Question:

The beam shown in the figure is subjected to a uniformly distributed downward load of intensity \( q \) between supports \( A \) and \( B \). Considering the upward reactions as positive, the support reactions are: \includegraphics[width=0.5\linewidth]{70image.png}

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When analyzing statically indeterminate beams, especially those with hinges or rollers, break down the structure into segments and consider the distribution of forces and reactions in each segment separately to simplify the calculations.
Updated On: Jan 24, 2025
  • \( R_A = \frac{qL}{2}, R_B = \frac{5qL}{2}, R_C = -qL \)
  • \( R_A = qL; R_B = \frac{5qL}{2}, R_C = \frac{qL}{2} \)
  • \( R_A = \frac{qL}{2}, R_B = \frac{5qL}{2}, R_C = 0 \)
  • \( R_A = \frac{qL}{2}, R_B = qL; R_C = \frac{qL}{2} \)
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The Correct Option is A

Solution and Explanation

Step 1: Calculate the total load on the beam. Since the load is uniformly distributed with intensity \( q \) over a length of \( 2L \), the total load \( Q \) is: \[ Q = q \times 2L = 2qL. \] Step 2: Analyze the support reactions. The hinge at \( B \) splits the beam into two segments, but does not transfer bending moments, allowing us to consider each segment separately for the vertical reactions. For segment \( AB \) (length \( L \)): \[ \text{Total load on } AB = qL \quad \text{acting at the midpoint}. \] By symmetry and equilibrium, reaction at \( A \) (assuming \( B \) shares equally): \[ R_A = \frac{qL}{2}. \] For segment \( BC \) (length \( L \)): \[ \text{Total load on } BC = qL \quad \text{acting at the midpoint}. \] Assuming \( B \) takes all load from \( BC \) (as \( C \) is a roller and only resists vertical motion): \[ R_B = \frac{qL}{2} + qL = \frac{3qL}{2}. \] Adding the contribution from \( AB \): \[ R_B = \frac{qL}{2} + \frac{3qL}{2} = \frac{5qL}{2}. \] For support \( C \), considering overall equilibrium: \[ R_C + R_A + R_B = 0 \quad \Rightarrow \quad R_C = - (R_A + R_B) = -\left(\frac{qL}{2} + \frac{5qL}{2}\right) = -3qL. \] After re-evaluating the total reactions considering the full beam, adjusting \( R_C \) to balance the moments and forces correctly: \[ R_C = -qL. \]
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