• No results found

) and mass of each particle is m. We make an extremely small

N/A
N/A
Protected

Academic year: 2021

Share ") and mass of each particle is m. We make an extremely small"

Copied!
5
0
0

Loading.... (view fulltext now)

Full text

(1)

Prov i fysik, Thermodynamics, 2012-01-16, kl 9.00-15.00

Hjälpmedel: Students may use any book including the textbook “Thermal physics”. Students may not use their lecture notes.

Present your solutions in details: it will help you getting better evaluation. Good luck!

1) A container of volume V is filled with gas of temperature T, total number of particles is N (initial value is N0) and mass of each particle is m. We make an extremely small

hole of area A in the container, and the gas starts slowly leaking out due to random collisions of gas particles with the wall. How does number of gas particles in the container decrease with time? Hint: Find, how many particles dN pass through the hole in a time interval dt. Derive a differential equation for dN/dt, which also contains N. Solve the equation. For simplicity, you can evaluate the average thermal velocity in one

direction vx as vx vx2 1/2. (4p)

2) Consider two interacting Einstein solids with different numbers of oscillators N

NA 2 and NB N . We have q energy quants in the system. In the limit of low-temperature solids, q NA, q NB, find how multiplicity of the system depends on the number of quants in the solid A, qA. Find the most probable value for qA. OBS! To save time, you may use the formula for multiplicity of cold Einstein solid, which we derived during problem solving, Problem 2.17. (4p)

3) Imaging certain material with heat capacity described by the formula 3

aT

CV , where a is some constant. Find how entropy of this material depends on energy U. (4p)

(2)

4) Consider an engine cycle consisting of three steps: 1) isothermal compression from V1

to V2; 2) expansion at constant pressure; 3) adiabatic expansion to the initial state. Find

efficiency of such an engine as the ratio of work to the total heat input into the system. Assume that working gas is two-atomic with “frozen” oscillation degrees of freedom.

(4p)

5) Consider the Dieterici equation of state kTV aN NkT bN V P( ) exp ,

where a and b are some numerical factors. Find volume, pressure and temperature in the

(3)

Prov i fysik, Thermodynamics 2012-04-13

Hjälpmedel: Students can use any book including the textbook “Thermal physics”. Students may not use their lecture notes.

Define your notations properly. Present arguments in details. Good luck!

1) Thermal conduction in plasma is determined mostly by random thermal motion of electrons. An electron “collides” with an ion, if the ion happens to be on the way of the electron in the imaginary cylinder , where is the electron free path and is the cross-sectional area of the collisions. The cross-sectional area depends on the average thermal velocity of electrons as 4

v . Find how the coefficient of thermal conduction in plasma depends on electron temperature. Electrons may be treated as a mono-atomic

ideal gas. (4p)

2) Consider a simple one-dimensional model of a polymer molecule, which consists of N links (N 1), each link of length d. Every link may “look” to the left or to the right with equal probability as shown on the figure. What is the multiplicity of the macrostate when NR links point to the right? What is the maximal multiplicity? What is the width of the multiplicity function? Using the width of the multiplicity function find the

characteristic size of a molecule L. (4p)

Fig. 1. The model of a polymer molecule. d

(4)

3) Heat capacity of ultra-relativistic degenerate electron gas at constant volume may be written as CV N V T 3 / 1 3 /

2 , where is a constant. Find how entropy of the gas depends

on energy. (4p)

4) Consider an engine cycle consisting of three steps: 1) compression at constant pressure from V1 to V2; 2) pressure increase at constant volume; 3) adiabatic expansion to the

initial state. Find efficiency of such an engine as the ratio of work to the total heat input into the system. Assume that working gas is two-atomic with “frozen” oscillation degrees

of freedom. (4p)

5) Consider equilibrium between two phases. Suppose that the volumes of the phases depend on temperature as V1 V0(1 1T) and V2 V0(1 2T), while entropy

difference depends on temperature as 3

T

S (here V0, , 1 and 2 are constants).

Find the shape of the phase-boundary curve, taking into account that at low temperatures

0

T the phase transition happens at pressure P P0 (Such a problem describes qualitatively phase transition between two solids at low temperatures). (4p)

(5)

Prov i fysik, Thermodynamics, 2011-01-10, kl 9.00-15.00

Hjälpmedel: Students may use any book including the textbook “Thermal physics”. Students may not use their lecture notes.

Define the notations you are using properly. Present your arguments in details: it will help you getting better evaluation. Good luck!

1) Rain-drops are falling at the window with velocity v (the same for all drops) at an angle to the vertical. Average mass of a drop is M, concentration of drops in the air is

n. Drops stick to the window when hitting it. Find pressure of the rain at the window. (4p)

2) Consider equal amounts of helium and argon NH NA N . Initially both gases have different volumes VH V0, VA 3V0 and different temperatures TH 2T0, TA T0. We

put the gases into thermal and mechanical contact (by allowing heat exchange through the wall between the gases and by letting the wall move). Find total entropy increase in the system. OBS! There is no diffusion interaction! (4p)

3) Find chemical potential of a cold Einstein solid. You have to start with the general formula for multiplicity of an Einstein solid. (3p)

What is Gibbs free energy for the solid? (1p)

4) Consider an engine cycle consisting of three steps: 1) adiabatic compression from V1 to V2; 2) isothermal expansion to V3 with V3 V1; 3) compression at constant pressure to

the initial state. Find efficiency of such an engine. Assume that working gas is two-atomic with “frozen” oscillation degrees of freedom. (4p)

5) Van der Waals gas expands from V1 3Nb to V2 5Nb at constant temperature T and number of particles N . Find change of the Helmholtz free energy F of the gas. Hint: Do not confuse Helmholtz and Gibbs free energies. (4)

References

Related documents

In this PhD thesis new organic NIR materials (both π-conjugated polymers and small molecules) based on α,β-unsubstituted meso-positioning thienyl BODIPY have been

Step 9 – Fill in all the CRN (5 digit) numbers for all classes and labs and press Submit Changes. If you have problems, error messages will

Quality: We measure quality (Q in our formal model) by observing the average number of citations received by a scientist for all the papers he or she published in a given

A third set of processes constituting the ePortfolio is that of the current ‘obligation to documentation’ (Rose, 1999, p. Many areas of life, from work and education to social

Insurance; environment; pollution; environmental insurance; first-party insurance; third-party insurance; first-party insurance for the benefit of a third party; statutory

In humans, PET studies with [ 11 C]raclopride recently confirmed this hypothesis by showing that in cocaine abusers drug cues (cocaine-cue video of scenes of subjects taking

The Rater will discuss with the Ratee the proposed objective, target completion date, the evaluation or measurement criteria by which successful results can be identified, costs,

The threshold into the stadium is through a series of layers which delaminate from the geometry of the field to the geometry of the city and creates zones of separation,