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Calculate the coordinates of the centroid of the lamina shown in FIGURE 2.
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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 over a length of .
The total force from the UDL is .
This force acts at the centroid of the UDL, which is from point A.
Let's define the positions of all forces and supports from point A (left end of the beam):
- Point A: (18 kN downward force)
- Support B: (Reaction upward)
- UDL equivalent force: (30 kN downward force)
- Point C: (40 kN downward force)
- Support D: (Reaction upward)
- Point E: (22 kN downward force)
Apply the equilibrium equation for the sum of vertical forces.
Assume upward forces are positive.
Apply the equilibrium equation for the sum of moments about support B.
Assume clockwise moments are positive.
The moment arms are calculated relative to point B ().
Substitute the value of into Equation (1) to find .
The reaction forces are:
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).
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At A (): (downward force)
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Just before B (): The UDL acts from to . Shear force due to UDL up to B = .
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Just after B ():
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Just before C (): Shear force from B to C due to UDL = .
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Just after C ():
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Just before D (): There are no distributed loads or point loads between C and D.
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Just after D ():
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At E (): There are no distributed loads or point loads between D and E. (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 to .
- At B, it jumps up to .
- From B to C, it decreases linearly from to .
- At C, it jumps down to .
- From C to D, it remains constant at .
- At D, it jumps up to .
- From D to E, it remains constant at and then drops to 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 be the distance from B where shear force is zero.
from B.
This corresponds to 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 =
- Height =
- Area
- Centroid
- Centroid
-
Rectangle 2 (Horizontal part on right):
- Width =
- Height =
- Area
- Centroid
- Centroid
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Rectangle 3 (Hole):
- This is a cutout, so its area will be negative.
- Width =
- Height =
- Area
- Centroid
- Centroid
Calculate the total area .
Calculate the x-coordinate of the centroid ().
Calculate the y-coordinate of the centroid ().
The coordinates of the centroid are:
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