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Tubular column load and eccentric loading

Short answer

Using I=1.187×10^6 mm^4, k=25.6 mm: hinged-hinged λ=117, Pcr=π²EI/L²=260.4 kN; fixed-free λ=234, Pcr=65.1 kN. Eccentric short column: σmax=P/A+Pe/Z=10.45 MPa, σmin=0.21 MPa; no-tension limit e≤h/6=41.7 mm.

(a) A hollow circular steel tube of 80 mm outside diameter and 64 mm inside diameter, 3 m long, is used as a column. E = 200 GPa. Find the Euler crippling load and the slenderness ratio when (i) both ends are hinged and (ii) one end is fixed and the other free. (b) A short column of rectangular section 150 mm x 250 mm carries a compressive load of 200 kN with an eccentricity of 40 mm measured along the 250 mm side. Find the maximum and minimum stresses at the base, and state the limit of eccentricity for no tension.

(a) Euler load for the tube

I=π64(804−644)=1.187×106 mm4I = \frac{\pi}{64}(80^4 - 64^4) = 1.187\times10^6\ \text{mm}^4 A=π4(802−642)=1809.6 mm2,k=IA=25.6 mmA = \frac{\pi}{4}(80^2 - 64^2) = 1809.6\ \text{mm}^2, \qquad k = \sqrt{\frac IA} = 25.6\ \text{mm}
End conditionLeL_e (mm)λ=Le/k\lambda = L_e/kPcr=π2EILe2P_{cr} = \dfrac{\pi^2EI}{L_e^2}
(i) Hinged-hinged3000117π2×200000×1.187×10630002=260.4\dfrac{\pi^2\times200000\times1.187\times10^6}{3000^2} = 260.4 kN
(ii) Fixed-free6000234π2×200000×1.187×10660002=65.1\dfrac{\pi^2\times200000\times1.187\times10^6}{6000^2} = 65.1 kN

The crippling load of the fixed-free column is one quarter of that of the hinged column. The Euler stresses are 143.9143.9 MPa and 36.036.0 MPa, both below the yield stress and consistent with λ>100\lambda>100, so Euler's formula is applicable.

(b) Eccentrically loaded short column

Eccentricity is along the 250 mm side (h=250h = 250 mm, b=150b = 150 mm).

A=150×250=37 500 mm2,Z=bh26=150×25026=1.5625×106 mm3A = 150\times250 = 37\,500\ \text{mm}^2, \qquad Z = \frac{bh^2}{6} = \frac{150\times250^2}{6} = 1.5625\times10^6\ \text{mm}^3 σ0=PA=200×10337500=5.33 MPa\sigma_0 = \frac PA = \frac{200\times10^3}{37500} = 5.33\ \text{MPa} σb=PeZ=200×103×401.5625×106=5.12 MPa\sigma_b = \frac{Pe}{Z} = \frac{200\times10^3\times40}{1.5625\times10^6} = 5.12\ \text{MPa} σmax=5.33+5.12=10.45 MPa (compressive),σmin=5.33−5.12=0.21 MPa (compressive)\sigma_{max} = 5.33 + 5.12 = 10.45\ \text{MPa (compressive)}, \qquad \sigma_{min} = 5.33 - 5.12 = 0.21\ \text{MPa (compressive)}

No tension if σmin≥0\sigma_{min} \ge 0:

PA≥PeZ  ⇒  e≤ZA=h6=41.7 mm\frac{P}{A}\ge\frac{Pe}{Z} \;\Rightarrow\; e\le\frac ZA = \frac h6 = 41.7\ \text{mm}

The load must lie within the middle third of the depth (the core, kernel). Here e=40<41.7e = 40 < 41.7 mm, so there is no tension.

Answer: (a) Pcr=260.4P_{cr} = 260.4 kN (λ=117\lambda=117) and 65.165.1 kN (λ=234\lambda=234); (b) σmax=10.45\sigma_{max} = 10.45 MPa, σmin=0.21\sigma_{min} = 0.21 MPa, limit e=h/6=41.7e = h/6 = 41.7 mm.

✓ Answer checked by Claude Opus 5.5 (high effort)

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