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Calculate the coordinates of the centroid of the lamina shown in FIGURE 2.

Mathematics

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Answer

RB=37.6 kNR_B = \text{37.6 kN}

RD=72.4 kNR_D = \text{72.4 kN}

(xˉ,yˉ)=(42.31 mm,31.54 mm)(\bar{x}, \bar{y}) = (42.31 \text{ mm}, 31.54 \text{ mm})

Step-by-step solution

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5.1.1 The reaction forces at supports B and D.

First, we need to determine the equivalent point load for the uniformly distributed load (UDL).
The UDL is 6 kN/m6 \text{ kN/m} over a length of 1.5 m+3.5 m=5 m1.5 \text{ m} + 3.5 \text{ m} = 5 \text{ m}.
The total force from the UDL is FUDL=6 kN/m×5 m=30 kNF_{UDL} = 6 \text{ kN/m} \times 5 \text{ m} = 30 \text{ kN}.
This force acts at the centroid of the UDL, which is 5 m/2=2.5 m5 \text{ m} / 2 = 2.5 \text{ m} from point A.

Let's define the positions of all forces and supports from point A (left end of the beam):

  • Point A: x=0 mx = 0 \text{ m} (18 kN downward force)
  • Support B: x=1.5 mx = 1.5 \text{ m} (Reaction RBR_B upward)
  • UDL equivalent force: x=2.5 mx = 2.5 \text{ m} (30 kN downward force)
  • Point C: x=1.5 m+3.5 m=5 mx = 1.5 \text{ m} + 3.5 \text{ m} = 5 \text{ m} (40 kN downward force)
  • Support D: x=5 m+1.5 m=6.5 mx = 5 \text{ m} + 1.5 \text{ m} = 6.5 \text{ m} (Reaction RDR_D upward)
  • Point E: x=6.5 m+2.5 m=9 mx = 6.5 \text{ m} + 2.5 \text{ m} = 9 \text{ m} (22 kN downward force)
  1. Apply the equilibrium equation for the sum of vertical forces.

    Assume upward forces are positive.

    ∑Fy=0\sum F_y = 0 RB+RD−18 kN−30 kN−40 kN−22 kN=0R_B + R_D - 18 \text{ kN} - 30 \text{ kN} - 40 \text{ kN} - 22 \text{ kN} = 0 RB+RD−110 kN=0R_B + R_D - 110 \text{ kN} = 0 RB+RD=110 kN(1)R_B + R_D = 110 \text{ kN} \quad (1)
  2. Apply the equilibrium equation for the sum of moments about support B.

    Assume clockwise moments are positive.

    ∑MB=0\sum M_B = 0

    The moment arms are calculated relative to point B (x=1.5 mx=1.5 \text{ m}).

    (18 kN×1.5 m)+(30 kN×(2.5 m−1.5 m))+(40 kN×(5 m−1.5 m))−(RD×(6.5 m−1.5 m))+(22 kN×(9 m−1.5 m))=0(18 \text{ kN} \times 1.5 \text{ m}) + (30 \text{ kN} \times (2.5 \text{ m} - 1.5 \text{ m})) + (40 \text{ kN} \times (5 \text{ m} - 1.5 \text{ m})) - (R_D \times (6.5 \text{ m} - 1.5 \text{ m})) + (22 \text{ kN} \times (9 \text{ m} - 1.5 \text{ m})) = 0 (18×1.5)+(30×1)+(40×3.5)−(RD×5)+(22×7.5)=0(18 \times 1.5) + (30 \times 1) + (40 \times 3.5) - (R_D \times 5) + (22 \times 7.5) = 0 27+30+140−5RD+165=027 + 30 + 140 - 5R_D + 165 = 0 362−5RD=0362 - 5R_D = 0 5RD=3625R_D = 362 RD=3625=72.4 kNR_D = \frac{362}{5} = 72.4 \text{ kN}
  3. Substitute the value of RDR_D into Equation (1) to find RBR_B.

    RB+72.4 kN=110 kNR_B + 72.4 \text{ kN} = 110 \text{ kN} RB=110 kN−72.4 kNR_B = 110 \text{ kN} - 72.4 \text{ kN} RB=37.6 kNR_B = 37.6 \text{ kN}

    The reaction forces are:

    • RB=37.6 kNR_B = \boxed{\text{37.6 kN}}
    • RD=72.4 kNR_D = \boxed{\text{72.4 kN}}

    5.1.2 Draw the shear force diagram for the beam.

    We will calculate the shear force at key points along the beam, starting from the left (point A).

    • At A (x=0 mx=0 \text{ m}): VA=−18 kNV_A = -18 \text{ kN} (downward force)

    • Just before B (x=1.5− mx=1.5^- \text{ m}): The UDL acts from x=0x=0 to x=5 mx=5 \text{ m}. Shear force due to UDL up to B = 6 kN/m×1.5 m=9 kN6 \text{ kN/m} \times 1.5 \text{ m} = 9 \text{ kN}. VB−=−18 kN−9 kN=−27 kNV_{B^-} = -18 \text{ kN} - 9 \text{ kN} = -27 \text{ kN}

    • Just after B (x=1.5+ mx=1.5^+ \text{ m}): VB+=VB−+RB=−27 kN+37.6 kN=10.6 kNV_{B^+} = V_{B^-} + R_B = -27 \text{ kN} + 37.6 \text{ kN} = 10.6 \text{ kN}

    • Just before C (x=5− mx=5^- \text{ m}): Shear force from B to C due to UDL = 6 kN/m×(5 m−1.5 m)=6 kN/m×3.5 m=21 kN6 \text{ kN/m} \times (5 \text{ m} - 1.5 \text{ m}) = 6 \text{ kN/m} \times 3.5 \text{ m} = 21 \text{ kN}. VC−=VB+−21 kN=10.6 kN−21 kN=−10.4 kNV_{C^-} = V_{B^+} - 21 \text{ kN} = 10.6 \text{ kN} - 21 \text{ kN} = -10.4 \text{ kN}

    • Just after C (x=5+ mx=5^+ \text{ m}): VC+=VC−−40 kN=−10.4 kN−40 kN=−50.4 kNV_{C^+} = V_{C^-} - 40 \text{ kN} = -10.4 \text{ kN} - 40 \text{ kN} = -50.4 \text{ kN}

    • Just before D (x=6.5− mx=6.5^- \text{ m}): There are no distributed loads or point loads between C and D. VD−=VC+=−50.4 kNV_{D^-} = V_{C^+} = -50.4 \text{ kN}

    • Just after D (x=6.5+ mx=6.5^+ \text{ m}): VD+=VD−+RD=−50.4 kN+72.4 kN=22 kNV_{D^+} = V_{D^-} + R_D = -50.4 \text{ kN} + 72.4 \text{ kN} = 22 \text{ kN}

    • At E (x=9 mx=9 \text{ m}): There are no distributed loads or point loads between D and E. VE=VD+−22 kN=22 kN−22 kN=0 kNV_E = V_{D^+} - 22 \text{ kN} = 22 \text{ kN} - 22 \text{ kN} = 0 \text{ kN} (This confirms the calculations are correct as the shear force closes to zero at the end of the beam).

    The shear force diagram will be drawn based on these values.

    • From A to B, the shear force decreases linearly from −18 kN-18 \text{ kN} to −27 kN-27 \text{ kN}.
    • At B, it jumps up to 10.6 kN10.6 \text{ kN}.
    • From B to C, it decreases linearly from 10.6 kN10.6 \text{ kN} to −10.4 kN-10.4 \text{ kN}.
    • At C, it jumps down to −50.4 kN-50.4 \text{ kN}.
    • From C to D, it remains constant at −50.4 kN-50.4 \text{ kN}.
    • At D, it jumps up to 22 kN22 \text{ kN}.
    • From D to E, it remains constant at 22 kN22 \text{ kN} and then drops to 0 kN0 \text{ kN} at E.

    The point where the shear force is zero between B and C can be found by similar triangles or by setting the shear force equation to zero.
    Let x′x' be the distance from B where shear force is zero.
    10.6−6x′=0  ⟹  x′=10.66≈1.767 m10.6 - 6x' = 0 \implies x' = \frac{10.6}{6} \approx 1.767 \text{ m} from B.
    This corresponds to x=1.5+1.767=3.267 mx = 1.5 + 1.767 = 3.267 \text{ m} from A.

    The shear force diagram is as follows:

    \begin{tikzpicture}[scale=0.8] % Beam line \draw (0,0) -- (9,0); % Supports \draw (1.5,-0.5) -- (1.5,0.5); \draw (1.5,-0.5) -- (1.2,-0.8); \draw (1.5,-0.5) -- (1.8,-0.8); \draw (6.5,-0.5) -- (6.5,0.5); \draw (6.5,-0.5) -- (6.2,-0.8); \draw (6.5,-0.5) -- (6.8,-0.8); % Labels for points \node at (0,-0.3) {A}; \node at (1.5,-0.3) {B}; \node at (5,-0.3) {C}; \node at (6.5,-0.3) {D}; \node at (9,-0.3) {E}; % Shear force diagram \draw[blue, thick] (0,0) node[left] {$V$} -- (0,-1.8) node[below left] {$-18$}; \draw[blue, thick] (0,-1.8) -- (1.5,-2.7) node[below left] {$-27$}; \draw[blue, thick] (1.5,-2.7) -- (1.5,1.06) node[above left] {10.6}; \draw[blue, thick] (1.5,1.06) -- (3.267,0); % Zero point \draw[blue, thick] (3.267,0) -- (5,-1.04) node[below left] {$-10.4$}; \draw[blue, thick] (5,-1.04) -- (5,-5.04) node[below left] {$-50.4$}; \draw[blue, thick] (5,-5.04) -- (6.5,-5.04); \draw[blue, thick] (6.5,-5.04) -- (6.5,2.2) node[above left] {22}; \draw[blue, thick] (6.5,2.2) -- (9,2.2) -- (9,0); % X-axis for diagram \draw[dashed] (0,0) -- (9,0); % Y-axis for diagram \draw[dashed] (0,-6) -- (0,3); \end{tikzpicture}

    5.2 Calculate the coordinates of the centroid of the lamina shown in FIGURE 2.

    We will divide the lamina into simpler geometric shapes and use the principle of composite areas.
    Let's divide the shape into three rectangles:

    • Rectangle 1 (Vertical part on left):

      • Width = 40 mm40 \text{ mm}
      • Height = 80 mm80 \text{ mm}
      • Area A1=40×80=3200 mm2A_1 = 40 \times 80 = 3200 \text{ mm}^2
      • Centroid x1=402=20 mmx_1 = \frac{40}{2} = 20 \text{ mm}
      • Centroid y1=802=40 mmy_1 = \frac{80}{2} = 40 \text{ mm}
    • Rectangle 2 (Horizontal part on right):

      • Width = 100 mm−40 mm=60 mm100 \text{ mm} - 40 \text{ mm} = 60 \text{ mm}
      • Height = 40 mm40 \text{ mm}
      • Area A2=60×40=2400 mm2A_2 = 60 \times 40 = 2400 \text{ mm}^2
      • Centroid x2=40 mm+602=40+30=70 mmx_2 = 40 \text{ mm} + \frac{60}{2} = 40 + 30 = 70 \text{ mm}
      • Centroid y2=402=20 mmy_2 = \frac{40}{2} = 20 \text{ mm}
    • Rectangle 3 (Hole):

      • This is a cutout, so its area will be negative.
      • Width = 20 mm20 \text{ mm}
      • Height = 20 mm20 \text{ mm}
      • Area A3=−(20×20)=−400 mm2A_3 = -(20 \times 20) = -400 \text{ mm}^2
      • Centroid x3=20 mm+202=20+10=30 mmx_3 = 20 \text{ mm} + \frac{20}{2} = 20 + 10 = 30 \text{ mm}
      • Centroid y3=20 mm+202=20+10=30 mmy_3 = 20 \text{ mm} + \frac{20}{2} = 20 + 10 = 30 \text{ mm}
  4. Calculate the total area AtotalA_{total}.

    Atotal=A1+A2+A3A_{total} = A_1 + A_2 + A_3 Atotal=3200 mm2+2400 mm2−400 mm2A_{total} = 3200 \text{ mm}^2 + 2400 \text{ mm}^2 - 400 \text{ mm}^2 Atotal=5200 mm2A_{total} = 5200 \text{ mm}^2
  5. Calculate the x-coordinate of the centroid (xˉ\bar{x}).

    xˉ=A1x1+A2x2+A3x3Atotal\bar{x} = \frac{A_1 x_1 + A_2 x_2 + A_3 x_3}{A_{total}} xˉ=(3200×20)+(2400×70)+(−400×30)5200\bar{x} = \frac{(3200 \times 20) + (2400 \times 70) + (-400 \times 30)}{5200} xˉ=64000+168000−120005200\bar{x} = \frac{64000 + 168000 - 12000}{5200} xˉ=2200005200\bar{x} = \frac{220000}{5200} xˉ=220052=55013≈42.31 mm\bar{x} = \frac{2200}{52} = \frac{550}{13} \approx 42.31 \text{ mm}
  6. Calculate the y-coordinate of the centroid (yˉ\bar{y}).

    yˉ=A1y1+A2y2+A3y3Atotal\bar{y} = \frac{A_1 y_1 + A_2 y_2 + A_3 y_3}{A_{total}} yˉ=(3200×40)+(2400×20)+(−400×30)5200\bar{y} = \frac{(3200 \times 40) + (2400 \times 20) + (-400 \times 30)}{5200} yˉ=128000+48000−120005200\bar{y} = \frac{128000 + 48000 - 12000}{5200} yˉ=1640005200\bar{y} = \frac{164000}{5200} yˉ=164052=41013≈31.54 mm\bar{y} = \frac{1640}{52} = \frac{410}{13} \approx 31.54 \text{ mm}

    The coordinates of the centroid are:

    (xˉ,yˉ)=(42.31 mm,31.54 mm)\boxed{(\bar{x}, \bar{y}) = (42.31 \text{ mm}, 31.54 \text{ mm})}
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