Lectures_12-13

Lectures_12-13 - Part IV Work Lecture 12 PV work Recall the...

Info iconThis preview shows pages 1–3. Sign up to view the full content.

View Full Document Right Arrow Icon
Part IV — Work Lecture 12 — PV work Recall the notion of a thermodynamic process: change of state via some external intervention. Common processes include: Adding or removing heat Expanding or compressing the system Often, the process involves requires or generates work. We say, work is done on the system, or done by the system. Sign convention: work done on the system is positive, work done by the system is negative. (We are keeping track of the energy of the system.) Recall that being able to calculate the required amount of work for a process, and designing a process so that the minimum amount of work is required, or the maximum amount of work is generated, are central goals of thermodynamics. An external force acting through a small displacement does a small amount of work dW = F ext dx = - P ext dV We integrate to Fnd the total work done during the process W = - ± V 2 V 1 P ext dV Sign convention: when we compress the system, dx > 0 (displacement in direction of force applied) and dV < 0. In compressing, we do work on the system, increasing its energy (like compressing a spring). Work is not a state variable — it depends on the path (i.e., the details of the process). ±or example: it is harder to compress a hot gas than a cold one. So consider a process in which we increase T by some amount and decrease V by some amount. If we warm Frst, the work will be greater than if we warm after compressing. (sketch) We will see more speciFc examples of this next lecture. To compute W , we need to know how P ext varies as we do the volume change. If we do the change slowly enough, P ext = P ( V,T ) (the equilibrium system pressure) to a close approximation — nearly balanced forces, very slow motion of the piston. This we call a reversible change — at every point along the way, we are very close to equilibrium. Then, we can compute the work, if we have an EOS to tell us P ( V,T ). In general, if the process is done at a Fnite rate, it won’t be “reversible”. In that case, W = W rev + W lost 30
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full Document Right Arrow Icon
We always have W lost > 0 (This is a postulate , that is consistent with our common experience — and detailed experiment besides. We shall meet other equivalent forms of this assumption in later lectures.) If we are doing work on the system ( W> 0), it takes more work than the minimum W rev to e f ect the change. If the system is doing work ( W< 0), we get less work than the maximum - W rev . Example: we slowly heat an ideal gas conFned by a Fxed external pressure P ext . “Slowly” means P P ext during the process. Because the external pressure is Fxed, the work is simple to com- pute. Pv = RT implies Δ v = R Δ T/P , hence W = - R Δ T . The gas does positive work on the surroundings (pushes in the direction of motion), so the surroundings do negative work on the gas ( W< 0). Example: we slowly expand an ideal gas at constant temperature. Again, “slowly” means we adjust
Background image of page 2
Image of page 3
This is the end of the preview. Sign up to access the rest of the document.

{[ snackBarMessage ]}

Page1 / 5

Lectures_12-13 - Part IV Work Lecture 12 PV work Recall the...

This preview shows document pages 1 - 3. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online