Thermodynamics Flashcards

1
Q

Thermal linear expansion

A

ΔL = αLiΔT

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2
Q

Thermal volumetric expansion

A

ΔV = βViΔT

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3
Q

Relationship between volumetric expansion and linear expansion

A

β = 3*ɑ

for all isotropic solids

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4
Q

ideal gas law

A

PV = nRT

or

PV=NkBT

  • n -> number of moles*
  • N -> number of molecules*
  • kB -> Boltzmann’s constant*
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5
Q

Energy and temperature change relationship

A

Q = mcΔT

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6
Q

Latent heat

A

Q = ± mL
energy required for a phase change

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7
Q

Work to expand or compress gas

A

W = -∫PdV

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8
Q

First law of thermodynamics

A

ΔEint = Q + W

internal energy is equal to heat transfered and work done on the system

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9
Q

Adiabatic process

A

No heat leaves or is added to a system
ΔEint = W

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10
Q

isobaric system

A

process occurs under constant pressure

W = -P(Vf - Vi)

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11
Q

Isovolumetric system

A

Process that takes place under constant volumn

ΔEint = Q

W = 0

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12
Q

work done during isothermal expansion

A

W = n*R*T*ln(Vi/Vf)

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13
Q

heat per second (power) transfered by coduction

A

P = kA|dT/dx|
|dT/dx| = (Th - Tc)/L

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14
Q

Pressure and molecular kinetic energy

A

P = 2/3*(N/V)*(1/2 m* vavg2)

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15
Q

Temperature and mean velocity

A

1/2 m*vavg2 = 3/2 kbT

vrms = sqrt(3RT/M) = sqrt(3kbT/m)

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16
Q

heat and temperature at constant volumn

A

Q = nCVΔT

17
Q

heat and temperature at constant pressure

A

Q = nCPΔT

18
Q

molar specific heat at constant volumn for ideal gas

A

CV = 3/2*R

19
Q

ratio of specific heats in ideal gas

A

CP - CV = R

γ = CP/CV = 5/3

20
Q

Constant during adiabatic process

A

PVγ = const

using ideal gas law:

TVγ-1 = const

21
Q

Boltzmann distribution law

A

number of molecules at a certain energy

nV(E) = n0e-E/kbT

22
Q

rms velocity

A

vrms = sqrt(3kT/m)

23
Q

average velocity of gas molecules

A

vavg = sqrt(8kT/πm)

24
Q

most probable speed of gas molecules

A

vmp = sqrt(2kT/m)

25
Q

mean free path of gas molecule

A

l = 1/(√(2)πd2nV)

26
Q

collision frequency of molecules

A

f = √(2)πd2vavgnV = vavg/l

27
Q

effeciency of heat engine

A

e = Weng/|Qh| = 1 -|Qc|/|Qh|

28
Q

Change in entropy (general)

A

dS = dQr/T

Qr -> amount of energy transfered by heat in a reversible process

29
Q

Total change in entropy for carnot engine

A

0

30
Q

change in entropy for ideal gas

A

ΔS = nCV*ln(Tf/Ti) + nR*ln(Vf/Vi)

31
Q

entropy of macrostate

A

S = kbln(W)

W -> nuber of microstates of the system corresponding to mactrostate