Problem set — work and thermodynamic paths
Problem set: work and thermodynamic paths¶
Use the convention throughout, and say so in your working. Take the gas to be ideal and monatomic (, ) unless told otherwise.
Problem 1 — three routes, one destination¶
One mole of gas begins at , and ends at , .
(a) Show that the two states lie on the same isotherm, and find that temperature.
(b) Compute for each of three routes: (i) the isotherm; (ii) expansion at constant followed by cooling at constant ; (iii) cooling at constant followed by expansion at constant .
(c) Compute and for each route. Comment on which quantities came out equal and which did not, and say why that was inevitable before doing any arithmetic.
Problem 2 — a cycle¶
A gas is taken clockwise around the rectangle in the – plane with corners , , , , where and .
(a) Compute the work done on the gas for each of the four legs, and the net work per cycle.
(b) State the net change in internal energy per cycle, and justify it in one sentence without computing anything.
(c) Deduce the net heat absorbed per cycle. Which direction around the loop makes the device an engine rather than a refrigerator?
(d) Show that the magnitude of the net work equals the area enclosed by the rectangle, and explain why the enclosed area — rather than the area under a single curve — is the relevant quantity for a cycle.
Problem 3 — isotherm against adiabat¶
A gas at expands to , once isothermally and once adiabatically.
(a) Sketch both paths on the same axes and state which is steeper, with a physical reason rather than an appeal to the exponent.
(b) Compute for each.
(c) Compute for each, and use the results to explain why the adiabatic expansion ends at a lower temperature.
(d) Which final state has the greater internal energy? Which has the greater entropy? (You may answer the second part qualitatively; module 8 makes it quantitative.)
Problem 4 — the sudden piston¶
A gas at pressure in volume is compressed to by pushing the piston with a constant external pressure , quickly enough that the gas is never in equilibrium during the process.
(a) Compute the work done on the gas.
(b) Explain why the answer is not evaluated along any curve in the – plane, and what would have to be true for it to be.
(c) Compare your answer with the work required to reach the same final volume quasistatically along an adiabat. Which is larger, and where did the extra energy go?
(d) A classmate objects that the gas ends at the same volume either way, so the work must be the same. Diagnose their error precisely.
Problem 5 — exactness by calculation¶
For one mole of ideal gas, write in terms of and .
(a) Apply the cross-derivative test and show explicitly that is inexact.
(b) Repeat the test for and show that it is exact.
(c) Integrate along two different routes between the same endpoints and confirm that you get the same answer. Name the state function you have just constructed.
(d) Explain in words what it means that a quantity becomes a state function only after division by .
Problem 6 — computational¶
Using the module’s laboratory notebook and thermolab.paths:
(a) Construct at least four different paths between the same endpoints, including one you invent yourself, and tabulate , and for each.
(b) Verify numerically that agrees across all of them to machine precision while does not, and quote the fractional spread of the work values.
(c) Compute the isothermal work at increasing sampling resolution and confirm that the error falls as the square of the step size. Report the fitted convergence order.
(d) Explain why the fractional spread in (b) is the meaningful comparison, and what would have gone wrong had you compared the work values with an absolute tolerance instead.