The Requirements of Equilibrium — Question 3

Section 12-2 · Physics pages 1796–1797

Question 3 A two-force member transmits force only along its endpoints A weightless member is acted on only at endpoints A = (0, 0) and B = (2, 1) m, with no end couples. The force at B has magnitude 10 N and points generally from A toward B. A B Schematic; labels, not drawing lengths, specify the data. (a) Find both endpoint forces required for equilibrium. (b) Could the force at B instead be purely vertical with nonzero magnitude?
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Question 3 - Solution A two-force member transmits force only along its endpoints A B (a) Derivation and calculation Force balance requires⃗FA = −⃗FB. About A,⃗ rAB ×⃗FB = 0,⃗ rAB = (2, 1) m. The stated direction selects⃗ FB = 102ˆx + ˆy √ 5 = (4 √ 5ˆx + 2 √ 5ˆy) N ,⃗ FA = −⃗FB . (b) Result and interpretation A nonzero purely vertical force at B would give τA = xBFBy −yBFBx = 2FBy̸ = 0. The force at A has no moment about A, so it cannot cancel this torque. A third force or an end couple would be needed. Physical check The calculated force has magnitude √80 + 20 = 10 N and zero moment because 2FBy −FBx = 0.

Question 3

A two-force member transmits force only along its endpoints

A weightless member is acted on only at endpoints A=(0,0)A=(0,0) and B=(2,1)mB=(2,1)\,\mathrm m, with no end couples. The force at BB has magnitude 10N10\,\mathrm N and points generally from AA toward BB.

Diagram shown in the original SVG worksheet.

  1. Find both endpoint forces required for equilibrium.

  2. Could the force at BB instead be purely vertical with nonzero magnitude?

Question 3 - Solution

A two-force member transmits force only along its endpoints

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Force balance requires F→A=−F→B\vec F_A=-\vec F_B. About AA, r→AB×F→B=0,r→AB=(2,1)m.\vec r_{AB}\times\vec F_B=0,\qquad \vec r_{AB}=(2,1)\ \mathrm m. The stated direction selects F→B=102x̂+ŷ5=(45x̂+25ŷ)N,\vec F_B=10\frac{2\hat x+\hat y}{\sqrt5} =\boxed{(4\sqrt5\hat x+2\sqrt5\hat y)\ \mathrm N}, F→A=−F→B.\boxed{\vec F_A=-\vec F_B}.

(b) Result and interpretation

A nonzero purely vertical force at BB would give τA=xBFBy−yBFBx=2FBy≠0.\tau_A=x_BF_{By}-y_BF_{Bx}=2F_{By}\ne0. The force at AA has no moment about AA, so it cannot cancel this torque. A third force or an end couple would be needed.

Physical check

The calculated force has magnitude 80+20=10\sqrt{80+20}=10 N and zero moment because 2FBy−FBx=02F_{By}-F_{Bx}=0.