36
Review , Examples and Problems Thermodynamics 221PHYS

Thermodynamic, Examples-A.ppt

  • Upload
    ibb

  • View
    1

  • Download
    0

Embed Size (px)

Citation preview

Review , Examples and

Problems

Thermodynamics221PHYS

HeatHeat

Example-1: An m1 = 485-gram brass block sits in boiling water (T1 = 100 C). It is taken out of the boiling water and placed in a cup containing m2 = 485 grams of ice water (T2 = 0 C). What is the final temperature, TF, of the system (i.e., when the two objects have the same T)? (cbrass = 380 J/kg.K; cwater = 4184 J/kg.K)

a. TF < 50 C b. TF = 50 C c. TF > 50 C Solution:Heat flows from the brass to the water. No work is done, and we assume that no energy is lost to the environment.

Remember: Q = CT = mcTBrass (heat flows out): Q1 = U1 = m1c1(TF-T1) Water (heat flows in): Q2 = U2 = m2c2(TF-T2)

Energy is conserved: Q1 + Q2 = 0Solve for TF: TF = (m1c1T1+m2c2T2) / (m1c1+m2c2)

= (c1T1+ c2T2) / (c1+ c2) = 8.3 CWe measured TF = _____ C.

QT1m1

T2m2

Kinetic theory Kinetic theory of the ideal of the ideal

gasgas

Example2 : The Speed of Molecules in AirAir is primarily a mixture of nitrogen N2 molecules (molecular mass 28.0 u) and oxygen O2 molecules (molecular mass 32.0 u). Assume that each behaves as an ideal gas and determine the rms speeds of the nitrogen and oxygen molecules when the temperature of the air is 293K.

Solution

For Nitrogen…

Example 3: A container of an ideal gas has a moveable top. The top has an area of 0.01 m2 and is 50 cm above the bottom of the cylinder. A mass of 200 kg is placed on the container, which compresses the gas by 20 cm. The gas in the container is initially at atmospheric pressure (1.01 x 105 Pa) and 20oC. What is the new temperature of the gas?

nRTPV nRTPV

2

22

1

11

TVP

TVP

Solution

1 2

1 1 2 2

V Ah and A AV Ah and V Ah

15.27311 cTT K15.293

1 0 101P P kPa

AFPP 02

AmgPP 02 kPa2.297

The following relations have been used

11

1222 VP

TVPT K6.51710

122

AhPTAhP

10

122

hPThP

CT 2442

The new temperature

Thermodynamic Thermodynamic lawslaws

Ex.4 : The process shown on the Pressure-Volume diagram is an

(A) adiabatic expansion.

(B) isothermal expansion.

(C) isometric expansion.

(D) isobaric expansion.

P

Vo

Ex.5: In an isochoric process, there is no change in

(A) pressure.

(B) temperature.

(C) volume.

(D) internal energy.

Ex-6: The process shown on the Temperature-Volume graph is an

(A) adiabatic compression.

(B) isothermal compression.

(C) isochoric compression.

(D) isobaric compression.

T

Vo

Ex-7: When the first law of thermodynamics, Q = ΔU + W, is applied to an ideal gas that is taken through an isothermal process,

(A) ΔU = 0

(B) W = 0

(C) Q = 0

(D) none of the above

Ex-8: An ideal gas is compressed to one-half its original volume during an isothermal process. The final pressure of the gas

(A) increases to twice its original value.

(B) increases to less than twice its original value.

(C) increases to more than twice its original value.

(D) does not change.

Ex-10: When the first law of thermodynamics, Q = ΔU + W, is applied to an ideal gas that is taken through an adiabatic process,

(A) ΔU = 0.

(B) W = 0.

(C) Q = 0.

(D) none of the above

Ex-11: A gas is taken through the cycle illustrated here. During one cycle, how much work is done by an engine operating on this cycle?

(A) PV

(B) 2PV

(C) 3PV

(D) 4PV

P

2P

V 2V 3V 4V

Ex-12: An ideal gas initially has pressure Po, at volume Vo and absolute temperature To. It then undergoes the following series of processes:

Po

2Po

Vo 2Vo 3Vo

I. Heated, at constant volume to pressure 2Po

II. Heated, at constant pressure to pressure 3Vo

III. Cooled, at constant volume to pressure Po

IV. Cooled, at constant pressure to volume Vo

I

II

III

IV

Po

2Po

Vo 2Vo 3Vo

I

II

III

IV

2To

Find the temperature at each end point in terms of To

nRTPV nR

VPT ooo

To

6To

3To

Po

2Po

Vo 2Vo 3Vo

I

II

III

IV

Find the net work done by the gas in terms of Po and Vo

ooVP2W

Net work equals net area under curve

Po

2Po

Vo 2Vo 3Vo

I

II

III

IV

Find the net change in internal energy in terms of Po and Vo

0U

Ex-13: A sample of gas expands from 1.0 m3 to 4.0 m3 while its pressure decreases from 40 Pa to 10 Pa. How much work is done by the gas if its pressure changes with volume via each of the three paths shown in the Figure below?

Path A: W = +120 JPath B: W =+75 JPath C: W =+30 J

Example-14Example-14

A cylinder of radius 5 cm is kept at pressure with a pistonof mass 75 kg.

a) What is the pressure inside the cylinder?b) If the gas expands such that the cylinder rises 12.0 cm, what work was done by the gas?c) What amount of the work went into changing the gravitational PE of the piston?d) Where did the rest of the work go?

SolutionGiven: M =75, A = π× 0.052, ∆x=0.12, Patm = 1.013x105 Pa

a) Find Pgasatmg as P

AMgP = 1.950x105 Pa

b) Find Wgas VPW

xAPW g a s = 183.8 J

c) Find Wgravity m g hW = 88.3 J

d) Where did the other work go? Compressing the outside air

Example-15 a) What amount of work is performed by the gas in the cycle IAFI?

b) How much heat was inserted into the gas in the cycle IAFI?

c) What amount of work is performed by the gas in the cycle IBFI?

a r e a e n c lo s e dWWIAFI = 3Patm

= 3.04x105 J

WQU U = 0

W = -3.04x105 J

Q = 3.04x105 J

V (m3)

Example-Example-1616Consider a monotonic ideal gas which expands according to the PV diagram.

a) What work was done by the gas from A to B?b) What heat was added to the gas between A and B?c) What work was done by the gas from B to C?d) What heat was added to the gas beween B and C?e) What work was done by the gas from C to A?f) What heat was added to the gas from C to A?

V (m3)

P (kPa)

25

50

75

0.2 0.4 0.6

A

B

C

Solutiona) Find WAB

b) Find QAB

V (m3)

P (kPa)

25

50

75

0.2 0.4 0.6

A

B

C

WAB = Area = 20,000 J

•First find UA and UBMonotonic Gas:

32

32

U nRT

PV nRT

U PV

UA = 22,500 J, UB = 22,500 J, U = 0

•Finally, solve for QU Q W Q = 20,000 J

c) Find WBC

d) Find QBC

V (m3)

P (kPa)

25

50

75

0.2 0.4 0.6

A

B

C

WBC = -Area = -10,000 J

•First find UB and UC

PVU23

UB = 22,500 J, UC = 7,500 J, U = -15,000

•Finally, solve for Q

WQU

Q = -25,000 J

e) Find WCA

f) Find QCA

V (m3)

P (kPa)

25

50

75

0.2 0.4 0.6

A

B

C

WAB = Area = 0 J

•First find UC and UA

UC = 7,500 J, UA = 22,500 J, ∆U = 15,000

•Finally, solve for Q

Q = 15,000 J

g) Net work done by gas in the cycleh) Amount of heat added to gas

WAB + WBC + WCA = 10,000 JQAB + QBC + QCA = 10,000 J

This does NOT mean that the engine is 100% efficient!

Example-17

Imagine that we rapidly compress a sample of air whose initial pressure is 105 Pa and temperature is 220C (= 295 K) to a volume that is a quarter of its original volume (e.g., pumping bike’s tire). What is its final temperature?

2211

222

111

VPVP

TNkVPTNkVP

B

B

1

2

1

2

12

1

1121

2

11

2

112 T

TVVT

TVPTNk

VVP

VVPP B

constVTVT 122

111

For adiabatic processes:

Rapid compression – approx. adiabatic, no time for the energy exchange with the environment due to thermal conductivity

constTP /1also

KKKVVTT 51474.12954295 4.0

1

2

112

Example-18: Finding the Work

An ideal gas with = 1.4 occupies 4.0 L at 300 K & 100 kPa pressure. It’s compressed

adiabatically to ¼ of original volume, then cooled at constant V back to 300 K, & finally

allowed to expand isothermally to its original V. How much work is done on the gas?

1A A B B

ABp V p VW

741 J

AB (adiabatic):

0BCW BC isochoric):

ln ACA

C

VW n R TV

CA (isothermal):

1.4 1100 4.0 1 4

1.4 1

kPa L

AB A

B

Vp pV

1

11

A A AAB

B

p V VWV

ln 4A Ap V 555 J

work done by gas: ABCA AB BC CAW W W W 186 J

Example-19: A thermodynamic system undergoes a process in which its internal energy decreases by 465 J. Over the same time interval, 236 J of work is done on the system. Find the energy transferred from it by heat.

465 236 701U Q WQ U W J J J

Note: Sign convention for Q : Q>0 system gains heat from environment

Example-20:. Diesel Power

Fuel ignites in a diesel engine from the heat of compression (no spark plug needed).

Compression is fast enough to be adiabatic.

If the ignit temperature is 500C, what compression ratio Vmax / Vmin is needed?

Air’s specific heat ratio is = 1.4, & before the compression the air is at 20 C.

1T V const

1 / 1.4 1273 500273 20K KK K

1 / 1

max min

min max

V TV T

11

Ex-21: Two cylinders at the same temperature contain the same gas. If B has twice the volume and half the number of moles as A, how does the pressure in B compare with the pressure in A?(A) PB = 1/2 PA

(B) PB = 2 PA

(C) PB = 1/4 PA

(D) PB = 4 PA

(E) PB = PA

Ex-22: A gas cylinder and piston are covered with heavy insulation. The piston is pushed into the cylinder, compressing the gas. In this process, the gas temperature

A. doesn’t change.B. decreases.C. increases.D. there’s not sufficient information to tell.

Ex-23: During an isothermal process, 5.0 J of heat is removed from an ideal gas. What is the change in internal energy?

A) zero

B) 2.5 J

C) 5.0 J

D) 10 J

The Laws of Thermodynamics

Ex-24: If the gas in a container absorbs 300 J of heat, has 100 J of work done on it, and then does 200 J of work on its surroundings, what is the increase in the internal energy of the gas?

(A) 600 J(B) 400 J(C) 0 J(D) 500 J(E) 200 J