Heat Transfer: cram pack

Formula sheets, the key method steps for every topic and 4 practice problems, with full solutions at the back.

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1Formulas and methods

Heat conduction

Fourier’s law
Q̇ = kAΔT/L
Conduction resistance
R = L/(kA)
Convection resistance
R = 1/(hA)
Resistances in series
Q̇ = ΔTtotal/ΣR
U-value
U = 1/(ΣR·A)

Heat exchangers (LMTD)

Heat duty
Q = U·A·ΔTlm
Log mean temperature difference
ΔTlm = (ΔT1 − ΔT2)/ln(ΔT1/ΔT2)
Stream balance
Q = ṁcp(Tin − Tout)

2Practice problems

1.Heat conductionMedium
Mineral wool, k = 0.0450 mmExpanded polystyrene, k = 0.03575 mm19 °C0 °CQ̇ = ?

A wall is made of 50 mm of mineral wool and 75 mm of expanded polystyrene, with an area of 15 m². The outer faces are at 19 °C and 0 °C. Find the heat flow Q̇ through the wall.

L1 = 50 mm, k1 = 0.04 W/(m·K)L2 = 75 mm, k2 = 0.035 W/(m·K)A = 15 m²T1 = 19 °CT3 = 0 °C
Q̇ = W
2.Heat conductionHard
Wood, k = 0.17150 mmExpanded polystyrene, k = 0.03575 mmroom 21 °Coutside 5 °CQ̇ = ?

A wall of 150 mm wood and 75 mm expanded polystyrene separates a room at 21 °C from outside air at 5 °C. The convection coefficients are 7.7 W/(m²·K) inside and 20 W/(m²·K) outside, and the wall area is 8 m². Find the heat loss Q̇ through the wall.

L1 = 150 mm, k1 = 0.17 W/(m·K)L2 = 75 mm, k2 = 0.035 W/(m·K)A = 8 m²hi = 7.7 W/(m²·K)ho = 20 W/(m²·K)Troom = 21 °CTout = 5 °C
Q̇ = W
3.Heat exchangers (LMTD)Medium
lengthT155 °C105 °C20 °C45 °CΔT₁ΔT₂parallel flow

A parallel-flow heat exchanger transfers 280 kW. The hot fluid cools from 155 to 105 °C and the cold fluid heats from 20 to 45 °C. The overall heat transfer coefficient is 300 W/(m²·K). Find the heat transfer area A needed.

Q̇ = 280 kWU = 300 W/(m²·K)Th: 155 → 105 °CTc: 20 → 45 °C
A = m²
4.Heat exchangers (LMTD)Hard
lengthT125 °C??15 °CΔT₁ΔT₂counter-flow

In a counter-flow heat exchanger both streams have the same heat capacity rate, ṁ·cp = 4 kW/K. The hot stream enters at 125 °C and the cold stream at 15 °C. The exchanger has A = 4 m² and U = 500 W/(m²·K). Find the hot outlet temperature Th,out.

Ch = Cc = 4 kW/KTh,in = 125 °CTc,in = 15 °CA = 4 m²U = 500 W/(m²·K)
Th,out = °C

3Solutions

1.Heat conduction

Answer: Q̇ = 84 W

Thermal resistance: steady heat flow through layers in series behaves like current through resistors in series: Q̇ = ΔT/ΣR, with R = L/(kA) for a conducting layer and R = 1/(hA) for a convecting surface. The temperature drop across each layer is proportional to its resistance.

Layer resistances

R1 = L1/(k1A) = (50/1000)/(0.04·15) = 0.08333 K/W
R2 = L2/(k2A) = (75/1000)/(0.035·15) = 0.1429 K/W

Heat flow

Q̇ = (T1 − T3)/(R1 + R2) = 19/0.2262 = 84 W

Answer

Q̇ = 84 W
2.Heat conduction

Answer: Q̇ = 39.94 W

Thermal resistance: steady heat flow through layers in series behaves like current through resistors in series: Q̇ = ΔT/ΣR, with R = L/(kA) for a conducting layer and R = 1/(hA) for a convecting surface. The temperature drop across each layer is proportional to its resistance.

Resistances in series

Ri = 1/(hiA) = 1/(7.7·8) = 0.01623 K/W
R1 = L1/(k1A) = (150/1000)/(0.17·8) = 0.1103 K/W
R2 = L2/(k2A) = (75/1000)/(0.035·8) = 0.2679 K/W
Ro = 1/(hoA) = 1/(20·8) = 0.00625 K/W
ΣR = 0.4006 K/W

Heat loss

Q̇ = (21 − (5))/0.4006 = 39.94 W

Answer

Q̇ = 39.94 W
3.Heat exchangers (LMTD)

Answer: A = 10.09 m²

LMTD method: the temperature difference between the streams changes along the exchanger, so the rate equation uses its logarithmic mean: Q̇ = U·A·ΔTlm, with ΔTlm = (ΔT₁ − ΔT₂)/ln(ΔT₁/ΔT₂), where ΔT₁ and ΔT₂ are the differences at the two ends. Counter-flow gives a larger ΔTlm than parallel flow for the same inlet and outlet temperatures.

End temperature differences

In parallel flow both inlets are at the same end, and both outlets at the other.

ΔT₁ = Th,in − Tc,in = 155 − 20 = 135 K
ΔT₂ = Th,out − Tc,out = 105 − 45 = 60 K

Log-mean temperature difference

ΔTlm = (ΔT₁ − ΔT₂)/ln(ΔT₁/ΔT₂) = (135 − 60)/ln(135/60) = 92.49 K

Area

A = Q̇/(U·ΔTlm) = 280000/(300·92.49) = 10.09 m²

Answer

A = 10.09 m²
4.Heat exchangers (LMTD)

Answer: Th,out = 88.33 °C

LMTD method: the temperature difference between the streams changes along the exchanger, so the rate equation uses its logarithmic mean: Q̇ = U·A·ΔTlm, with ΔTlm = (ΔT₁ − ΔT₂)/ln(ΔT₁/ΔT₂), where ΔT₁ and ΔT₂ are the differences at the two ends. Counter-flow gives a larger ΔTlm than parallel flow for the same inlet and outlet temperatures.

Constant temperature difference

The cold outlet sits opposite the hot inlet: Tc,out = Tc,in + (Th,in − Th,out), so ΔT₁ = Th,in − Tc,out = Th,out − Tc,in = ΔT₂.

ΔTlm = Th,out − Tc,in

Energy balance equals rate equation

4·(125 − Th,out) = 2·(Th,out − 15)
Th,out = (4·125 + 2·15)/(4 + 2) = 88.33 °C

Answer

Th,out = 88.33 °C

Heat transferred: Q̇ = 146.7 kW; the cold stream leaves at 51.67 °C.

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