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A light, horizontal beam, ABCDE, with A on the left-hand side is 26 m long. It is supported at two points, A and D. A point load of 20 kN is at B, 12 m from A. A point load of 30 is at C, 6 m from B. A uniform distributed load of 8 kN/m is between A and B. D is 4 m from C.

Physics

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2 parts
2.2

84.36 kN\text{84.36 kN}

61.64 kN\text{61.64 kN}

2.4

436.32 kN⋅m\text{436.32 kN} \cdot \text{m}

246.48 kN⋅m\text{246.48 kN} \cdot \text{m}

Step-by-step solution

4 steps

Here are the solutions to your statics problem:

Part 2.1

Make a neat, labelled diagram of the beam as described above.

A light, horizontal beam ABCDE, 26 m long, with A on the left-hand side.

  • Support at A (0 m) with reaction RAR_A.
  • Uniformly Distributed Load (UDL) of 8 kN/m8 \text{ kN/m} from A to B (0 m to 12 m).
  • Point load of 20 kN20 \text{ kN} downwards at B (12 m from A).
  • Point load of 30 kN30 \text{ kN} downwards at C (6 m from B, so 12+6=18 m12+6=18 \text{ m} from A).
  • Support at D (4 m from C, so 18+4=22 m18+4=22 \text{ m} from A) with reaction RDR_D.
  • End of beam at E (26 m from A).
      <------------------ 26 m ------------------>
      A       UDL=8kN/m       B       C       D       E
      |-----------------------|-------|-------|-------|
      ^                       |       |       ^
      RA                      20kN    30kN    RD
      0m                      12m     18m     22m     26m

Part 2.2

84.36 kN\text{84.36 kN}

Calculate the reactions of the supports at points A and D and test your answers.

  1. Convert the UDL to an equivalent point load.

    The UDL is 8 kN/m8 \text{ kN/m} over 12 m12 \text{ m} (from A to B).
    Equivalent UDL force FUDL=8 kN/m×12 m=96 kNF_{UDL} = 8 \text{ kN/m} \times 12 \text{ m} = 96 \text{ kN}.
    This force acts at the midpoint of A-B, which is 12 m/2=6 m12 \text{ m} / 2 = 6 \text{ m} from A.

  2. Apply the equilibrium equation for moments about point A (∑MA=0\sum M_A = 0).

    Taking clockwise moments as positive:

    (96 kN×6 m)+(20 kN×12 m)+(30 kN×18 m)−(RD×22 m)=0(96 \text{ kN} \times 6 \text{ m}) + (20 \text{ kN} \times 12 \text{ m}) + (30 \text{ kN} \times 18 \text{ m}) - (R_D \times 22 \text{ m}) = 0 576 kN⋅m+240 kN⋅m+540 kN⋅m−22RD=0576 \text{ kN} \cdot \text{m} + 240 \text{ kN} \cdot \text{m} + 540 \text{ kN} \cdot \text{m} - 22 R_D = 0 1356 kN⋅m−22RD=01356 \text{ kN} \cdot \text{m} - 22 R_D = 0 22RD=1356 kN⋅m22 R_D = 1356 \text{ kN} \cdot \text{m} RD=135622≈61.64 kNR_D = \frac{1356}{22} \approx 61.64 \text{ kN}
  3. Apply the equilibrium equation for vertical forces (∑Fy=0\sum F_y = 0).

    Taking upward forces as positive:

    RA+RD−96 kN−20 kN−30 kN=0R_A + R_D - 96 \text{ kN} - 20 \text{ kN} - 30 \text{ kN} = 0 RA+61.64 kN−146 kN=0R_A + 61.64 \text{ kN} - 146 \text{ kN} = 0 RA−84.36 kN=0R_A - 84.36 \text{ kN} = 0 RA=84.36 kNR_A = 84.36 \text{ kN}
  4. Test the answers by taking moments about point D (∑MD=0\sum M_D = 0).

    (RA×22 m)−(96 kN×(22−6) m)−(20 kN×(22−12) m)−(30 kN×(22−18) m)=0(R_A \times 22 \text{ m}) - (96 \text{ kN} \times (22-6) \text{ m}) - (20 \text{ kN} \times (22-12) \text{ m}) - (30 \text{ kN} \times (22-18) \text{ m}) = 0 (84.36×22)−(96×16)−(20×10)−(30×4)=0(84.36 \times 22) - (96 \times 16) - (20 \times 10) - (30 \times 4) = 0 1856.00−1536−200−120=01856.00 - 1536 - 200 - 120 = 0 1856.00−1856=01856.00 - 1856 = 0

    The reactions are correct.

    The reactions are:
    RA=84.36 kNR_A = \boxed{\text{84.36 kN}}
    RD=61.64 kNR_D = \boxed{\text{61.64 kN}}

Part 2.3

Draw a shear-force diagram and show ALL the main values on the diagram.

  • At A (x=0 m): Shear force VA=RA=84.36 kNV_A = R_A = 84.36 \text{ kN}.
  • From A to B (0 m to 12 m): Shear force decreases linearly due to UDL.
    • At B (just left, x=12 m): VB,left=RA−(8 kN/m×12 m)=84.36−96=−11.64 kNV_{B,left} = R_A - (8 \text{ kN/m} \times 12 \text{ m}) = 84.36 - 96 = -11.64 \text{ kN}.
  • At B (x=12 m): Shear force drops due to 20 kN20 \text{ kN} point load.
    • At B (just right): VB,right=−11.64−20=−31.64 kNV_{B,right} = -11.64 - 20 = -31.64 \text{ kN}.
  • From B to C (12 m to 18 m): Shear force is constant.
    • At C (just left, x=18 m): VC,left=−31.64 kNV_{C,left} = -31.64 \text{ kN}.
  • At C (x=18 m): Shear force drops due to 30 kN30 \text{ kN} point load.
    • At C (just right): VC,right=−31.64−30=−61.64 kNV_{C,right} = -31.64 - 30 = -61.64 \text{ kN}.
  • From C to D (18 m to 22 m): Shear force is constant.
    • At D (just left, x=22 m): VD,left=−61.64 kNV_{D,left} = -61.64 \text{ kN}.
  • At D (x=22 m): Shear force jumps up due to RDR_D.
    • At D (just right): VD,right=−61.64+RD=−61.64+61.64=0 kNV_{D,right} = -61.64 + R_D = -61.64 + 61.64 = 0 \text{ kN}.
  • From D to E (22 m to 26 m): Shear force is constant.
    • At E (x=26 m): VE=0 kNV_E = 0 \text{ kN}.

The shear force diagram starts at 84.36 kN84.36 \text{ kN} at A, decreases linearly to −11.64 kN-11.64 \text{ kN} at B, drops to −31.64 kN-31.64 \text{ kN}, remains constant to C, drops to −61.64 kN-61.64 \text{ kN}, remains constant to D, jumps to 0 kN0 \text{ kN}, and remains 0 kN0 \text{ kN} to E.
The point of zero shear force occurs between A and B where RA−8x=0  ⟹  84.36−8x=0  ⟹  x=10.55 mR_A - 8x = 0 \implies 84.36 - 8x = 0 \implies x = 10.55 \text{ m} from A.

Part 2.4

436.32 kN⋅m\text{436.32 kN} \cdot \text{m}

Calculate the bending moments at B and C.

  • Bending Moment at A (MAM_A): MA=0 kN⋅mM_A = 0 \text{ kN} \cdot \text{m} (support at end of beam).

  • Bending Moment at B (MBM_B, at x=12 m): Consider forces to the left of B: RAR_A and the UDL.

    MB=(RA×12 m)−(8 kN/m×12 m×12 m2)M_B = (R_A \times 12 \text{ m}) - (8 \text{ kN/m} \times 12 \text{ m} \times \frac{12 \text{ m}}{2}) MB=(84.36 kN×12 m)−(96 kN×6 m)M_B = (84.36 \text{ kN} \times 12 \text{ m}) - (96 \text{ kN} \times 6 \text{ m}) MB=1012.32 kN⋅m−576 kN⋅mM_B = 1012.32 \text{ kN} \cdot \text{m} - 576 \text{ kN} \cdot \text{m} MB=436.32 kN⋅mM_B = \boxed{\text{436.32 kN} \cdot \text{m}}
  • Bending Moment at C (MCM_C, at x=18 m): Consider forces to the left of C: RAR_A, UDL, and 20 kN20 \text{ kN} point load at B.

    MC=(RA×18 m)−(96 kN×(18−6) m)−(20 kN×(18−12) m)M_C = (R_A \times 18 \text{ m}) - (96 \text{ kN} \times (18-6) \text{ m}) - (20 \text{ kN} \times (18-12) \text{ m}) MC=(84.36 kN×18 m)−(96 kN×12 m)−(20 kN×6 m)M_C = (84.36 \text{ kN} \times 18 \text{ m}) - (96 \text{ kN} \times 12 \text{ m}) - (20 \text{ kN} \times 6 \text{ m}) MC=1518.48 kN⋅m−1152 kN⋅m−120 kN⋅mM_C = 1518.48 \text{ kN} \cdot \text{m} - 1152 \text{ kN} \cdot \text{m} - 120 \text{ kN} \cdot \text{m} MC=246.48 kN⋅mM_C = \boxed{\text{246.48 kN} \cdot \text{m}}

Part 2.5

Draw a neat bending-moment diagram and show ALL the main values on the diagram.

  • Bending Moment at A (MAM_A): 0 kN⋅m0 \text{ kN} \cdot \text{m}.
  • Maximum Bending Moment (between A and B): Occurs at x=10.55 mx = 10.55 \text{ m} (where shear force is zero). Mmax=(RA×10.55)−(8×10.55×10.552)M_{max} = (R_A \times 10.55) - (8 \times 10.55 \times \frac{10.55}{2}) Mmax=(84.36×10.55)−(4×10.552)M_{max} = (84.36 \times 10.55) - (4 \times 10.55^2) Mmax=889.70−445.21=444.49 kN⋅mM_{max} = 889.70 - 445.21 = 444.49 \text{ kN} \cdot \text{m}
  • Bending Moment at B (MBM_B): 436.32 kN⋅m436.32 \text{ kN} \cdot \text{m}.
  • Bending Moment at C (MCM_C): 246.48 kN⋅m246.48 \text{ kN} \cdot \text{m}.
  • Bending Moment at D (MDM_D, at x=22 m): MD=(RA×22)−(96×(22−6))−(20×(22−12))−(30×(22−18))M_D = (R_A \times 22) - (96 \times (22-6)) - (20 \times (22-12)) - (30 \times (22-18)) MD=(84.36×22)−(96×16)−(20×10)−(30×4)M_D = (84.36 \times 22) - (96 \times 16) - (20 \times 10) - (30 \times 4) MD=1856.00−1536−200−120=0 kN⋅mM_D = 1856.00 - 1536 - 200 - 120 = 0 \text{ kN} \cdot \text{m}
  • Bending Moment at E (MEM_E): 0 kN⋅m0 \text{ kN} \cdot \text{m} (free end).

The bending moment diagram starts at 0 kN⋅m0 \text{ kN} \cdot \text{m} at A, curves parabolically upwards to a maximum of 444.49 kN⋅m444.49 \text{ kN} \cdot \text{m} at x=10.55 mx=10.55 \text{ m}, then decreases to 436.32 kN⋅m436.32 \text{ kN} \cdot \text{m} at B. From B to C, it decreases linearly to 246.48 kN⋅m246.48 \text{ kN} \cdot \text{m}. From C to D, it decreases linearly to 0 kN⋅m0 \text{ kN} \cdot \text{m}. From D to E, it remains 0 kN⋅m0 \text{ kN} \cdot \text{m}.

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