Torque — Question 9

Section 10-7 · Physics pages 1508–1509

Question 9 A distributed load has a torque-weighted application point A horizontal beam from x = 0 to L carries a downward load density w(x) = w0x/L in N/m. Find moments about its left end. 0 L Downward arrows indicate a linearly increasing force per unit length. (a) Find the total downward force and torque. (b) Find the application point of an equivalent single downward force and explain why the midpoint is wrong.
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Question 9 - Solution A distributed load has a torque-weighted application point 0 L (a) Derivation and calculation Integrate the force density over the beam: F = ∫L 0 w0x L dx = w0L 2 downward. The signed moment weights each contribution by its distance: τz = − ∫L 0 xw0x L dx = −w0L2 3 . (b) Result and interpretation A single equivalent downward force must reproduce both results: −Fxeq = τz ⇒xeq = w0L2/3 w0L/2 = 2L 3 . The midpoint would give only −w0L2/4, so it would not reproduce the load’s moment. Physical check The equivalent point lies toward the more heavily loaded right end.

Question 9

A distributed load has a torque-weighted application point

A horizontal beam from x=0x=0 to LL carries a downward load density w(x)=w0x/Lw(x)=w_0x/L in N/m. Find moments about its left end.

Diagram shown in the original SVG worksheet.

  1. Find the total downward force and torque.

  2. Find the application point of an equivalent single downward force and explain why the midpoint is wrong.

Question 9 - Solution

A distributed load has a torque-weighted application point

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Integrate the force density over the beam: F=∫0Lw0xLdx=w0L2downward.\boxed{F=\int_0^L\frac{w_0x}{L}\,dx=\frac{w_0L}{2}}\quad\text{downward}. The signed moment weights each contribution by its distance: τz=−∫0Lxw0xLdx=−w0L23.\boxed{\tau_z=-\int_0^Lx\frac{w_0x}{L}\,dx=-\frac{w_0L^2}{3}}.

(b) Result and interpretation

A single equivalent downward force must reproduce both results: −Fxeq=τz⇒xeq=w0L2/3w0L/2=2L3.-Fx_{\mathrm{eq}}=\tau_z\Rightarrow \boxed{x_{\mathrm{eq}}=\frac{w_0L^2/3}{w_0L/2}=\frac{2L}{3}}. The midpoint would give only −w0L2/4-w_0L^2/4, so it would not reproduce the load’s moment.

Physical check

The equivalent point lies toward the more heavily loaded right end.