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
Wood, k = 0.17250 mmGypsum board, k = 0.17150 mm22 °C-8 °CQ̇ = ?

A wall is made of 250 mm of wood and 150 mm of gypsum board, with an area of 8 m². The outer faces are at 22 °C and -8 °C. Find the heat flow Q̇ through the wall.

L1 = 250 mm, k1 = 0.17 W/(m·K)L2 = 150 mm, k2 = 0.17 W/(m·K)A = 8 m²T1 = 22 °CT3 = -8 °C
Q̇ = W
2.Heat conductionHard
Concrete, k = 1.4150 mmWood, k = 0.1775 mmroom 21 °Coutside -5 °CQ̇ = ?

A wall of 150 mm concrete and 75 mm wood separates a room at 21 °C from outside air at -5 °C. The convection coefficients are 6 W/(m²·K) inside and 25 W/(m²·K) outside, and the wall area is 6 m². Find the heat loss Q̇ through the wall.

L1 = 150 mm, k1 = 1.4 W/(m·K)L2 = 75 mm, k2 = 0.17 W/(m·K)A = 6 m²hi = 6 W/(m²·K)ho = 25 W/(m²·K)Troom = 21 °CTout = -5 °C
Q̇ = W
3.Heat exchangers (LMTD)Medium
lengthT90 °C50 °C40 °C15 °CΔT₁ΔT₂counter-flow

A counter-flow heat exchanger transfers 240 kW. The hot fluid cools from 90 to 50 °C and the cold fluid heats from 15 to 40 °C. The overall heat transfer coefficient is 800 W/(m²·K). Find the heat transfer area A needed.

Q̇ = 240 kWU = 800 W/(m²·K)Th: 90 → 50 °CTc: 15 → 40 °C
A = m²
4.Heat exchangers (LMTD)Hard
lengthT150 °C??15 °CΔT₁ΔT₂counter-flow

In a counter-flow heat exchanger both streams have the same heat capacity rate, ṁ·cp = 1 kW/K. The hot stream enters at 150 °C and the cold stream at 15 °C. The exchanger has A = 1.5 m² and U = 500 W/(m²·K). Find the hot outlet temperature Th,out.

Ch = Cc = 1 kW/KTh,in = 150 °CTc,in = 15 °CA = 1.5 m²U = 500 W/(m²·K)
Th,out = °C

3Solutions

1.Heat conduction

Answer: Q̇ = 102 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) = (250/1000)/(0.17·8) = 0.1838 K/W
R2 = L2/(k2A) = (150/1000)/(0.17·8) = 0.1103 K/W

Heat flow

Q̇ = (T1 − T3)/(R1 + R2) = 30/0.2941 = 102 W

Answer

Q̇ = 102 W
2.Heat conduction

Answer: Q̇ = 206.6 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/(6·6) = 0.02778 K/W
R1 = L1/(k1A) = (150/1000)/(1.4·6) = 0.01786 K/W
R2 = L2/(k2A) = (75/1000)/(0.17·6) = 0.07353 K/W
Ro = 1/(hoA) = 1/(25·6) = 0.006667 K/W
ΣR = 0.1258 K/W

Heat loss

Q̇ = (21 − (-5))/0.1258 = 206.6 W

Answer

Q̇ = 206.6 W
3.Heat exchangers (LMTD)

Answer: A = 7.133 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 counter-flow the hot inlet faces the cold outlet, and the hot outlet faces the cold inlet.

ΔT₁ = Th,in − Tc,out = 90 − 40 = 50 K
ΔT₂ = Th,out − Tc,in = 50 − 15 = 35 K

Log-mean temperature difference

ΔTlm = (ΔT₁ − ΔT₂)/ln(ΔT₁/ΔT₂) = (50 − 35)/ln(50/35) = 42.06 K

Area

A = Q̇/(U·ΔTlm) = 240000/(800·42.06) = 7.133 m²

Answer

A = 7.133 m²
4.Heat exchangers (LMTD)

Answer: Th,out = 92.14 °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

1·(150 − Th,out) = 0.75·(Th,out − 15)
Th,out = (1·150 + 0.75·15)/(1 + 0.75) = 92.14 °C

Answer

Th,out = 92.14 °C

Heat transferred: Q̇ = 57.86 kW; the cold stream leaves at 72.86 °C.

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