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Intermediate beam for office hall 16 m x 6 m

Short answer

Provide ISMB 300. Factored moment 137.3 kN·m < moment capacity 152.4 kN·m; shear 87.2 kN < 303.1 kN; deflection 10.27 mm < L/300 = 21 mm. Lateral stability is ensured because the compression flange is continuously supported by the slab.

An office hall measuring 16m x 6m consists of beams spaced at 3m c/c. RCC slab of 12cm is cast over the beam. The imposed load is 3kN/m². The beam is supported on 300mm wall. The compression flange is supported throughout its length. Design intermediate beam and check for shear, deflection and lateral stability.

Data

  • Steel Fe 410 (E250): fy=250f_y = 250 N/mm², fu=410f_u = 410 N/mm², E=2×105E = 2\times10^5 N/mm², γm0=1.10\gamma_{m0} = 1.10 (IS 800:2007, Table 5). Limit state design.
  • Effective span L=6.30L = 6.30 m, bearing length of support =300= 300 mm.

Loads and design forces

The hall is 6 m wide, so the beams span 6 m and are spaced 3 m c/c. With 300 mm wall bearing, effective span =6.0+0.3=6.3= 6.0 + 0.3 = 6.3 m. Unit weight of RCC =25= 25 kN/m³ (assumed); no floor finish is given.

  • Slab: 0.12×25=3.000.12\times25 = 3.00 kN/m², per metre of beam =3.00×3=9.00= 3.00\times3 = 9.00 kN/m
  • Imposed load: 3×3=9.003\times3 = 9.00 kN/m

Factored load wu=1.5(9.00+9.00)=27.00w_u = 1.5(9.00 + 9.00) = 27.00 kN/m (plus self-weight).

Moment without self-weight M=134.0M = 134.0 kN·m, so Zp,req≈Mγm0/fy=134.0×106×1.1/250=589Z_{p,req} \approx M\gamma_{m0}/f_y = 134.0\times10^6\times1.1/250 = 589 cm³ (self-weight adds a little).

Trial section

Try 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, R1=14R_1 = 14 mm; Izz=8990I_{zz} = 8990 cm⁴; Ze=599Z_e = 599 cm³; Zp≈Btf(D−tf)+tw(D−2tf)2/4=670Z_p \approx B t_f (D - t_f) + t_w (D - 2t_f)^2/4 = 670 cm³; mass 46.046.0 kg/m.

Self-weight =46.0×9.81/1000=0.451= 46.0\times9.81/1000 = 0.451 kN/m, factored =1.5×0.451=0.677= 1.5\times0.451 = 0.677 kN/m. Total factored UDL w=27.00+0.68=27.68w = 27.00 + 0.68 = 27.68 kN/m.

Mu=wL28=27.68×6.3028=137.3 kN⋅mVu=wL2=87.2 kN\begin{aligned} M_u &= \frac{wL^2}{8} = \frac{27.68\times6.30^2}{8} = 137.3\ \text{kN·m} \\ V_u &= \frac{wL}{2} = 87.2\ \text{kN} \end{aligned}

Section classification (Table 2)

ε=250/fy=1.00\varepsilon = \sqrt{250/f_y} = 1.00. Flange: b/tf=(140/2)/13.1=5.34<9.4ε=9.4b/t_f = (140/2)/13.1 = 5.34 < 9.4\varepsilon = 9.4. Web: d/tw=31.9<84ε=84d/t_w = 31.9 < 84\varepsilon = 84 (with d=D−2(tf+R1)=245.8d = D - 2(t_f + R_1) = 245.8 mm). The section is plastic, so βb=1.0\beta_b = 1.0.

Moment capacity (cl. 8.2.1.2)

The compression flange is supported throughout its length by the slab, so lateral buckling is prevented (cl. 8.2.2); this is the check for lateral stability.

Md=βbZpfyγm0=670×103×2501.1×106=152.4 kN⋅m1.2Zefy/γm0=1.2×599×103×250/(1.1×106)=163.4 kN⋅m\begin{aligned} M_d &= \frac{\beta_b Z_p f_y}{\gamma_{m0}} = \frac{670\times10^3\times250}{1.1\times10^6} = 152.4\ \text{kN·m} \\ 1.2 Z_e f_y/\gamma_{m0} &= 1.2\times599\times10^3\times250/(1.1\times10^6) = 163.4\ \text{kN·m} \end{aligned}

The smaller value governs: Md=152.4M_d = 152.4 kN·m.

Md=152.4 kN⋅m>Mu=137.3 kN⋅mSafeM_d = 152.4\ \text{kN·m} > M_u = 137.3\ \text{kN·m}\quad \text{Safe}

Shear capacity (cl. 8.4)

Av=Dtw=300×7.7=2310 mm2Vd=Avfy3 γm0=2310×2503×1.1×103=303.1 kN\begin{aligned} A_v &= D t_w = 300\times7.7 = 2310\ \text{mm}^2 \\ V_d &= \frac{A_v f_y}{\sqrt3\,\gamma_{m0}} = \frac{2310\times250}{\sqrt3\times1.1\times10^3} = 303.1\ \text{kN} \end{aligned}

Vu=87.2V_u = 87.2 kN <Vd< V_d; also Vu<0.6Vd=181.9V_u < 0.6V_d = 181.9 kN, so the shear is low and the moment capacity is not reduced (cl. 9.2.1). Web shear buckling does not govern since d/tw=31.9<67ε=67d/t_w = 31.9 < 67\varepsilon = 67 (cl. 8.4.2.1).

Deflection (Table 6)

Deflection under unfactored service (imposed) loads, limit span/300 (floor and roof members, Table 6):

δ=5wL4384EI=5×9.00×(6300)4384×2×105×8990×104=10.27 mm\delta = \frac{5 w L^4}{384 E I} = \frac{5\times9.00\times(6300)^4}{384\times2\times10^5\times8990\times10^4} = 10.27\ \text{mm}

δ=10.27\delta = 10.27 mm <L/300=21.00< L/300 = 21.00 mm. OK.

Web buckling and bearing at support (cl. 8.7.3 and 8.7.4)

Stiff bearing length b1=300b_1 = 300 mm. Clear web depth d=245.8d = 245.8 mm; dispersion of load at 45° to mid-depth at an end support n1=d/2=122.9n_1 = d/2 = 122.9 mm. Effective length 0.7d0.7d (cl. 8.7.1.5), λ=0.7d/(tw/12)=77.4\lambda = 0.7d/(t_w/\sqrt{12}) = 77.4; curve c gives fcd=140.4f_{cd} = 140.4 N/mm².

Fcdw=(b1+n1)twfcd=(300+122.9)×7.7×140.4/103=457.1 kNn2=2.5(tf+R1)=67.8 mmFw=(b1+n2)twfyγm0=(300+67.8)×7.7×2501.1×103=643.6 kN\begin{aligned} F_{cdw} &= (b_1 + n_1) t_w f_{cd} = (300 + 122.9)\times7.7\times140.4/10^3 = 457.1\ \text{kN} \\ n_2 &= 2.5(t_f + R_1) = 67.8\ \text{mm} \\ F_w &= \frac{(b_1 + n_2) t_w f_y}{\gamma_{m0}} = \frac{(300 + 67.8)\times7.7\times250}{1.1\times10^3} = 643.6\ \text{kN} \end{aligned}

Support reaction R=87.2R = 87.2 kN <Fcdw< F_{cdw} and <Fw< F_w. No web stiffener is needed.

Final design

Provide ISMB 300 (46.0 kg/m): Md=152.4M_d = 152.4 kN·m >Mu=137.3> M_u = 137.3 kN·m, Vd=303V_d = 303 kN >Vu=87.2> V_u = 87.2 kN, δ=10.3\delta = 10.3 mm <21.0< 21.0 mm.

✓ Answer checked by Claude Opus 5.5 (high effort)

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