Difficulty: Easy
Correct Answer: Correct
Explanation:
Introduction / Context:
In strength of materials, understanding how shear force varies along a beam under specific loads is fundamental. A simply supported beam with a central point load is a classic case used to teach sign conventions and the relationship between loads, shear force, and bending moment.
Given Data / Assumptions:
Concept / Approach:
Shear force V(x) is the algebraic sum of vertical forces to the left or right of a section. For a point load, V has a jump (discontinuity) at the load location. With the load at mid-span, the shear changes from positive to negative (or vice versa depending on sign convention) at that exact point.
Step-by-Step Solution:
Take sections to the left of mid-span: V_left = +P/2 (upward reaction).Take sections immediately to the right of the point load: V_right = +P/2 − P = −P/2.The sudden change from +P/2 to −P/2 at mid-span shows a sign change in V(x).Bending moment is maximum where shear crosses zero; here it occurs at mid-span, consistent with theory.
Verification / Alternative check:
The bending moment diagram is triangular on each half with peak M_max = (P/2)(L/2) = PL/4 at mid-span. Maximum moment coincides with V = 0, confirming the shear sign change at the center.
Why Other Options Are Wrong:
“It changes sign only at the supports” is false; supports are reaction points, not zero-shear locations for this load case. “It never changes sign for a point load” contradicts the jump at the load. “Depends on beam material only” is incorrect; material does not affect static equilibrium of internal forces.
Common Pitfalls:
Mixing sign conventions; forgetting that a concentrated load introduces a shear force jump; assuming zero shear only for distributed loads.
Final Answer:
Correct
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