Thermodynamics He expanding volume directly proportional to pressure

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SUMMARY

The discussion focuses on a thermodynamics problem involving helium gas expanding from 1 litre to 3 litres while its pressure increases proportionally to its volume. The work done on the gas is calculated using the equation W = -∫PdV, leading to W = -m*4E-6, where m is a proportionality constant. The change in internal energy is derived from U = (3/2)NkT, and the heat exchange is expressed as Q = -(5/2)W. A simple experimental setup is proposed, involving a horizontally positioned cylinder and a rotating drum to measure work done.

PREREQUISITES
  • Understanding of the ideal gas law (PV = NkT)
  • Familiarity with thermodynamic equations for work (W = -∫PdV) and internal energy (U = Q + W)
  • Knowledge of quasi-static processes in thermodynamics
  • Basic principles of pressure-volume (PV) diagrams
NEXT STEPS
  • Calculate specific values for work done using different proportionality constants (m)
  • Explore the relationship between internal energy and heat exchange in thermodynamic processes
  • Learn about PV diagrams and their applications in visualizing thermodynamic processes
  • Investigate experimental setups for measuring work done in gas expansion
USEFUL FOR

Students and educators in physics and engineering, particularly those studying thermodynamics and gas laws, will benefit from this discussion.

relativespeak
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Homework Statement



Imagine some helium in a cylinder with an initial volume of 1 litre and an initial pressure of 1 atm. Somehow,
the helium is made to expand to a final volume of 3 litres, in such a way that its pressure rises in direct
proportion to its volume.

(b) Calculate the work done on the gas during this process, assuming that the process occurs quasi-statically,
and no other types of work are being done.
(c) Calculate the change in the internal energy of the helium during the process.
(d) Calculate the amount of heat added to or removed from the helium during this process,
(e) What would you have to do to cause the pressure to rise as the helium expands?
(f ) Describe a simple experimental setup in which this form of the expansion would occur, i.e., where the
pressure would rise proportional to the volume of the gas.

Homework Equations



W = -∫PdV
U = Q+W = (f/2)NkT

PV = NkT

The Attempt at a Solution



For the first part I used W = -∫PdV and P=mV where m is some proportionality constant. Then W=-∫mVdV= -(m/2)V^2 which equals -m*4E-6. I'm not sure if this work is correct.

Then for part c, U=(3/2)NkT=(3/2)PV=-(3/2)W (because helium has 3 degrees of freedom) and the heat is given by:
-(3/2)W=Q+W, Q=-(5/2)W. I'm just not sure if this is correct
 
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Your work for (a) looks good. You should be able to determine the numerical value of the constant of proportionality m and thus determine a numerical value for the work. You should specify units in your answers.

For part (c), note that you are asked for the change in U. Also, it is not correct to equate PV with -W.
 
How can I find a numerical value for m without knowing the change in P?

The change in U would then be U=ΔPΔV=mΔVΔV=m(ΔV)^2?
 
What does m have to be so that P = 1 atm when V = 1 litre?
 
relativespeak said:
How can I find a numerical value for m without knowing the change in P?

The change in U would then be U=ΔPΔV=mΔVΔV=m(ΔV)^2?

No. ΔU means Uf - Ui = (3/2)(PV)f - (3/2)(PV)i.
 
The process is easily visualized on a PV diagram. The path followed by the system is shown by a straight line with a positive slope (joining the points (3,3) and (1,1). Taking this line as the hypotenuse complete the right angled triangle The third vertex will be the point (1,3).

The area under the hypotenuse gives the heat supplied to the system. The area of the triangle gives the increase internal energy. the difference between the above two areas gives (the area under the straight line parallel to the volume axis) gives the work done by the system. You will get all areas ( and the corresponding quantities) in terms of liter atm.

(e) heat the gas
(f) keep the cylinder horizontally so that the piston moves horizontally. As it moves the piston rotates a drum over which a thread, to one end of which a mass is attached, is wound. As the drum rotates the weight is lifted, which gives a measure of the work.
 

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