Thermodynamics Flashcards

random things I may need to know

1
Q

difference between heat and temperature?

A

heat: refers to energy transfer caused by dif temps.

temperature: form of measurement. associated with the sense of touch and related to kinetic energies of the molecules in the material.

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2
Q

0th law of thermodynamics

A

if C is initially at eqlbm w both A & B, then A & B are both at eqlbm with each other

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3
Q

Actual temperature vs temperature interval

A

actual temp: written as __°C (blank degrees Celsius)

temp interval: __ C° ( blank Celsius degrees); its a difference/ change in temp

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4
Q

when volume is constant, pressure is directly proportional to…

A

Kelvin temperature so T1/T2 = P1/P2

ratio of two temps in Kelvin equals the ratio of corresponding pressures

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5
Q

To find the temp of T at the triple point of water…

A

Use the temp-pressure ratio.

T/T_triple = P/P_triple

T_triple = 273.16K

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6
Q

Linear Thermal Expansion eqn

A

ΔL = αL_oΔT

ΔL = change in length
α = coefficient of linear expansion
L_o = original length
ΔT = temp change

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7
Q

what is α and what are the units?

A

α is the coefficient of linear expansion, it is constant and is based on material.

units are K^-1 or C°^-1

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8
Q

Volume Thermal Expansion Eqn

A

ΔV = ßV_oΔT

ΔV= Change in Volume
ß = coefficient of volume expansion
V_o = Original volume
ΔT= change in temp

same units as linear expansion

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9
Q

When do you use volume expansion versus linear expansion

A

Volume expansion = liquids

linear = rods, change in length, solids

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10
Q

How to find ß when given the α of a material?

A

ß = 3α

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11
Q

Young’s modulus eqn - this involves tension

A

Y = (F/A)/(ΔL/L_o)
= (FL_o)/(AΔL)

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12
Q

to calculate thermal strain…

A

ΔL/L_o = αΔT

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13
Q

To solve thermal stress F/A…

A

F/A = -YαΔT

F = force needed to keep length of rod
A = cross sectional area of material
Y= young’s modulus
α = coefficient of linear expansion
ΔT= change in temp

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14
Q

what is young’s modulus and the units?

A

Young’s modulus is a measure of stiffness of a material

it is Tensile Stress/ Tensile Strain

Low Y =more flexible
High Y = more stiff

Units are Pa or N/m^2

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15
Q

what is tensile stress eqn

A

stress is force applied per area (F/A)

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16
Q

what is tensile strain eqn

A

deformity / change in shape due to force (ΔL/L_o)

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17
Q

What’s Hooke’s Law?

A

the greater the deforming forces, the greater the resulting deformation

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18
Q

tensile stress vs compressive stress

A

tensile stress is when force stretches/ elongates material

compressive stress is when force compresses/ shrinks the material

in general tensile is stretching

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19
Q

when temperature goes down, what force /stress is needed to maintain length?

A

contraction would happen when ΔT is negative so tensile force and stress is needed to pull the material to keep the length

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20
Q

when temp goes up, what force/stress is needed to maintain length?

A

material expands when ΔT is positive so required force and stress is compressive in order to maintain length

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21
Q

elastic modulus

A

property of material of which object is made

the ratio is stress/ strain

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22
Q

what is elasticity? elastic v plastic?

A

it depends on the type of material and not size

elastic: return to OG state after stress is removed

plastic: remains deformed after stress is removed

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22
Q

what is Bulk strain

A

ΔV/V_o

change in volume per unit volume

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23
Q

pressure in a fluid eqn

A

P=F/A

P = pressure in a fluid
F = force
A = area over which force is exerted

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24
Q

what is the bulk modulus for compression?

A

bulk stress/ bulk strain = -ΔP/(ΔV/V_o)

ΔP= additional pressure on object
ΔV = change in volume
V_o= OG volume

*minus sign is bc inc in pressure always leads to dec in volume

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25
Q

pressure is inversely proportional to…

A

volume

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26
Q

stress is proportional to…

A

strain

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27
Q

heat flow/ heat transfer

A

energy transferred only by ΔT

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28
Q

equation for heat required to change temp

A

Q=mcΔT

m = mass of material
c = specific heat of material
ΔT = change in temperature

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29
Q

high v low specific heat

A

high specific heat needs more heat to change temp

low specific heat heats up and slows down quicker

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30
Q

heat required to change temp of a certain number of moles

A

Q =nCΔT

n = # of moles
C = molar mass times specific heat capacity
ΔT = change in temp

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31
Q

heat of fusion/ latent heat of fusion (solid to liquid) Q needed

A

Q = +/- mL_f

m = mass of material
L_f = latent heat

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32
Q

what is heat of vaporization

A

the heat per unit mass to change liquid to gas

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33
Q

heat current in conduction/ rate of heat flow eqn

A

H = kA(Th-Tc)/L

H= heat current
k= thermal conductivity of rod material
A= cross-sectional area of rod
Th-Tc = temp of hot and cold rod

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34
Q

thermal resistance of slab in correlation to H is

A

H = A(Th-Tc)/R

R= thermal resistance
A = cross-sectional area

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35
Q

thermal resistance is given by

A

L/k

L= thickness of rod
k = thermal conductivity

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36
Q

materials with low k…

A

are good insulators

37
Q

materials with a large k…

A

are good conductors of heat

38
Q

when doubling thickness what happens to R

39
Q

what is emissivity?

A

e is a measurement of how efficiently a surface emits thermal radiation compared to a perfect black body at the same temperature

40
Q

what is a black body?

A

A black body is an idealized object that absorbs all incident radiation and emits the maximum possible radiation at a given temperature

41
Q

heat current of radiation equation aka Stefan-Boltzmann Law

A

H = AeσT^4

H = rate of heat flow
A = surface area of emitting surface
e = emissivity of surface
σ = Stephan Boltzmann constant = 5.67037442 * 10^-8 W/(m^2*K^4)
T = absolute temp of surface

42
Q

Net Heat current in radiation

A

H_net = H-emitted - H-absorbed
= AeσT^4 - AeσT_s^4
H_net = Aeσ(T^4 - T_s^4)

T = temperature of the radiating surface
T_s = temperature of the surroundings or the object with which the surface is radiating to

43
Q

Wien’s Law

A

λ_max = (2.9Kmm)/T

λ_max = peak wavelength

44
Q

what is the fraction of power in a certain range of wavelength?

A

the fraction of area under the graph in that range

45
Q

when two objects are at equilibrium…

A

H_in = H_out

H_in = rate at which sunlight/ source of heat is absorbed

H_out = rate at which heat is absorbed

46
Q

what is albedo

A

albedo is the overall average reflection coefficient for solar radiation incident on an object

47
Q

What is H_in due to sunlight

A

H_in = I_scpir_e^2 (1-a_e)

I_sc = solar constant
r_e = radius of earth
a_e = albedo

47
Q

what is solar constant

A

the intensity of sunlight, I_sc

48
Q

What is the temperature equilibrium equation for radiation?

A

T_e = [(1-a_e)I_sc/(4e_eσ)]^1/4

T_e = temperature eqlbm
a_e = albedo
I_sc = solar constant
e_e = emissivity
σ = stephan boltzmann constant

49
Q

what is intensity formula

A

power/area

50
Q

what is total power in terms of intensity

A

power = intensity * area

51
Q

H_in for earth

A

H _in = H_sun (r_e^2)/(4R_s-e^2)(1-a_e)

r_e = radius of earth
R_s-e = distance from sun to earth
a_e= albedo of earth

52
Q

if surface moves towards particle…

A

surface does work on particle during collision

52
Q

if surface is stationary…

A

work is done on the surface by the particle

53
Q

in a PV- diagram, if the volume expands….

A

work is positive - work is also the area under the curve

54
Q

in a PV - diagram, if the volume decrease…

A

work is negative

55
Q

in a PV- diagram, if work is done at constant pressure…

A

work is positive and is equal to p=(V_2-V_1)

56
Q

path

A

a series of intermediate states that get passed thru when a thermodynamic system changes from an initial state to a final state

57
Q

is work path dependent

A

yes it is
- depends not only on the final and initial state but also the intermediate states
- Q is also path dependent

58
Q

First Law of Thermodynamics

A

ΔU = Q - W

59
Q

is ΔU path dependent

A

no it is independent from the path; only depends on initial and final state

60
Q

Adiabatic

A

no heat transfer into or out of system;

Q = 0 therefore:

ΔU = -W

61
Q

when system expands adiabatically, work…

A

is done on its surroundings

work is pos = -ΔU

62
Q

when system compresses adiabatically, work…

A

is done on the system by surroundings

W is neg = + ΔU

63
Q

Isochoric

A

constant volume process

W = 0 therefore

ΔU = Q

64
Q

For isochoric processes, work is….

A

not done on surroundings, it doesn’t exist.

65
Q

Isobaric

A

constant - pressure process

W = p(V2-V1)

none of the qualities are zero

66
Q

Isothermal

A

constant temp

ΔU = 0 therefore:

W = Q

67
Q

For an ideal gas Cp =

A

Cp = Cv + R

Cp = molar heat capacity at constant pressure
Cv= molar heat capacity at constant volume
R = gas constant (8.314 J/(mol*K))

68
Q

Ratio of heat capacities

A

γ = Cp/Cv

69
Q

at constant pressure for an ideal gas ΔU…

A

ΔU = nCpΔT

70
Q

at constant volume for an ideal gas ΔU…

A

ΔU = nCvΔT

71
Q

thermal efficiency of an engine

A

e = W/Q_H = 1 - |Qc/Q_H|

e = thermal efficiency
W = work done by engine
Qc= heat rejected by engine
Q_H = heat absorbed by engine

72
Q

Steps in an Otto Cycle

A

cyclic process (starts and ends at the same place)

1.compressed adiabatically
2. heated at constant volume
3. expands adiabatically
4. cooled at constant volume

73
Q

thermal efficiency in otto cycle

A

e = 1- 1/(r(γ -1))

r= compression ratio
γ = ratio of heat capacities

74
Q

Steps in a Diesel Cycle

A
  1. compressed adiabatically
  2. heated at constant pressure
  3. expanded adiabatically
  4. cooled at constant pressure
75
Q

work for an engine

A

W = Q_H + Qc
W = |Q_H| - |Qc|

76
Q

work for refrigerator

A

|W| = |Q_H| - Qc

77
Q

what is the equation for CoP?

A

K = |Qc|/|W|
= |Qc| / [ |Q_H| - |Qc| ]

K = coefficient of performance of a refrigerator
W = work input of refrigerator
Q_H = Heat rejected from refrigerator
Qc = heat removed from inside of refrigerator

78
Q

Irreversible Processes

A

proceeds spontaneously in one direction but not the other

79
Q

Second Law of Thermodynamics - Kelvin Plank Statement “Engine” Statement

A

heat cannot completely be converted into mechanical work and be a cyclic process

80
Q

Second Law of Thermodynamics - “refrigerator” statement

A

heat does not go from cold to hot naturally without assistance

81
Q

entropy

A

the randomness of molecules; the more entropy, the more energy there is

82
Q

total entropy change during a reversible isothermal process

83
Q

total entropy for a Carnot engine

84
Q

is entropy path dependent

A

no; only needs initial and final state

85
Q

Second Law of Thermodynamics

A

no process is possible in which total entropy decreases

86
Q

Carnot Engine

A

maximum possible efficiency of an engine

on a temp v entropy graph its a square

87
Q

Steps of the Carnot Engine

A
  1. expands isothermally -> absorbs heat Q_H
  2. expands adiabatically -> Tc drops
  3. compresses isothermally -> rejects |Qc|
  4. expands adiabatically to OG state