PHY 3513 Fall 1999 Homework 1: Thermodynamics Problems, Assignments of Thermal Physics

The solutions manual for homework 1 of phy 3513 fall 1999, which covers various thermodynamics problems. Students are required to find the heat flow, final equilibrium state, and work done by a gas under different expansion conditions.

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PHY 3513 Fall 1999 Homework 1
Due at the start of class on Friday, September 3.
Answer all questions. To obtain full credit, you must explain your reasoning and show all
working. Please write neatly and include your name on the front page of your answers.
1. For temperatures below about 2 K, the molar heat capacity of argon is well-described by
the formula
cmol =αT3,(1)
where Tis the absolute temperature, and α= 2.5 mJ mol1K4.
Starting from the equation
¯dQ =nc
mol dT,
where nis the number of moles, find the total heat Qflowing into 0.065 mol of argon when
it is first heated from 1.30 K to 1.90 K, then cooled to 0.80 K.
2. Supp ose that 10 g of ice initially at 20 C is dropped into 20g of water initially at 5 C.
Assuming that the combined ice-water system is closed (i.e., no material or heat crosses
its boundaries and no work is done by/on the system), what is the final equilibrium state?
Express your final answer in roughly the same format as the following sample answers (all
of which are physically nonsensical): “30 g of ice at 30 C,” “5 g of ice at 20 Cplus25g
ofwaterat5
C,” and “20 g of water and 20 g of steam, both at 100 C.”
Data: cice = 2220 J kg1K1,cwater = 4190 J kg1K1,csteam = 1520 J kg1K1,
LF= 333 kJ kg1,LV= 2256 kJ kg1.
3. The pressure P, the molar volume v, and the temperature Tof a certain gas are related
by the equation of state
P(vb)+ a
Tv =RT. (2)
Here a,b,andRare positive constants.
Consider nmoles of the gas sealed inside a cylinder with a movable piston. Calculate the
total work done by the gas on expanding from volume V1to V2>V
1when the expansion
is performed in each of four different ways specified by the various constraints specified in
(a)–(d) below.
(a) Isothermal: T=T0, a constant.
(b) Isobaric: P=P0,aconstant.
(c) Isochoric: V=V1=V2.
(d) Arbitrary: T=c(vb), where cis a constant.
Hints: (i) Don’t confuse the volume Vwith the molar volume v=V/n. (ii) There are a
couple of places where it will be useful to use partial fractions to re-express 1/[v(vb)].

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PHY 3513 Fall 1999 – Homework 1

Due at the start of class on Friday, September 3.

Answer all questions. To obtain full credit, you must explain your reasoning and show all working. Please write neatly and include your name on the front page of your answers.

  1. For temperatures below about 2 K, the molar heat capacity of argon is well-described by the formula cmol = α T 3 , (1)

where T is the absolute temperature, and α = 2.5 mJ mol−^1 K−^4.

Starting from the equation dQ¯ = n cmol dT,

where n is the number of moles, find the total heat Q flowing into 0.065 mol of argon when it is first heated from 1.30 K to 1.90 K, then cooled to 0.80 K.

  1. Suppose that 10 g of ice initially at − 20 ◦C is dropped into 20 g of water initially at 5 ◦C. Assuming that the combined ice-water system is closed (i.e., no material or heat crosses its boundaries and no work is done by/on the system), what is the final equilibrium state? Express your final answer in roughly the same format as the following sample answers (all of which are physically nonsensical): “30 g of ice at − 30 ◦C,” “5 g of ice at − 20 ◦C plus 25 g of water at 5 ◦C,” and “20 g of water and 20 g of steam, both at 100 ◦C.”

Data: cice = 2220 J kg−^1 K−^1 , cwater = 4190 J kg−^1 K−^1 , csteam = 1520 J kg−^1 K−^1 , LF = 333 kJ kg−^1 , LV = 2256 kJ kg−^1.

  1. The pressure P , the molar volume v, and the temperature T of a certain gas are related by the equation of state P (v − b) +

a T v

= R T. (2)

Here a, b, and R are positive constants.

Consider n moles of the gas sealed inside a cylinder with a movable piston. Calculate the total work done by the gas on expanding from volume V 1 to V 2 > V 1 when the expansion is performed in each of four different ways specified by the various constraints specified in (a)–(d) below.

(a) Isothermal: T = T 0 , a constant.

(b) Isobaric: P = P 0 , a constant.

(c) Isochoric: V = V 1 = V 2.

(d) Arbitrary: T = c(v − b), where c is a constant.

Hints: (i) Don’t confuse the volume V with the molar volume v = V /n. (ii) There are a couple of places where it will be useful to use partial fractions to re-express 1/[v(v − b)].