Indeterminate Structures — Question 9

Section 12-5 · Physics pages 1868–1869

Question 9 An energy minimum recovers displacement compatibility Two linear springs of stiffnesses k1, k2 > 0 support the same load point with total load P. For this system the physical force sharing minimizes the complementary energy C = R2 1/(2k1) + R2 2/(2k2) subject to R1 + R2 = P. R1 C R∗ 1 unique minimum Complementary energy along the constraint R2 = P −R1 is strictly convex. (a) Derive the reactions by constrained minimization. (b) Show that the minimum is unique and interpret the stationary condition physically.
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Question 9 - Solution An energy minimum recovers displacement compatibility R1 C R∗ 1 unique minimum (a) Derivation and calculation Eliminate R2 = P −R1 to obtain C(R1) = R2 1 2k1 + (P −R1)2 2k2 . Stationarity requires dC dR1 = R1 k1 −P −R1 k2 = 0. Solving, R1 = Pk1 k1 + k2 , R2 = Pk2 k1 + k2 . (b) Result and interpretation The second derivative is everywhere positive: d2C dR2 1 = 1 k1 + 1 k2 > 0 . Therefore the stationary point is the unique minimum. Physically, R1 k1 = R2 k2 = P k1 + k2 = δ, which is the common load-point displacement required by compatibility. Physical check The stiffer spring carries the larger force, but both undergo the same displacement.

Question 9

An energy minimum recovers displacement compatibility

Two linear springs of stiffnesses k1,k2>0k_1,k_2>0 support the same load point with total load PP. For this system the physical force sharing minimizes the complementary energy C=R12/(2k1)+R22/(2k2)C=R_1^2/(2k_1)+R_2^2/(2k_2) subject to R1+R2=PR_1+R_2=P.

Diagram shown in the original SVG worksheet.

  1. Derive the reactions by constrained minimization.

  2. Show that the minimum is unique and interpret the stationary condition physically.

Question 9 - Solution

An energy minimum recovers displacement compatibility

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Eliminate R2=P−R1R_2=P-R_1 to obtain C(R1)=R122k1+(P−R1)22k2.C(R_1)=\frac{R_1^2}{2k_1}+\frac{(P-R_1)^2}{2k_2}. Stationarity requires dCdR1=R1k1−P−R1k2=0.\frac{dC}{dR_1}=\frac{R_1}{k_1}-\frac{P-R_1}{k_2}=0. Solving, R1=Pk1k1+k2,R2=Pk2k1+k2.\boxed{R_1=\frac{Pk_1}{k_1+k_2}},\qquad\boxed{R_2=\frac{Pk_2}{k_1+k_2}}.

(b) Result and interpretation

The second derivative is everywhere positive: d2CdR12=1k1+1k2>0.\boxed{\frac{d^2C}{dR_1^2}=\frac1{k_1}+\frac1{k_2}>0}. Therefore the stationary point is the unique minimum. Physically, R1k1=R2k2=Pk1+k2=δ,\frac{R_1}{k_1}=\frac{R_2}{k_2}=\frac{P}{k_1+k_2}=\delta, which is the common load-point displacement required by compatibility.

Physical check

The stiffer spring carries the larger force, but both undergo the same displacement.