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Strain energy method for frame displacement

Short answer

Castigliano’s theorem including bending and axial strain energy gives vertical displacement ≈ 23.26 m downward (bending integral 45.667 m³, bending dominates; axial contributes only 0.32 mm). Load is very heavy for the 100 mm rod.

Use the strain energy method for the given frame to calculate the vertical displacement of the point with load 500 kN. The frame is made of steel rod of diameter 100 mm. Take E=2×105 N/mm2E = 2\times10^5\ \text{N/mm}^2. [Figure: frame fixed at joint 0; member 0-1 horizontal, 3 m; member 1-2 vertical, 1 m; member 2-3 horizontal, 2 m, with 500 kN acting downward at joint 3; a steel bar of diameter 100 mm runs from joint 0 to the lower member.]

Given data and assumptions

Frame fixed at joint 0, all members of solid circular section d=100d = 100 mm, E=2×105E = 2\times10^5 N/mm2^2 (=2×108= 2\times10^8 kN/m2^2). Taking the figure as a cantilever frame with horizontal member 0-1 (3 m), vertical member 1-2 (1 m) and horizontal member 2-3 (2 m), the 500 kN load PP acts downward at joint 3. Shear energy is neglected (small for slender members; GG is not given). Vertical displacement of joint 3 is found by Castigliano's theorem: δ3=∂U/∂P\delta_3 = \partial U/\partial P.

I=πd464=4.9087e−06 m4,EI=981.7 kNm2,A=0.00785 m2,AE=1.5708e+06 kNI = \frac{\pi d^4}{64} = 4.9087e-06\ \text{m}^4,\quad EI = 981.7\ \text{kNm}^2,\quad A = 0.00785\ \text{m}^2,\quad AE = 1.5708e+06\ \text{kN}

Internal forces (s measured from joint 3)

MemberLengthBending moment MMAxial force NN
3-2 (horizontal)2 mPsPs0
2-1 (vertical)1 m2P2P (constant)PP (compression)
1-0 (horizontal)3 mP(2+s)P(2+s)0

Strain energy and displacement

U=∫M22EIdx+∫N22AEdxU = \int\frac{M^2}{2EI}dx + \int\frac{N^2}{2AE}dx δ3=∂U∂P=PEI[∫02s2ds+(2)2(1)+∫03(2+s)2ds]+PL2−1AE\delta_3 = \frac{\partial U}{\partial P} = \frac{P}{EI}\left[\int_0^2 s^2ds + (2)^2(1) + \int_0^3 (2+s)^2 ds\right] + \frac{PL_{2-1}}{AE} ∫02s2ds=2.667,22×1=4,∫03(2+s)2ds=53−233=39\int_0^2 s^2ds = 2.667,\qquad 2^2\times1 = 4,\qquad \int_0^3(2+s)^2ds = \frac{5^3-2^3}{3} = 39 δbending=500×(2.667+4+39)981.7=500×45.667981.7=23.258 m\delta_{bending} = \frac{500\times(2.667+4+39)}{981.7} = \frac{500\times45.667}{981.7} = 23.258\ \text{m} δaxial=500×11.5708e+06=0.318 mm\delta_{axial} = \frac{500\times1}{1.5708e+06} = 0.318\ \text{mm}

Answer: vertical displacement of the loaded joint ≈23.26\approx 23.26 m downward (bending governs; axial part is only 0.32 mm). The very large value shows that the given load is extremely heavy for a 100 mm rod; the small-deflection theory is used as asked.

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