assumption, if we add mechanical work to the system, for instance, then Q would have to go up and thus the temperature would have to increase. If, on the other hand, we had allowed U to be nonzero, then the input of mechanical work may have been counterbalanced by an output of heat energy, thus allowing the overall Q (and thus temperature) to remain constant.
This is totally incorrect. For an ideal gas, if ΔU = 0, the temperature is constant. Q = 0 (not ΔU=0) means that you are not allowing any heat energy to enter or leave the system. So, I agree with post #7. Not that this has anything to do with the solution of this problem, which is strictly an ideal gas law application.

Chet
 
  • #10
Chestermiller said:
This is totally incorrect. For an ideal gas, if ΔU = 0, the temperature is constant. Q = 0 (not ΔU=0) means that you are not allowing any heat energy to enter or leave the system. So, I agree with post #7. Not that this has anything to do with the solution of this problem, which is strictly an ideal gas law application.

Woah, yes that's completely right. Sorry. The book I use has a plus sign convention for W and I think that threw me off.
 
  • #11
rpthomps: Are you unable to answer the leading questions I asked you in post #5?

Chet
 
  • #12
Hey Chet: Still working on it. :) I usually have to think quite a bit about this stuff. What I lack in natural talent though, I gain in perseverance.
 
  • #13
rpthomps said:
Okay..I will look at the problem again but before I do, doesn't the statement ##\Delta U=0## mean that the gas doesn't increase its temperature

For an ideal gas, ##\Delta U=0## means the temperature is constant.

and that by making ##\Delta Q## not 0 that I am allowing for the possibility of an adiabatic transfer of energy?

##\Delta Q=0## means the process is adiabatic. Making ##\Delta Q## nonzero means there is a transfer of heat energy.
 
  • #14
USEFUL EQUATIONS:
##P_iV_i=nRT\\\\P_fV_f=nRT\\\\V_i=h_1A\\\\V_f=h_2A\\\\##

ATTEMPT AT A SOLUTION:

through substation and elimination##P_f=P_i\frac{h_1}{h_2}##At h2 mass of sand is in static equilibrium with the pressure of the gas, using Newton’s equations:##P_fA=mg\\\\P_f=\frac{mg}{A}\\##More substitutions:##m=\frac{P_ih_1A}{gh_2}##Which is different then the book still. Not sure, how they got the difference in values, that’s why I was thinking work originally.
 
  • #15
Your answer for Pf in terms of mg is incorrect. You left something out. What is it that you think you might have omitted from the equation?

Chet
 
  • Like
Likes rpthomps
  • #16
rpthomps said:
##P_f=P_i\frac{h_1}{h_2}##

Right. This follows from Boyle's Law.

At h2 mass of sand is in static equilibrium with the pressure of the gas, using Newton’s equations:

##P_fA=mg\\\\P_f=\frac{mg}{A}\\##

I made this same mistake when I first did it in my head. I had to write it out before I realized that ##\frac{mg}{A}## is the pressure increase (caused by the sand).
 
  • Like
Likes rpthomps
  • #17
Mister T said:
I made this same mistake when I first did it in my head. I had to write it out before I realized that ##\frac{mg}{A}## is the pressure increase (caused by the sand).
Don't you think it would have been better for rpthomps if he had been given the opportunity to deduce this himself?
 
  • Like
Likes rpthomps
  • #18
Chestermiller said:
Your answer for Pf in terms of mg is incorrect. You left something out. What is it that you think you might have omitted from the equation?

Chet

Is there some kind of normal force that is present before the sand is on? This would be equivalent to ##P_i\times A## The sand adds mg to this downward force which is balanced by ##P_f\times A##. Solving for m gives me the expression at the back of the text. I have a real difficulty seeing this. I just assumed the weight of the sand was equivalent to the pressure of the gas. Thanks again for all your help!
 
  • #19
rpthomps said:
Is there some kind of normal force that is present before the sand is on? This would be equivalent to ##P_i\times A## The sand adds mg to this downward force which is balanced by ##P_f\times A##. Solving for m gives me the expression at the back of the text. I have a real difficulty seeing this. I just assumed the weight of the sand was equivalent to the pressure of the gas. Thanks again for all your help!
The words "initially in equilibrium with the surrounding air at temperature T and pressure P" in the problem statement means that the piston is initially in force equilibrium. Do a force balance on the piston before the sand is added, starting with a free body diagram. What are the forces acting on the massless piston initially? What is the force balance equation on the massless piston initially?

Chet
 
  • Like
Likes rpthomps
  • #20
Oh, it is the pressure of the air above it! :) Thank you so much sir!
 
  • Like
Likes Chestermiller

1. What is the First Law of Thermodynamics?

The First Law of Thermodynamics is a fundamental principle in physics that states that energy can neither be created nor destroyed, only transferred or transformed from one form to another.

2. How does the First Law of Thermodynamics apply to a piston?

In the context of a piston, the First Law of Thermodynamics explains that the energy inside the piston (in the form of heat or work) can be transferred to or from the surroundings, but the total energy of the system remains constant.

3. What is the role of a piston in the First Law of Thermodynamics?

A piston is a component of a system that allows for the transfer of energy in the form of heat or work. It is often used in engines and other mechanical systems to convert energy from one form to another, while following the principles of the First Law of Thermodynamics.

4. Can the First Law of Thermodynamics be violated?

No, the First Law of Thermodynamics is a fundamental law of nature and cannot be violated. It is a physical principle that has been observed and tested in numerous experiments.

5. How is the First Law of Thermodynamics related to the conservation of energy?

The First Law of Thermodynamics is directly related to the conservation of energy, as it states that energy can neither be created nor destroyed. This principle is at the core of the conservation laws in physics, which state that certain quantities (such as energy, mass, and momentum) remain constant in a closed system.

Similar threads

  • Introductory Physics Homework Help
Replies
6
Views
1K
  • Introductory Physics Homework Help
Replies
8
Views
743
  • Introductory Physics Homework Help
Replies
5
Views
1K
  • Introductory Physics Homework Help
Replies
8
Views
936
  • Introductory Physics Homework Help
Replies
1
Views
185
  • Introductory Physics Homework Help
Replies
1
Views
417
  • Introductory Physics Homework Help
Replies
1
Views
895
  • Introductory Physics Homework Help
Replies
3
Views
122
  • Introductory Physics Homework Help
Replies
14
Views
2K
  • Introductory Physics Homework Help
Replies
6
Views
1K
Back
Top