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UDL capacity of MB 300 with flange plates

Short answer

Plastic design per IS 800:2007. Shear capacity of the ISMB 300 web governs; moment capacity under high shear is adequate. The factored uniformly distributed load capacity is 173 kN/m (including self-weight).

Determine uniformly distributed load carrying capacity of a laterally restrained built-up beam having MB 300 and two plates 200 mm×12 mm. Effective length of beam is 3.5 m.

Approach. Plastic design strength of the built-up section (IS 800:2007 cl. 8.2.1), then reduction of moment capacity under high shear (cl. 9.2), and the load found from the governing check. fy=250f_y = 250 N/mm², γm0=1.10\gamma_{m0} = 1.10. The beam is laterally restrained, so lateral-torsional buckling is ignored. Plates are assumed fully connected to the flanges (continuous welds or adequate bolts), one 200×12 plate on each flange. Effective span L=3.5L = 3.5 m.

Section properties

ISMB 300 (IS 808): D=300D = 300 mm, bf=140b_f = 140 mm, tw=7.7t_w = 7.7 mm, tf=13.1t_f = 13.1 mm, Izz=8990I_{zz} = 8990 cm⁴, mass 46.0 kg/m. Plastic modulus of ISMB 300 from its dimensions: Zp,I=670Z_{p,I} = 670 cm³.

Overall depth=300+2×12=324 mmyc=150+6=156 mm (plate centroid from N.A.)Izz=8990×104+2[200×12312+200×12×1562]=20677 cm4Ze=Izz162=1276 cm3Zp=Zp,I+2(200×12)(156)=670+749=1419 cm3\begin{aligned} \text{Overall depth} &= 300 + 2\times12 = 324\ \text{mm} \\ y_c &= 150 + 6 = 156\ \text{mm (plate centroid from N.A.)} \\ I_{zz} &= 8990\times10^4 + 2\left[\frac{200\times12^3}{12} + 200\times12\times156^2\right] = 20677\ \text{cm}^4 \\ Z_e &= \frac{I_{zz}}{162} = 1276\ \text{cm}^3 \\ Z_p &= Z_{p,I} + 2(200\times12)(156) = 670 + 749 = 1419\ \text{cm}^3 \end{aligned}

Classification: plate outstand from the web face =(200−7.7)/2=96.2= (200 - 7.7)/2 = 96.2 mm, b/t=96.2/12=8.0<9.4ε=9.4b/t = 96.2/12 = 8.0 < 9.4\varepsilon = 9.4 (plastic); ISMB web d/tw=31.9<84d/t_w = 31.9 < 84. So βb=1\beta_b = 1.

Moment capacity

Md=Zpfyγm0=1419×103×2501.1×106=322.6 kN⋅m1.2Zefy/γm0=348.1 kN⋅m\begin{aligned} M_d &= \frac{Z_pf_y}{\gamma_{m0}} = \frac{1419\times10^3\times250}{1.1\times10^6} = 322.6\ \text{kN·m} \\ 1.2Z_ef_y/\gamma_{m0} &= 348.1\ \text{kN·m} \end{aligned}

Md=322.6M_d = 322.6 kN·m. Load limited by moment: w=8Md/L2=8×322.6/3.52=210.7w = 8M_d/L^2 = 8\times322.6/3.5^2 = 210.7 kN/m.

Shear capacity

Shear is resisted by the web of the rolled section: Av=Dtw=300×7.7=2310A_v = D t_w = 300\times7.7 = 2310 mm² (plates ignored, conservative).

Vd=Avfy3γm0=2310×2503×1.1×103=303.1 kNV_d = \frac{A_vf_y}{\sqrt3\gamma_{m0}} = \frac{2310\times250}{\sqrt3\times1.1\times10^3} = 303.1\ \text{kN}

Load limited by shear: w=2Vd/L=2×303.1/3.5=173.2w = 2V_d/L = 2\times303.1/3.5 = 173.2 kN/m. Shear governs (173.2 < 210.7).

Moment capacity under high shear (cl. 9.2.2)

At w=173.2w = 173.2 kN/m: V=Vd=303.1V = V_d = 303.1 kN >0.6Vd> 0.6V_d, so the moment capacity is reduced. MfdM_{fd} is the plastic strength of the section without the shear area: Zfd=Zp−twD2/4=1419−173=1246Z_{fd} = Z_p - t_wD^2/4 = 1419 - 173 = 1246 cm³, Mfd=283.2M_{fd} = 283.2 kN·m.

β=(2VVd−1)2=1.00Mdv=Md−β(Md−Mfd)=322.6−1.00(322.6−283.2)=283.2 kN⋅m\begin{aligned} \beta &= \left(\frac{2V}{V_d} - 1\right)^2 = 1.00 \\ M_{dv} &= M_d - \beta(M_d - M_{fd}) = 322.6 - 1.00(322.6 - 283.2) = 283.2\ \text{kN·m} \end{aligned}

Moment at this load =wL2/8=173.2×3.52/8=265.2= wL^2/8 = 173.2\times3.5^2/8 = 265.2 kN·m <Mdv=283.2< M_{dv} = 283.2 kN·m. OK.

Result

Self-weight =(46.0+2×0.2×0.012×7850)×9.81/1000=0.82= (46.0 + 2\times0.2\times0.012\times7850)\times9.81/1000 = 0.82 kN/m.

Answer: the safe factored uniformly distributed load is ≈173\approx 173 kN/m (including self-weight; governed by shear), i.e. a service load of ≈115\approx 115 kN/m, or about 172 kN/m factored superimposed load after deducting the factored self-weight of 1.23 kN/m. Total factored reaction =303= 303 kN.

✓ Answer checked by Claude Opus 5.5 (high effort)

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