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Free FE Civil practice problems

Ten real questions from our FE Civil bank, drawn from 10 of its 14 study topics, with fully worked solutions and the same figures our members get. No signup, no email. Try each one first, then reveal the solution.

10 with figures10 topicsFull worked solutions
  1. 1
    medium
    A. Earned value & CPM scheduling
    In the activity-on-node network shown for a storm-sewer replacement, the durations are A 6, B 9, C 14, D 4, E 2, F 7 and G 10 days. A, B and C start at day 0; D follows A and B; E and F follow D; G follows C; E, F and G precede End. The total float of activity D is most nearly:
    Figure for this questionStartd=0Ad=6Bd=9Cd=14Dd=4Ed=2Fd=7Gd=10Endd=0

    Figure — drag or pinch to move around

    1. 4 d
    2. 7 d
    3. 9 d
    4. 12 d
    Show the answer & worked solution

    Answer: A.4 d

    Float =LS−ES=LF−EF= LS - ES = LF - EF, with ESES = latest EFEF of the predecessors and LFLF = earliest LSLS of the successors (FE Reference Handbook, Civil Engineering — Construction, Nomenclature). Forward pass: ESD=max⁡(EFA, EFB)=max⁡(6, 9)=9ES_D = \max(EF_A,\, EF_B) = \max(6,\, 9) = 9 d, so EFD=9+4=13EF_D = 9 + 4 = 13 d; then EFE=13+2=15EF_E = 13 + 2 = 15, EFF=13+7=20EF_F = 13 + 7 = 20 and EFG=14+10=24EF_G = 14 + 10 = 24 d. The project takes 2424 d, set by the longest path (C–G). Backward pass: LSE=24−2=22LS_E = 24 - 2 = 22 and LSF=24−7=17LS_F = 24 - 7 = 17 d, so LFD=min⁡(22, 17)=17LF_D = \min(22,\, 17) = 17 d (F controls) and LSD=17−4=13LS_D = 17 - 4 = 13 d. Float of D =LSD−ESD=13−9=4= LS_D - ES_D = 13 - 9 = 4 d (equally LFD−EFD=17−13LF_D - EF_D = 17 - 13). Distractors: took the EARLIER finish at D's merge (ESD=EFA=6ES_D = EF_A = 6 d) in the forward pass, giving 7 d; took the LATER late start at D's burst (LFD=LSE=22LF_D = LS_E = 22 d) in the backward pass, giving 9 d; and measured D against the SHORTEST path through it (A–D–E) instead of the longest, reversing both rules, giving 12 d.
  2. 2
    medium
    A. Time value of money & equivalence
    An engineer borrows $200,000 to be repaid in 15 equal end-of-year payments at 6% per year. The annual payment is most nearly:
    Figure for this question0123456789101112131415PA = ?

    Figure — drag or pinch to move around

    1. $8,593
    2. $13,333
    3. $20,593
    4. $25,333
    Show the answer & worked solution

    Answer: C.$20,593

    The capital recovery factor (FE Reference Handbook 10.6 p. 235) converts a present amount into equal end-of-year payments: (A/P, 6%, 15)=i(1+i)n(1+i)n−1=0.06 (1.06)15(1.06)15−1=0.10296(A/P,\ 6\%,\ 15)=\dfrac{i(1+i)^n}{(1+i)^n-1}=\dfrac{0.06\,(1.06)^{15}}{(1.06)^{15}-1}=0.10296, printed as 0.1030 in the handbook's 6% factor table. The annual payment is $200,000 × 0.10296 = $20,593. Distractors: P/nP/n, spreading the principal evenly and ignoring interest ($13,333); the sinking-fund factor (A/F)(A/F) read in place of (A/P)(A/P) ($8,593), which treats the loan as a future sum; and simple interest on the full principal for all 15 years, spread evenly, P(1+in)/nP(1+in)/n ($25,333), which charges interest on money already repaid.
  3. 3
    medium
    A. Fluid properties, statics & energy/momentum
    Water flows steadily through a pipe that contracts from a diameter D1=200D_1 = 200 mm to D2=150D_2 = 150 mm. The upstream velocity is V1=1.5V_1 = 1.5 m/s. The velocity in the smaller section is most nearly:
    Figure for this questionV1 = 1.5 m/sD1 = 200 mmD2 = 150 mm(1)(2)

    Figure — drag or pinch to move around

    1. 0.844 m/s
    2. 2 m/s
    3. 2.67 m/s
    4. 4.74 m/s
    Show the answer & worked solution

    Answer: C.2.67 m/s

    Continuity (FE Reference Handbook 10.6 p. 185): the same flow Q=AvQ=Av passes both sections, so A1V1=A2V2A_1V_1=A_2V_2. With A=πD2/4A=\pi D^2/4 the π/4\pi/4 cancels, leaving V2=V1(D1D2)2=1.5(200150)2=2.67V_2=V_1\left(\dfrac{D_1}{D_2}\right)^2=1.5\left(\dfrac{200}{150}\right)^2=2.67 m/s, faster in the smaller section, as it must be. Distractors: the diameter ratio used un-squared, V1D1/D2V_1D_1/D_2 (2 m/s), forgetting that area goes as D2D^2; the area ratio inverted, V1(D2/D1)2V_1(D_2/D_1)^2 (0.844 m/s), which would have the water slow down in the smaller section; and the ratio squared twice, V1(D1/D2)4V_1(D_1/D_2)^4 (4.74 m/s), the area-ratio squaring applied a second time.
  4. 4
    medium
    A. Index properties, phase relations & effective stress
    At the Memphis levee borrow area the water table is 3 m below the ground surface. The soil above it is moist, with γ=16\gamma = 16 kN/m³; below it the soil is saturated, with γsat=19.5\gamma_{sat} = 19.5 kN/m³. The vertical effective stress at point A, 3.5 m below the water table, is most nearly:
    Figure for this questionγ = 16 kN/m³γsat = 19.5 kN/m³GWTA

    Figure — drag or pinch to move around

    1. 52.5 kPa
    2. 69.7 kPa
    3. 81.9 kPa
    4. 116 kPa
    Show the answer & worked solution

    Answer: C.81.9 kPa

    Effective stress (FE Reference Handbook, Civil Engineering — Geotechnical): σ′=σ−u\sigma' = \sigma - u with u=huγwu = h_u\gamma_w. Total stress at A: σ=(16 kN/m3)(3 m)+(19.5 kN/m3)(3.5 m)=116.25\sigma = (16\ \text{kN/m}^3)(3\ \text{m}) + (19.5\ \text{kN/m}^3)(3.5\ \text{m}) = 116.25 kPa. A is 3.5 m below the water table, so u=(9.81 kN/m3)(3.5 m)=34.34u = (9.81\ \text{kN/m}^3)(3.5\ \text{m}) = 34.34 kPa. σ′=116.25−34.34=81.9\sigma' = 116.25 - 34.34 = 81.9 kPa. Distractors: reported the total stress σ\sigma (pore pressure never subtracted), 116 kPa; measured the pressure head from the ground surface (u=9.81×6.5u = 9.81 \times 6.5), as if the water table were at the surface, 52.5 kPa; and used the moist γ=16\gamma = 16 kN/m³ for the full 6.5 m, ignoring the change at the water table, 69.7 kPa.
  5. 5
    medium
    A. Stress, strain, deformation & Mohr's circle
    A beam of solid rectangular cross-section, width b=50 mmb=50\,\text{mm} and depth h=100 mmh=100\,\text{mm}, carries an internal bending moment M=5 kN⋅mM=5\,\text{kN}\cdot\text{m}. The maximum bending (flexural) stress is most nearly:
    Rectangular beam section with the linear bending-stress distribution (max at the extreme fibre)M = 5 kN·mN.A.h = 100 mmb = 50 mmCTσ

    Figure — drag or pinch to move around

    1. 10 MPa
    2. 15 MPa
    3. 40 MPa
    4. 60 MPa
    Show the answer & worked solution

    Answer: D.60 MPa

    Maximum bending stress (Mechanics of Materials — Stresses in Beams): σ=McI\sigma=\dfrac{Mc}{I}, with the centroidal I=bh312=(50)(100)312=4.167×106 mm4I=\dfrac{bh^3}{12}=\dfrac{(50)(100)^3}{12}=4.167\times10^{6}\ \text{mm}^4 and c=h/2=50 mmc=h/2=50\ \text{mm}, which for a rectangle is σ=6Mbh2\sigma=\dfrac{6M}{bh^2}. With M=5 kN⋅m=5×106 N⋅mmM=5\ \text{kN·m}=5\times10^{6}\ \text{N·mm}: σ=6(5×106 N⋅mm)(50 mm)(100 mm)2=60\sigma=\dfrac{6(5\times10^{6}\ \text{N·mm})}{(50\ \text{mm})(100\ \text{mm})^2}=60 MPa. Distractors: used I=bh3/3I=bh^3/3, the area table's moment of inertia about the BASE, instead of the centroidal bh3/12bh^3/12 (¼ of the true stress); dropped the factor 6 (used σ=M/bh2\sigma=M/bh^2); and divided by the plastic section modulus Z=bh2/4Z=bh^2/4 instead of the elastic S=bh2/6S=bh^2/6 (two-thirds of the true stress).
  6. 6
    medium
    A. Equilibrium, trusses, centroids & friction
    A simply-supported beam of span L=6L=6 m carries a uniform load w=4w=4 kN/m over its entire length plus a point load P=12P=12 kN located 2 m from the left support (A). The pin reaction at A is most nearly:
    Loaded beam schematic with its supports and applied loadsw = 4 kN/mP = 12 kNRARBa = 2 mL = 6 m

    Figure — drag or pinch to move around

    1. 10 kN
    2. 16 kN
    3. 18 kN
    4. 20 kN
    Show the answer & worked solution

    Answer: D.20 kN

    Replace the uniform load by its resultant, wL=(4 kN/m)(6 m)=24wL=(4\ \text{kN/m})(6\ \text{m})=24 kN acting at midspan, 3 m from each support. Then take moments about the roller B, which removes RBR_B (Statics — Equilibrium Requirements, ΣM=0\Sigma M=0): RA(6 m)=(12 kN)(4 m)+(24 kN)(3 m)R_A(6\ \text{m})=(12\ \text{kN})(4\ \text{m})+(24\ \text{kN})(3\ \text{m}), so RA=48+726=20R_A=\dfrac{48+72}{6}=20 kN. Check with ΣFy=0\Sigma F_y=0: RB=12+24−20=16R_B=12+24-20=16 kN. Distractors: the point-load moment arm taken as aa instead of (L−a)(L-a) — moments summed about the wrong support — yielding RBR_B (16 kN); the point load split evenly regardless of its position (P/2P/2, giving 18 kN); and the load intensity w=4w=4 kN/m used as if it were the distributed load's resultant, instead of wL=24wL=24 kN, so A gets only w/2w/2 from it (10 kN).
  7. 7
    medium
    A. Determinate analysis, internal forces, deflection & buckling
    A simply supported beam of span L=6 mL=6\,\text{m} carries a uniformly distributed load w=10 kN/mw=10\,\text{kN/m} over its full length (self-weight included) and a concentrated load P=36 kNP=36\,\text{kN} at midspan, as shown. The maximum bending moment in the beam is most nearly:
    Loaded beam schematic with its supports and applied loadsABw = 10 kN/mP = 36 kNL = 6 m

    Figure — drag or pinch to move around

    1. 45 kN·m
    2. 57 kN·m
    3. 72 kN·m
    4. 99 kN·m
    Show the answer & worked solution

    Answer: D.99 kN·m

    Both loads are symmetric, so each one's maximum moment is at midspan and they superpose there (FE Reference Handbook, Mechanics of Materials — Simply Supported Beam Slopes and Deflections: Mmax=wL2/8M_{max} = wL^2/8 for the full uniform load and PL/4PL/4 for the central point load). Mmax=(10 kN/m)(6 m)28+(36 kN)(6 m)4=45+54=99M_{max} = \dfrac{(10\ \text{kN/m})(6\ \text{m})^2}{8} + \dfrac{(36\ \text{kN})(6\ \text{m})}{4} = 45 + 54 = 99 kN·m. Check by statics: each reaction is (wL+P)/2=48(wL + P)/2 = 48 kN, and at midspan M=48(3)−10(3)2/2=99M = 48(3) - 10(3)^2/2 = 99 kN·m. Distractors: kept only the uniform load's wL2/8wL^2/8 and forgot the point load, 45 kN·m; gave the point load the uniform load's coefficient, wL2/8+PL/8wL^2/8 + PL/8, 72 kN·m; and used the fixed-end moments wL2/12+PL/8wL^2/12 + PL/8, which belong to a beam fixed at both ends, 57 kN·m.
  8. 8
    medium
    A. Angles, distances, traverse & areas
    The corners of a four-sided parcel, taken in order around its boundary, have site coordinates (easting, northing, in m) of A (100, 100), B (320, 110), C (350, 290), D (120, 350). The area of the parcel is most nearly:
    Figure for this questionABBCCDDAABCDN

    Figure — drag or pinch to move around

    1. 49,000 m²
    2. 60,500 m²
    3. 98,000 m²
    4. 119,200 m²
    Show the answer & worked solution

    Answer: A.49,000 m²

    Area by coordinates (FE Reference Handbook, Civil Engineering — Area formulas): Area=12[XA(YB−YD)+XB(YC−YA)+XC(YD−YB)+XD(YA−YC)]\text{Area} = \tfrac12\left[X_A(Y_B - Y_D) + X_B(Y_C - Y_A) + X_C(Y_D - Y_B) + X_D(Y_A - Y_C)\right]. Substituting, in m: 12[100(110−350)+320(290−100)+350(350−110)+120(100−290)]=12[(−24,000)+60,800+84,000+(−22,800)]=12(98,000)=49,000\tfrac12\left[100(110 - 350) + 320(290 - 100) + 350(350 - 110) + 120(100 - 290)\right] = \tfrac12\left[(-24{,}000) + 60{,}800 + 84{,}000 + (-22{,}800)\right] = \tfrac12(98{,}000) = 49{,}000 m². Distractors: the ½ forgotten, 98,000 m²; the closing course left out (the products xDyA−xAyDx_Dy_A - x_Ay_D never formed, so the loop never returns to A), 60,500 m²; and only the xiyi+1x_iy_{i+1} products summed and halved, the second set xi+1yix_{i+1}y_i never subtracted, 119,200 m².
  9. 9
    medium
    A. Horizontal & vertical geometric design
    A simple horizontal circular curve has radius R=300 mR=300\,\text{m} and intersection angle Δ=80∘\Delta=80^\circ (see figure). The length of curve LL, from PC to PT along the arc, is most nearly:
    Figure for this questionOPCPTPIΔ = 80°R = 300 mT

    Figure — drag or pinch to move around

    1. 252 m
    2. 386 m
    3. 419 m
    4. 503 m
    Show the answer & worked solution

    Answer: C.419 m

    Length of curve (FE Reference Handbook, Civil Engineering — Horizontal Curves): L=R I π180L = R\,I\,\dfrac{\pi}{180} with I=ΔI = \Delta in degrees. L=(300 m)(80∘)π180=418.9L = (300\ \text{m})(80^\circ)\dfrac{\pi}{180} = 418.9 m. Distractors: returned the tangent distance T=Rtan⁡(Δ/2)T = R\tan(\Delta/2), PI to PC, 252 m; returned the long chord LC=2Rsin⁡(Δ/2)LC = 2R\sin(\Delta/2), the straight PC–PT distance, 386 m; and measured along both tangents, PC–PI–PT =2T= 2T, 503 m. Using RΔR\Delta with Δ\Delta still in degrees, without the π/180\pi/180, gives about 57×57\times the arc.
  10. 10
    medium
    A. Hydrology & open-channel hydraulics
    A rectangular concrete channel 3 m wide carries water at a uniform (normal) depth of 1.2 m. Manning's roughness is n=0.013n = 0.013 and the bed slope is S=0.001S = 0.001. The discharge is most nearly:
    Figure for this questiony = 1.2 mb = 3 m

    Figure — drag or pinch to move around

    1. 1.86 m³/s
    2. 6.68 m³/s
    3. 7.15 m³/s
    4. 9.89 m³/s
    Show the answer & worked solution

    Answer: B.6.68 m³/s

    Manning's equation (FE Reference Handbook, Civil Engineering — Hydraulics): Q=KnARH2/3S1/2Q = \dfrac{K}{n}A R_H^{2/3} S^{1/2} with K=1.0K = 1.0 in SI and RH=A/PR_H = A/P. Here A=by=(3)(1.2)=3.6A = by = (3)(1.2) = 3.6 m², P=b+2y=3+2(1.2)=5.4P = b + 2y = 3 + 2(1.2) = 5.4 m and RH=3.6/5.4=0.667R_H = 3.6/5.4 = 0.667 m, so Q=1.00.013(3.6)(0.667)2/3(0.001)1/2=6.68Q = \dfrac{1.0}{0.013}(3.6)(0.667)^{2/3}(0.001)^{1/2} = 6.68 m³/s. Distractors: the velocity V=1nRH2/3S1/2=1.856V = \tfrac{1}{n}R_H^{2/3}S^{1/2} = 1.856 m/s reported as the discharge (the ×A\times A forgotten), 1.86 m³/s; RH1/2R_H^{1/2} in place of RH2/3R_H^{2/3} (the square root taken of RHR_H as well as of SS), 7.15 m³/s; and the depth y=1.2y = 1.2 m used as the hydraulic radius, 9.89 m³/s.

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