The problem describes a simply supported beam of span L. The load is distributed such that the first half of the span (0 to L/2) has a total weight W, and the second half (L/2 to L) has a total weight 2W. We need to find the maximum shear force.
First, let's determine the intensity of the distributed loads:
The total load on the beam is $W_{total} = W + 2W = 3W$. Let the reactions at the supports A (left) and B (right) be $R_A$ and $R_B$, respectively.
Using the principle of moments about support A:
$ R_B \times L = \left(W \times \frac{L}{4}\right) + \left(2W \times \frac{3L}{4}\right) $
The term $W \times \frac{L}{4}$ represents the moment due to the load W (whose centroid is at L/4). The term $2W \times \frac{3L}{4}$ represents the moment due to the load 2W (whose centroid is at L/2 + L/4 = 3L/4).
$ R_B \times L = \frac{WL}{4} + \frac{6WL}{4} = \frac{7WL}{4} $
$ R_B = \frac{7W}{4} = 1.75W $
Now, using the equilibrium equation for vertical forces ($\sum F_y = 0$):
$ R_A + R_B = W_{total} $
$ R_A + 1.75W = 3W $
$ R_A = 3W - 1.75W = 1.25W $
The shear force $V(x)$ is calculated as follows:
The shear forces at critical points are:
The maximum absolute shear force is the largest magnitude among these values:
$ \text{Max Shear Force} = \max(|1.25W|, |0.25W|, |-1.75W|) = 1.75W $
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