Final Exam Formula Sheet
Final Exam Formula Sheet
Final Exam Formula Sheet
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M.P. Bradley <br />
11 April 2012 <br />
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EP271 <strong>Formula</strong> <strong>Sheet</strong> <br />
<br />
1 ST LAW OF THERMODYNAMICS: <br />
<br />
Delta‐Form: ΔE = ΔKE + ΔPE + ΔU = Q −W <br />
Differential Form: dE = dKE + dPE + dU = δQ −δW <br />
dE<br />
Time Rate Form: <br />
dt = dKE + dPE + dU = Q ˙ −W ˙ <br />
dt dt dt<br />
€<br />
<br />
€<br />
where Q = positive heat INPUT to system <br />
and W = positive work OUTPUT from system <br />
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<br />
WORK <br />
<br />
Expansion Work: δW = pdV <br />
<br />
Generalized work: δW = pdV −σd(Ax) −εdZ − E ⋅ d VP<br />
<br />
€<br />
<br />
HEAT TRANSFER: <br />
€<br />
Conduction: Q ˙<br />
x<br />
<br />
Radiation: <br />
= κA dT<br />
dx <br />
˙ Q rad<br />
= εσAT 4 <br />
( ) − µ 0<br />
<br />
H ⋅ d VM<br />
<br />
( ) + ... <br />
Special case: € Q ˙<br />
rad<br />
= εσA(T 4 4<br />
− T environment<br />
) NET radiative heat transfer to environment <br />
<br />
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Convection: <br />
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Q ˙<br />
c<br />
= hA(T − T fluid<br />
) <br />
<br />
ENTHALPY: H = U + PV SPECIFIC ENTHALPY: h = u + pv <br />
<br />
TWO‐PHASE LIQUID‐VAPOUR SYSTEMS <br />
€<br />
€<br />
m<br />
Vapour “Quality” Factor χ ≡<br />
vapour<br />
<br />
m liquid<br />
+ m vapour<br />
<br />
Specific volume of two‐phase mixture: v = ( 1− χ)v f<br />
+ χv g<br />
= v f<br />
+ χ( v g<br />
− v f ) <br />
Specific internal energy of two‐phase mixture: <br />
€<br />
u = ( 1− χ)u f<br />
+ χu g<br />
= u f<br />
+ χ( u g<br />
− u f ) <br />
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M.P. Bradley <br />
11 April 2012 <br />
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Specific enthalpy of two‐phase mixture: <br />
<br />
SPECIFIC HEATS: <br />
<br />
€<br />
⎛<br />
Specific heat at constant volume c v<br />
≡ ∂u ⎞<br />
⎜ ⎟ <br />
⎝ ∂T ⎠<br />
v<br />
⎛<br />
Specific heat at constant pressure c p<br />
≡ ∂h ⎞<br />
⎜ ⎟ <br />
⎝ ∂T ⎠<br />
h = ( 1− χ)h f<br />
+ χh g<br />
= h f<br />
+ χ( h g<br />
− h f ) <br />
Specific heat ratio: k ≡ c € p<br />
(Note that k is also often called “gamma” γ ) <br />
c v<br />
<br />
€<br />
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IDEAL GAS MODEL: <br />
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Gas Compressibility Factor Z = pv<br />
R T <br />
For an ideal gas, Z =1.0 <br />
and therefore: <br />
<br />
€<br />
pv = R<br />
€<br />
T (per unit mole, R = 8.314 J/mol.K) <br />
<br />
pv = RT (per unit mass) <br />
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Pressure‐Volume Relationship for a Polytropic process: pV n = constant <br />
Work done in polytropic expansion (2 cases): <br />
W = p 2V 2<br />
− p 1<br />
V 1<br />
(valid for n ≠1) <br />
1− n<br />
⎛<br />
W = p 1<br />
V 1<br />
ln V ⎞<br />
2<br />
⎜ ⎟ (valid for n =1.0) <br />
⎝ V 1 ⎠<br />
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<br />
CONTROL VOLUME (CV) ANALYSIS <br />
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<br />
Mass Flow Rate Balance: ∑ m ˙ i<br />
= ∑ ˙<br />
<br />
Energy Rate Balance: <br />
€<br />
<br />
CARNOT EFFICIENCY <br />
<br />
€<br />
⎛<br />
η MAX<br />
= W ⎞<br />
OUT<br />
⎜ ⎟<br />
⎝ ⎠<br />
Q H<br />
MAX<br />
dE CV<br />
dt<br />
=1− T C<br />
T H<br />
<br />
i<br />
e<br />
m e<br />
p<br />
€<br />
where m ˙ = ρAV <br />
= Q ˙<br />
CV<br />
− ˙ ⎛<br />
W € CV<br />
+ m ˙ i<br />
h i<br />
+ V 2<br />
i<br />
2 + gz ⎞ ⎛<br />
∑ ⎜<br />
i⎟<br />
− m ˙ e<br />
h e<br />
+ V 2<br />
e<br />
⎝<br />
⎠<br />
2 + gz ⎞<br />
∑ ⎜<br />
e⎟<br />
<br />
⎝<br />
⎠<br />
i<br />
e<br />
€
M.P. Bradley <br />
11 April 2012 <br />
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ENTROPY <br />
<br />
⎛<br />
Clausius <strong>Formula</strong> for Entropy Changes: dS = δQ ⎞<br />
⎜ ⎟ <br />
⎝ T ⎠<br />
<br />
⎛ 2δQ⎞<br />
S 2<br />
= S 1<br />
+ ⎜ ∫ ⎟ <br />
⎝<br />
1<br />
T ⎠<br />
internally reversible €<br />
<br />
Boltzmann <strong>Formula</strong> for Absolute Entropy: S = k B<br />
lnΩ <br />
<br />
KINETIC THEORY OF GASES <br />
Maxwell Boltzmann Distribution of Molecular Speeds <br />
€<br />
<br />
3 /<br />
⎛ m ⎞<br />
g(v) = ⎜ ⎟<br />
24πv 2 e − mv 2<br />
2k B T<br />
⎝ 2πk B<br />
T ⎠<br />
<br />
<br />
Characteristic Atomic/Molecular Speeds in a Gas <br />
Most Probable Atomic/Molecular Speed <br />
v MP<br />
= 2 k T B<br />
m ≈1.41 k BT /m <br />
Mean Atomic/Molecular Speed <br />
v MP<br />
=<br />
8 k B<br />
T<br />
π m ≈1.60 k BT /m <br />
RMS Speed <br />
<br />
€<br />
Maxwell Boltzmann Energy Distribution <br />
1<br />
( k B T ) 3 / 2 Ee −E / k B T <br />
g E<br />
(E) = 2 π<br />
<br />
Atomic/Molecular Collision Theory <br />
Mean Free Path in a Gas: <br />
λ =<br />
1<br />
2σn =<br />
k B T<br />
2σP <br />
<br />
FREE ENERGY FUNCTIONS <br />
<br />
€<br />
€<br />
v MP<br />
=<br />
3 k B T<br />
m ≈1.73 k BT /m <br />
Gibbs: G = H − TS <br />
<br />
Helmholtz: Ψ = U − TS <br />
€<br />
<br />
Equilibrium condition at constant Temperature & pressure: dG] T ,p<br />
= 0 <br />
(i.e. at equilibrium the Gibbs Free Energy Function has its minimum value ) <br />
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M.P. Bradley <br />
11 April 2012 <br />
€<br />
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THERMODYNAMIC RELATIONS <br />
<br />
TdS Equations: <br />
<br />
TdS = dU + pdV <br />
<br />
TdS = dH −Vdp <br />
<br />
<br />
Maxwell Relations: <br />
<br />
⎛ ∂T ⎞ ⎛<br />
⎜ ⎟ = − ∂p ⎞<br />
⎛ ∂p ⎞ ⎛<br />
⎜ ⎟ ⎜ ⎟ = ∂s ⎞<br />
⎜ ⎟ <br />
⎝ ∂v ⎠<br />
s<br />
⎝ ∂s ⎠<br />
v<br />
⎝ ∂T ⎠<br />
v<br />
⎝ ∂v ⎠<br />
T<br />
<br />
⎛ ∂T ⎞ ⎛<br />
⎜ ⎟ = ∂v ⎞<br />
⎛ ∂v ⎞ ⎛<br />
⎜ ⎟ ⎜ ⎟ = − ∂s ⎞<br />
⎜ ⎟ <br />
⎝ ∂p ⎠ ⎝ ∂s⎠<br />
s<br />
p € ⎝ ∂T ⎠<br />
p ⎝ ∂p⎠<br />
T<br />
<br />
<br />
USEFUL CONSTANTS: <br />
€<br />
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Boltzmann’s Constant: kB = 1.38 x 10 23 J/K <br />
<br />
Avogadro’s Number: NA = 6.022 x 10 23 particles/mole <br />
<br />
Molar Gas Constant: R = 8.314 J/mol.K <br />
<br />
Stefan‐Boltzmann Constant: σ = 5.67 × 10 ‐8 W/m 2 •K 4 <br />
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