FE and PE Exam

FE Mechanical · knowledge area 12 · 7–11 questions

FE heat transfer review, three modes, one network

Heat transfer is 7–11 questions on five topics: conduction, convection, radiation, transient processes and heat exchangers. Most problems reduce to a thermal-resistance network or a single energy balance; the work is in choosing the right one.

Updated Oct 29, 2026 · Not affiliated with NCEES.

What the area covers

The specification names five topics. What each one means on the exam:

  • Conduction: Fourier's law in plane walls, cylinders and spheres, composite layers, fins and extended surfaces.
  • Convection: the convection coefficient, dimensionless groups (Reynolds, Prandtl, Nusselt) and the standard correlations for internal and external flow.
  • Radiation: blackbody and gray-body exchange, emissivity, view factors.
  • Transient processes: lumped capacitance and the conditions under which it holds.
  • Heat exchangers: overall coefficient U, log mean temperature difference, effectiveness-NTU.

15 heat transfer problems, every option explained

0 / 15 answered · 0 correct
Question 1 of 15 · Heat Transfer · 7–11 items

An enclosure consists of three surfaces: Surface 1 is a flat circular base of area A1, Surface 2 is a cylindrical side wall of area A2, and Surface 3 is a hemispherical dome of area A3 closing the top. If the view factor from the base to the cylindrical wall is F12, which expression represents the correct view factor from the dome to the base (F31)?

Solution

F11 = 0 → F13 = 1 − F12

A1F13 = A3F31 → F31 = (A1/A3)(1 − F12)

FE Reference Handbook, Heat Transfer: radiation (view factor relations).

F12 describes the wall, not the base-to-dome exchange, and A2 does not appear in the reciprocity for F31.
The area ratio is inverted: A1F13 = A3F31 gives F31 = (A1/A3)F13.
This subtracts a term built from the wrong reciprocity pair; F12 must first be turned into F13 by the summation rule.
This mixes view factors from different surfaces; a summation rule adds factors leaving one surface only.
The flat base sees nothing of itself, so F13 = 1 − F12; reciprocity A1F13 = A3F31 then gives F31.
Question 2 of 15 · Heat Transfer · 7–11 items

A long, straight rectangular aluminum fin (k = 205 W/(m·K)) is 2 mm thick, extends 50 mm from the base, and is 20 mm wide. The convection coefficient is 25 W/(m2·K), and the fin tip is insulated. Using η = tanh(mL)/(mL) with m = √(2h/(kt)), what is the fin efficiency?

Given
  • Thermal conductivity k = 205 W/(m·K)
  • Fin thickness t = 2 mm
  • Fin length L = 50 mm
  • Fin width w = 20 mm
  • Convection coefficient h = 25 W/(m2·K)
FindFin efficiency η (%)

Solution

m = √(2h/(kt)) = √(2 × 25/(205 × 0.002)) = 11.04 m−1, mL = 11.04 × 0.050 = 0.552

ηf = tanh(mL)/(mL) = 0.502/0.552 = 0.91

FE Reference Handbook, Heat Transfer: fins.

This uses the 20 mm width as the fin length; L is the 50 mm the fin projects from the base.
Dropping the 2 in m = √(2h/(kt)) counts only one face of the fin and overstates its efficiency.
m = √(2h/(kt)) = √(2 × 25/(205 × 0.002)) = 11.0 m−1, mL = 0.552, and η = tanh(0.552)/0.552 = 0.91.
tanh(mL) = 0.50 is only the numerator; the efficiency divides it by mL.
Question 3 of 15 · Heat Transfer · 7–11 items

A composite wall has two layers in series: the first is 0.10 m thick with k = 1.5 W/(m·K), and the second is 0.05 m thick with k = 0.05 W/(m·K). The inner and outer surface convection coefficients are 10 and 15 W/(m2·K), respectively. What is the overall heat transfer coefficient U?

Given
  • Layer 1 thickness L1 = 0.10 m
  • Layer 1 conductivity k1 = 1.5 W/(m·K)
  • Layer 2 thickness L2 = 0.05 m
  • Layer 2 conductivity k2 = 0.05 W/(m·K)
  • Inner convection coefficient hi = 10 W/(m2·K)
  • Outer convection coefficient ho = 15 W/(m2·K)
FindOverall heat transfer coefficient U (W/(m2·K))

Solution

R'' = 1/hi + L1/k1 + L2/k2 + 1/ho = 0.100 + 0.067 + 1.000 + 0.067 = 1.233 m2·K/W

U = 1/R'' = 0.81 W/(m2·K)

FE Reference Handbook, Heat Transfer: conduction through a composite wall.

Leaving out the 0.05 m insulation layer drops the largest resistance in the wall.
Multiplying thickness by conductivity (L·k) instead of dividing gives the wrong layer resistances.
This includes only the two conduction layers; the inner and outer film resistances also belong in the series sum.
Rtotal = 1/10 + 0.10/1.5 + 0.05/0.05 + 1/15 = 1.233 m2·K/W, so U = 1/1.233 = 0.81 W/(m2·K).
Question 4 of 15 · Heat Transfer · 7–11 items

Air flows parallel to a flat plate of length L = 2.0 m and width W = 1.0 m with a free-stream velocity of u∞ = 5.0 m/s. The free-stream temperature is T∞ = 300 K, and the plate surface is held at Ts = 400 K. Take the critical Reynolds number for transition as Rec = 5 × 105. Using the appropriate correlation below (laminar: NuL = 0.664 ReL0.5 Pr1/3; mixed: NuL = (0.037 ReL0.8 − 871) Pr1/3) and air properties from the table, what is the total convective heat loss from one side of the plate?

T (K)ν × 106 (m2/s)k × 103 (W/(m·K))Pr
30015.8926.30.707
35020.9230.00.700
40026.4133.80.690
Given
  • Plate length L = 2.0 m
  • Plate width W = 1.0 m
  • Free-stream velocity u∞ = 5.0 m/s
  • Free-stream temperature T∞ = 300 K
  • Surface temperature Ts = 400 K
  • Critical Reynolds number Rec = 5 × 105
  • Air properties: table at 300, 350 and 400 K
FindConvective heat loss from one side q (kW)

Solution

Tf = (300 + 400)/2 = 350 K: ν = 20.92 × 10−6 m2/s, k = 0.0300 W/(m·K), Pr = 0.700

ReL = (5.0)(2.0)/(20.92 × 10−6) = 4.78 × 105 < 5 × 105 → laminar

NuL = 0.664(4.78 × 105)0.5(0.700)1/3 = 407, h = Nu·k/L = 6.11 W/(m2·K)

q = hA(Ts − T∞) = 6.11 × 2.0 × 100 = 1.22 kW

FE Reference Handbook, Heat Transfer: forced convection (flat plate).

This uses the mixed correlation with properties at the surface temperature; properties belong at the film temperature, where the flow is laminar.
The mixed correlation applies only when ReL exceeds 5 × 105; at the film temperature the whole plate is laminar.
At the 350 K film temperature ReL = 5.0 × 2.0/20.92 × 10−6 = 4.78 × 105 < 5 × 105, so the laminar correlation applies: Nu = 407, h = 6.1 W/(m2·K), q = 1.22 kW.
Evaluating properties at the free-stream temperature makes ReL exceed 5 × 105 and wrongly switches to the mixed correlation.
This counts both faces of the plate (2 × 1.223 kW); the question asks for one side.
Question 5 of 15 · Heat Transfer · 7–11 items

What is the critical radius of insulation for a cylindrical pipe with insulation having a thermal conductivity of 0.05 W/(m·K) and exposed to air with a convection heat transfer coefficient of 10 W/(m²·K)?

Given
  • Insulation conductivity k = 0.05 W/(m·K)
  • Convection coefficient h = 10 W/(m2·K)
FindCritical radius rcr (mm)

Solution

rcr = k/h = 0.05 W/(m·K)/10 W/(m2·K) = 0.005 m = 5.0 mm

FE Reference Handbook, Heat Transfer: critical insulation radius.

For a cylinder rcr = k/h = 0.05/10 = 0.005 m = 5.0 mm.
2k/h is the critical radius of a sphere, not a cylinder.
4k/h = 20.0 mm is the critical diameter of a sphere; the question asks for the critical radius of a cylinder, k/h.
h/k = 200 is the inverse ratio and has units of 1/m, not length.
Question 6 of 15 · Heat Transfer · 7–11 items

Two parallel plates with emissivities ε1 = 0.8 and ε2 = 0.4 face each other. If the view factor is 1, what is the effective emissivity for radiation heat transfer between these surfaces?

Given
  • Emissivity of plate 1 ε1 = 0.8
  • Emissivity of plate 2 ε2 = 0.4
  • View factor F = 1
FindEffective emissivity εeff

Solution

εeff = 1/(1/ε1 + 1/ε2 − 1) = 1/(1/0.8 + 1/0.4 − 1) = 0.364

FE Reference Handbook, Heat Transfer: radiation between infinite parallel plates.

1 − (1 − ε1)(1 − ε2) = 1 − 0.2 × 0.6 = 0.880 is the chance a ray is absorbed by one of two thin layers, not the gray-plate exchange factor.
Averaging the emissivities has no physical basis; the resistances 1/ε add in series.
The lower emissivity alone is the limit only if the other plate were black (ε = 1).
εeff = 1/(1/ε1 + 1/ε2 − 1) = 1/(1.25 + 2.5 − 1) = 0.364 for infinite parallel gray plates.
Question 7 of 15 · Heat Transfer · 7–11 items

An engineer is evaluating a 1-shell-pass, 2-tube-pass heat exchanger. The shell-side (hot) fluid cools from 200 °F to 140 °F, while the tube-side (cold) fluid heats from 80 °F to 135 °F. Based on common design practice and the correction factor (F) values below for this configuration, what is the main conclusion about this design?

P valueF at R = 1.0F at R = 1.1
0.300.960.95
0.400.880.85
0.460.730.65
0.50AsymptoteAsymptote
Given
  • Configuration = 1 shell pass, 2 tube passes
  • Shell side (hot) = 200 °F → 140 °F
  • Tube side (cold) = 80 °F → 135 °F
  • F at P = 0.40: 0.88 (R = 1.0), 0.85 (R = 1.1)
  • F at P = 0.46: 0.73 (R = 1.0), 0.65 (R = 1.1)
  • F at P = 0.50: asymptote
FindAcceptability of the design

Solution

R = (Th,in − Th,out)/(tc,out − tc,in) = 60/55 = 1.09, P = (tc,out − tc,in)/(Th,in − tc,in) = 55/120 = 0.46

F(P = 0.46, R ≈ 1.1) ≈ 0.65 < 0.75 → add a shell pass

FE Reference Handbook, Heat Transfer: heat exchangers (LMTD correction factor).

A cold exit below the hot exit avoids a temperature cross at the outlets, but F still falls steeply here.
The method can be applied, but the low F shows the exchanger sits on the steep part of the curve and needs more shells.
P = 0.46 is below the asymptote near 0.50, so the LMTD and F are both defined.
R above 1 does not make a design acceptable; the F-factor at the operating P is what decides it.
R = 60/55 = 1.09 and P = 55/120 = 0.46 give F ≈ 0.65–0.73, below the usual 0.75–0.80 floor where a 1-2 exchanger becomes unreliable.
Question 8 of 15 · Heat Transfer · 7–11 items

A counterflow heat exchanger cools 10 kg/s of oil (cp = 2.0 kJ/(kg·K)) from 90 °C to 50 °C using water (cp = 4.0 kJ/(kg·K)) that enters at 20 °C and leaves at 30 °C. If the overall heat transfer coefficient is U = 0.5 kW/(m2·K), what is the required surface area?

Given
  • Oil flow = 10 kg/s
  • Oil cp = 2.0 kJ/(kg·K)
  • Oil temperatures: 90 °C in, 50 °C out
  • Water cp = 4.0 kJ/(kg·K)
  • Water temperatures: 20 °C in, 30 °C out
  • U = 0.5 kW/(m2·K)
FindRequired surface area (m2)

Solution

q = ṁcpΔToil = 10 × 2.0 × (90 − 50) = 800 kW

ΔTlm = [(90 − 30) − (50 − 20)]/ln(60/30) = 43.28 K

A = q/(U·ΔTlm) = 800/(0.5 × 43.28) = 36.97 m2

FE Reference Handbook, Heat Transfer: heat exchangers (LMTD).

Using the inlet-to-inlet difference (90 − 20 = 70 K) as the driving ΔT overstates it.
The arithmetic mean ΔT (45 K) is larger than the log mean, so it underestimates the area.
q = 10 × 2.0 × 40 = 800 kW; counterflow ΔTlm = (60 − 30)/ln 2 = 43.3 K, so A = 800/(0.5 × 43.3) = 36.97 m2.
This uses the parallel-flow end differences (70 K and 20 K); the exchanger is counterflow.
Using the water's cp of 4.0 for the oil doubles the duty; the oil has cp = 2.0 kJ/(kg·K).
Question 9 of 15 · Heat Transfer · 7–11 items

A composite wall consists of an outer brick layer, a middle section containing insulation and parallel wooden studs, and an inner drywall layer. Heat flows 1-dimensionally from the inside to the outside environment. Represent series heat-transfer paths with thermal-resistance networks: for conduction Rcond = L/(k · A) and for convection Rconv = 1/(h · A); combine resistances (series and parallel). Based on the variables defined in the table below, which of the following expressions correctly represents the equivalent conductive thermal resistance of the solid composite wall (excluding the air convective boundary layers)?

LayerDescriptionThermal Resistance Variable
OuterBrick layerR1
MiddleInsulationR2
MiddleWooden studsR3
InnerDrywallR4

Solution

Req = R1 + (R2R3)/(R2 + R3) + R4

Brick and drywall are in series with the middle layer, where insulation and studs are parallel paths: Rtotal = R1 + (R2 ∥ R3) + R4.
The parallel pair is combined correctly, but series resistances add directly, not as reciprocals.
This pairs the layers backwards: insulation and studs are side by side, not one after the other.
This puts all four layers in parallel; brick and drywall carry the full heat flow in series.
Adding reciprocals gives a conductance-like sum and treats every layer as parallel.
Question 10 of 15 · Heat Transfer · 7–11 items

A 5 mm diameter steel sphere (k = 50 W/(m·K), ρ = 7800 kg/m3, cp = 450 J/(kg·K)) initially at 200 °C is suddenly immersed in a fluid at 20 °C with h = 250 W/(m2·K). What is the Biot number for this transient process?

Given
  • Sphere diameter D = 5 mm
  • Conductivity k = 50 W/(m·K)
  • Density ρ = 7800 kg/m3
  • Specific heat cp = 450 J/(kg·K)
  • Convection coefficient h = 250 W/(m2·K)
FindBiot number Bi

Solution

Lc = V/As = D/6 = 0.005/6 = 8.33 × 10−4 m

Bi = hLc/k = 250 × 8.33 × 10−4/50 = 0.0042 (< 0.1, lumped model valid)

FE Reference Handbook, Heat Transfer: transient conduction (lumped capacitance).

For a sphere Lc = V/As = D/6 = 0.833 mm, so Bi = hLc/k = 250 × 0.000833/50 = 0.0042.
This uses Lc = D/3; V/As for a sphere is r/3 = D/6.
This uses the radius as Lc; the lumped-capacitance length is V/As = r/3.
This uses the full diameter as the characteristic length.
Question 11 of 15 · Heat Transfer · 7–11 items

For a lumped-capacitance thermal system, how is the time constant τ defined?

Solution

(T − T∞)/(Ti − T∞) = e−t/τ, τ = ρVcp/(hA)

FE Reference Handbook, Heat Transfer: transient conduction (lumped capacitance).

This is the reciprocal of τ, the decay rate in 1/s.
Multiplying capacitance by conductance does not give a time; the units are not seconds.
k/(ρcp) is the thermal diffusivity α, in m2/s, not a time constant.
The time constant is thermal capacitance ρVcp divided by convective conductance hA; the temperature falls to 37% of the initial difference after one τ.
Question 12 of 15 · Heat Transfer · 7–11 items

What is the Nusselt number for fully developed laminar flow in a circular tube with constant heat flux at the wall?

Solution

Fully developed laminar flow in a circular tube: NuD = 4.36 (uniform q''), 3.66 (uniform Ts). FE Reference Handbook, Heat Transfer: forced convection (internal flow).

3.66 is the value for a uniform wall temperature, not a uniform heat flux.
For fully developed laminar flow in a circular tube with uniform wall heat flux, NuD = 48/11 = 4.36.
7.54 is for laminar flow between infinite parallel plates at uniform temperature.
8.23 is for parallel plates with uniform heat flux, not a circular tube.
Question 13 of 15 · Heat Transfer · 7–11 items

What is the shape of the steady temperature distribution in a plane wall with uniform heat generation?

Solution

d2T/dx2 + q̇/k = 0 → T(x) = −q̇x2/(2k) + C1x + C2

A logarithmic profile belongs to radial conduction in a cylinder without generation.
With uniform generation, d2T/dx2 = −q̇/k is constant, so T(x) is a second-order polynomial with its peak at the center.
A linear profile belongs to a plane wall without heat generation.
Exponential profiles appear in fins and transient decay, not in steady conduction with uniform generation.
Question 14 of 15 · Heat Transfer · 7–11 items

A counterflow heat exchanger has an overall heat transfer coefficient of 500 W/(m2·K) and an area of 10 m2. Hot fluid enters at 80 °C at 2 kg/s (cp = 4.2 kJ/(kg·K)), and cold fluid enters at 30 °C at 1 kg/s (cp = 4.2 kJ/(kg·K)). What are the NTU and the effectiveness of the exchanger?

Given
  • Overall coefficient U = 500 W/(m2·K)
  • Area A = 10 m2
  • Hot inlet T = 80 °C
  • Hot flow ṁh = 2 kg/s
  • cp,h = 4.2 kJ/(kg·K)
  • Cold inlet T = 30 °C
  • Cold flow ṁc = 1 kg/s
  • cp,c = 4.2 kJ/(kg·K)
FindNTU and effectiveness ε

Solution

Cmin = 1 × 4200 = 4200 W/K, Cr = 4200/8400 = 0.5, NTU = UA/Cmin = 5000/4200 = 1.19

ε = [1 − e−NTU(1 − Cr)]/[1 − Cre−NTU(1 − Cr)] = 0.62

FE Reference Handbook, Heat Transfer: heat exchangers (effectiveness-NTU).

1 − e−NTU holds only when Cr = 0 (one fluid changing phase); here Cr = 0.5.
This divides UA by Cmax (8400 W/K); NTU is based on the smaller capacity rate.
The NTU is right, but this is the parallel-flow effectiveness; the exchanger is counterflow.
Cmin = 1 × 4200 = 4200 W/K, NTU = 5000/4200 = 1.19 and Cr = 0.5; the counterflow relation gives ε = 0.62.
Question 15 of 15 · Heat Transfer · 7–11 items

The thermal resistance of a cylindrical pipe with inner radius r1, outer radius r2, length L, and thermal conductivity k is given by:

Solution

R = ln(r2/r1)/(2πkL)

FE Reference Handbook, Heat Transfer: conduction through a cylindrical wall.

Radial conduction through a cylindrical shell gives a logarithmic temperature profile and this resistance.
This is the resistance to axial conduction along the pipe wall, not radial conduction through it.
This has no conductivity in it; it looks like a convection resistance 1/(hA) with h missing.
The plane-wall formula ignores that the area grows with radius; it is a fair approximation only for thin walls.

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Common traps

Checked against the Heat Transfer chapter of the FE Reference Handbook and Incropera's Fundamentals of Heat and Mass Transfer:

  • Radiation needs absolute temperature, to the fourth power. Subtracting temperatures first and then raising to the fourth power is a different, wrong number. Convert to K or °R, raise each to the fourth power, then subtract.
  • h is not U. The convection coefficient h describes one surface. The overall coefficient U combines both films and the wall, and it must be referenced to an area: inner and outer U of a thick tube differ.
  • Draw the network before adding numbers. Layers in the heat path are in series; side-by-side materials across the same path are in parallel. Writing the network first prevents adding conductances where resistances belong.
  • Check the Biot number before using lumped capacitance. The lumped model assumes a uniform temperature inside the body, which holds only when internal conduction resistance is small next to surface convection.
  • LMTD end differences. In counterflow, pair the hot inlet with the cold outlet; in parallel flow, inlet with inlet. Shell-and-tube and crossflow units need the correction factor on top.
  • Mass-based specific heat. The Handbook notes that its thermal diffusivity expression holds only when the specific heat is per unit mass.

Emissivity is a surface property, the view factor is geometry

Two surfaces with perfect emissivity still exchange little radiation if they barely see each other. Keep the two effects separate: emissivities go into the surface resistances, the view factor into the space resistance.

Other FE Mechanical areas

Heat transfer, quick answers

Should I use LMTD or effectiveness-NTU?

Use LMTD when all four end temperatures are known or easy to find. Use effectiveness-NTU when the outlet temperatures are the unknowns, because it avoids iterating.

How many heat transfer questions are on the FE Mechanical exam?

7–11, the same range as material properties and processing.

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FE Mechanical questions, answers and worked solutions in a study app.

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