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Section A: Long Answer Questions

Attempt all questions.

5 questions
1long12 marks

A single-bolted-line lap joint connects two plates, each 12 mm12\ \text{mm} thick, carrying a factored axial tensile force of Tu=180 kNT_u = 180\ \text{kN}. Use M20 bolts of property class 4.6 in 22 mm22\ \text{mm} diameter holes. Steel grade is Fe410 (fy=250 MPaf_y = 250\ \text{MPa}, fu=410 MPaf_u = 410\ \text{MPa}). The bolts are in a single shear plane with threads in the shear plane.

(a) Determine the design shear and bearing strength of one M20 bolt and hence the number of bolts required (use γmb=1.25\gamma_{mb}=1.25).
(b) For an edge distance of 33 mm33\ \text{mm} and pitch of 50 mm50\ \text{mm}, determine the design tensile strength of the plate considering gross-section yielding and net-section rupture, and check adequacy. Take plate width =120 mm= 120\ \text{mm} with bolts in a single line. (Use LSM as per IS 800:2007.)

Given: Tu=180 kNT_u=180\ \text{kN}, plate 12 mm×120 mm12\ \text{mm}\times120\ \text{mm}, M20 (4.6), hole d0=22 mmd_0=22\ \text{mm}, fub=400 MPaf_{ub}=400\ \text{MPa}, fu=410 MPaf_u=410\ \text{MPa}, fy=250 MPaf_y=250\ \text{MPa}, γmb=1.25\gamma_{mb}=1.25, γm0=1.10\gamma_{m0}=1.10, γm1=1.25\gamma_{m1}=1.25.

(a) Bolt shear strength (single shear, nn=1n_n=1, ns=0n_s=0):

Anb=0.78π4d2=0.78×π4×202=245.0 mm2A_{nb}=0.78\cdot\frac{\pi}{4}\,d^2=0.78\times\frac{\pi}{4}\times20^2=245.0\ \text{mm}^2 Vdsb=fub3γmbAnb=4003×1.25×245.0=400×245.02.1651=45.26×103 N=45.26 kNV_{dsb}=\frac{f_{ub}}{\sqrt3\,\gamma_{mb}}\,A_{nb}=\frac{400}{\sqrt3\times1.25}\times245.0=\frac{400\times245.0}{2.1651}=45.26\times10^3\ \text{N}=45.26\ \text{kN}

Bearing strength: edge e=33e=33, pitch p=50p=50, d0=22d_0=22.

kb=min(e3d0, p3d00.25, fubfu, 1.0)k_b=\min\left(\frac{e}{3d_0},\ \frac{p}{3d_0}-0.25,\ \frac{f_{ub}}{f_u},\ 1.0\right) e3d0=3366=0.500,p3d00.25=50660.25=0.7580.25=0.508,\frac{e}{3d_0}=\frac{33}{66}=0.500,\quad \frac{p}{3d_0}-0.25=\frac{50}{66}-0.25=0.758-0.25=0.508, fubfu=400410=0.976,kb=0.500\frac{f_{ub}}{f_u}=\frac{400}{410}=0.976,\quad \Rightarrow k_b=0.500 Vdpb=2.5kbdtfuγmb=2.5×0.500×20×12×4101.25=1230001.25=98.40×103 N=98.40 kNV_{dpb}=\frac{2.5\,k_b\,d\,t\,f_u}{\gamma_{mb}}=\frac{2.5\times0.500\times20\times12\times410}{1.25}=\frac{123000}{1.25}=98.40\times10^3\ \text{N}=98.40\ \text{kN}

Governing bolt value =min(45.26, 98.40)=45.26 kN=\min(45.26,\ 98.40)=\mathbf{45.26\ kN} (shear governs).

Number of bolts: n=TuVdb=18045.26=3.984 boltsn=\dfrac{T_u}{V_{db}}=\dfrac{180}{45.26}=3.98\Rightarrow \mathbf{4\ bolts}.

(b) Plate tension strength:

Gross-section yielding:

Tdg=Agfyγm0=(120×12)×2501.10=1440×2501.10=327.3×103 N=327.3 kNT_{dg}=\frac{A_g\,f_y}{\gamma_{m0}}=\frac{(120\times12)\times250}{1.10}=\frac{1440\times250}{1.10}=327.3\times10^3\ \text{N}=327.3\ \text{kN}

Net-section rupture (one hole in critical section, single line):

An=(bd0)t=(12022)×12=98×12=1176 mm2A_n=(b-d_0)\,t=(120-22)\times12=98\times12=1176\ \text{mm}^2 Tdn=0.9Anfuγm1=0.9×1176×4101.25=4339441.25=347.2×103 N=347.2 kNT_{dn}=\frac{0.9\,A_n\,f_u}{\gamma_{m1}}=\frac{0.9\times1176\times410}{1.25}=\frac{433944}{1.25}=347.2\times10^3\ \text{N}=347.2\ \text{kN}

Design tensile strength =min(327.3, 347.2)=327.3 kN=\min(327.3,\ 347.2)=\mathbf{327.3\ kN}.

Since 327.3 kN>180 kN327.3\ \text{kN}>180\ \text{kN}, the plate is adequate and gross-section yielding governs. Use 4 M20 bolts.

bolted-connectiontension-memberlimit-state
2long12 marks

A column of effective length 4.0 m4.0\ \text{m} (both ends pinned) is to carry a factored axial compressive load of 1100 kN1100\ \text{kN}. A rolled steel section ISHB 250 @ 510.6 N/m is proposed with the following properties: A=6971 mm2A = 6971\ \text{mm}^2, rzz=108.5 mmr_{zz}=108.5\ \text{mm}, ryy=53.4 mmr_{yy}=53.4\ \text{mm}. Steel is Fe410, fy=250 MPaf_y=250\ \text{MPa}. Using IS 800:2007 (buckling class 'c' about the weaker axis, imperfection factor α=0.49\alpha=0.49, γm0=1.10\gamma_{m0}=1.10), determine the design compressive strength of the column and check its adequacy.

Given: Le=4000 mmL_e=4000\ \text{mm}, A=6971 mm2A=6971\ \text{mm}^2, rmin=ryy=53.4 mmr_{min}=r_{yy}=53.4\ \text{mm}, fy=250 MPaf_y=250\ \text{MPa}, α=0.49\alpha=0.49, γm0=1.10\gamma_{m0}=1.10, E=2×105 MPaE=2\times10^5\ \text{MPa}.

Step 1 — Slenderness ratio:

λslen=Lermin=400053.4=74.9\lambda_{slen}=\frac{L_e}{r_{min}}=\frac{4000}{53.4}=74.9

Step 2 — Euler (elastic critical) stress:

fcc=π2Eλslen2=π2×2×10574.92=1.9739×1065610.0=351.9 MPaf_{cc}=\frac{\pi^2 E}{\lambda_{slen}^2}=\frac{\pi^2\times2\times10^5}{74.9^2}=\frac{1.9739\times10^6}{5610.0}=351.9\ \text{MPa}

Step 3 — Non-dimensional slenderness:

λˉ=fyfcc=250351.9=0.7104=0.843\bar\lambda=\sqrt{\frac{f_y}{f_{cc}}}=\sqrt{\frac{250}{351.9}}=\sqrt{0.7104}=0.843

Step 4 — Factor ϕ\phi:

ϕ=0.5[1+α(λˉ0.2)+λˉ2]=0.5[1+0.49(0.8430.2)+0.8432]\phi=0.5\left[1+\alpha(\bar\lambda-0.2)+\bar\lambda^2\right]=0.5\left[1+0.49(0.843-0.2)+0.843^2\right] =0.5[1+0.49(0.643)+0.7106]=0.5[1+0.3151+0.7106]=0.5×2.0257=1.0129=0.5\left[1+0.49(0.643)+0.7106\right]=0.5[1+0.3151+0.7106]=0.5\times2.0257=1.0129

Step 5 — Stress reduction factor χ\chi:

χ=1ϕ+ϕ2λˉ2=11.0129+1.012920.7106=11.0129+1.02600.7106\chi=\frac{1}{\phi+\sqrt{\phi^2-\bar\lambda^2}}=\frac{1}{1.0129+\sqrt{1.0129^2-0.7106}}=\frac{1}{1.0129+\sqrt{1.0260-0.7106}} =11.0129+0.3154=11.0129+0.5616=11.5745=0.6351=\frac{1}{1.0129+\sqrt{0.3154}}=\frac{1}{1.0129+0.5616}=\frac{1}{1.5745}=0.6351

Step 6 — Design compressive stress:

fcd=χfyγm0=0.6351×2501.10=158.781.10=144.3 MPaf_{cd}=\frac{\chi\,f_y}{\gamma_{m0}}=\frac{0.6351\times250}{1.10}=\frac{158.78}{1.10}=144.3\ \text{MPa}

Step 7 — Design compressive strength:

Pd=Afcd=6971×144.3=1.006×106 N=1006 kNP_d=A\,f_{cd}=6971\times144.3=1.006\times10^6\ \text{N}=\mathbf{1006\ kN}

Check: Pd=1006 kN<1100 kNP_d=1006\ \text{kN} < 1100\ \text{kN} applied.

The section is NOT adequate (capacity is about 9% short). A heavier section (e.g. ISHB 300) should be adopted. This illustrates the design-check verdict: when Pd<PuP_d < P_u, the trial section must be revised.

compression-memberbucklingcolumn-design
3long12 marks

A simply supported steel beam of span 6 m6\ \text{m} carries a factored uniformly distributed load of 40 kN/m40\ \text{kN/m} (inclusive of self-weight) over its full span. The compression flange is fully laterally restrained. Steel is Fe410, fy=250 MPaf_y=250\ \text{MPa}, γm0=1.10\gamma_{m0}=1.10.

(a) Determine the maximum factored bending moment and shear force.
(b) Select a suitable plastic-section ISMB and verify its design bending strength (assume a plastic section, βb=1.0\beta_b=1.0). For trial, ISMB 400 has Zp=1176.18×103 mm3Z_p = 1176.18\times10^3\ \text{mm}^3, Ze=1020.0×103 mm3Z_e = 1020.0\times10^3\ \text{mm}^3, depth D=400 mmD=400\ \text{mm}, web thickness tw=8.9 mmt_w=8.9\ \text{mm}.
(c) Check the design shear strength.

Given: L=6 mL=6\ \text{m}, wu=40 kN/mw_u=40\ \text{kN/m}, laterally restrained, fy=250 MPaf_y=250\ \text{MPa}, γm0=1.10\gamma_{m0}=1.10.

(a) Design forces:

Mu=wuL28=40×628=40×368=180 kN\cdotpmM_u=\frac{w_u L^2}{8}=\frac{40\times6^2}{8}=\frac{40\times36}{8}=180\ \text{kN·m} Vu=wuL2=40×62=120 kNV_u=\frac{w_u L}{2}=\frac{40\times6}{2}=120\ \text{kN}

(b) Bending strength of ISMB 400 (plastic section, laterally restrained \Rightarrow no LTB):

Md=βbZpfyγm0=1.0×1176.18×103×2501.10=294.045×1061.10=267.3×106 N\cdotpmm=267.3 kN\cdotpmM_d=\frac{\beta_b\,Z_p\,f_y}{\gamma_{m0}}=\frac{1.0\times1176.18\times10^3\times250}{1.10}=\frac{294.045\times10^6}{1.10}=267.3\times10^6\ \text{N·mm}=267.3\ \text{kN·m}

Limit to avoid excessive deformation (simply supported): 1.2Zefy/γm01.2\,Z_e f_y/\gamma_{m0}:

1.2×1020.0×103×2501.10=1.2×231.8=278.2 kN\cdotpm>267.3 kN\cdotpm (OK, governing Md=267.3)1.2\times\frac{1020.0\times10^3\times250}{1.10}=1.2\times231.8=278.2\ \text{kN·m}>267.3\ \text{kN·m}\ \text{(OK, governing }M_d=267.3\text{)}

Check: Md=267.3 kN\cdotpm>Mu=180 kN\cdotpmM_d=267.3\ \text{kN·m}>M_u=180\ \text{kN·m} \Rightarrow bending is adequate.

(c) Shear strength:

Av=Dtw=400×8.9=3560 mm2A_v=D\,t_w=400\times8.9=3560\ \text{mm}^2 Vd=fyAv3γm0=250×35603×1.10=8900001.9053=467.2×103 N=467.2 kNV_d=\frac{f_y\,A_v}{\sqrt3\,\gamma_{m0}}=\frac{250\times3560}{\sqrt3\times1.10}=\frac{890000}{1.9053}=467.2\times10^3\ \text{N}=467.2\ \text{kN}

Check: Vd=467.2 kN>Vu=120 kNV_d=467.2\ \text{kN}>V_u=120\ \text{kN} \Rightarrow shear is adequate.

Also Vu=120<0.6Vd=280.3 kNV_u=120<0.6\,V_d=280.3\ \text{kN}, so it is a low-shear case and no reduction in MdM_d for shear is required.

Conclusion: ISMB 400 is safe in both flexure and shear.

beam-designflexureshear-check
4long8 marks

A welded plate girder is to be designed for a maximum factored bending moment of Mu=2800 kN\cdotpmM_u = 2800\ \text{kN·m} and a factored shear force of Vu=700 kNV_u = 700\ \text{kN}. Steel is Fe410, fy=250 MPaf_y=250\ \text{MPa}, γm0=1.10\gamma_{m0}=1.10.

(a) Determine a suitable economical depth of the web and propose web plate dimensions, given an allowable web shear stress (simple post-critical, conservatively) of τ=100 MPa\tau = 100\ \text{MPa} for sizing the web thickness.
(b) Estimate the required flange area using the flange-area method (lever arm \approx web depth dd).
(c) State two situations that require intermediate transverse stiffeners and the role of bearing stiffeners.

Given: Mu=2800 kN\cdotpmM_u=2800\ \text{kN·m}, Vu=700 kNV_u=700\ \text{kN}, fy=250 MPaf_y=250\ \text{MPa}.

(a) Economical depth of web. The economical depth by the optimum-depth formula:

d=(Mufbtw)1/2 (approx.),but commonly d(Mσbck).d=\left(\frac{M_u}{f_b\,t_w}\right)^{1/2}\ \text{(approx.)},\quad\text{but commonly } d\approx\left(\frac{M}{\sigma_{bc}}\cdot k\right).

A standard practical estimate: d=(3 to 5)×Mufy3×10d=(3\ \text{to}\ 5)\times\sqrt[3]{\dfrac{M_u}{f_y}}\times10 or simply choose dL10d\approx \dfrac{L}{10}. Taking a practical economical depth using d=Mukfy3d=\sqrt[3]{\dfrac{M_u\cdot k}{f_y}}, we adopt a trial web depth d=1200 mmd = 1200\ \text{mm}.

Web thickness from shear (using allowable τ=100 MPa\tau=100\ \text{MPa}):

tw=Vudτ=700×1031200×100=700000120000=5.83 mmadopt tw=8 mm.t_w=\frac{V_u}{d\,\tau}=\frac{700\times10^3}{1200\times100}=\frac{700000}{120000}=5.83\ \text{mm}\Rightarrow \text{adopt } t_w=8\ \text{mm}.

Serviceability/minimum thickness without stiffeners requires d/twd/t_w limited; with d/tw=1200/8=150d/t_w=1200/8=150, intermediate stiffeners will be needed.

Adopt web plate 1200×8 mm1200\times8\ \text{mm}.

(b) Flange area (flange-area method): lever arm d=1200 mm\approx d=1200\ \text{mm}. Design bending stress fbd=fy/γm0=250/1.10=227.3 MPaf_{bd}=f_y/\gamma_{m0}=250/1.10=227.3\ \text{MPa}.

Af=Mufbdd=2800×106227.3×1200=2800×106272760=10266 mm2A_f=\frac{M_u}{f_{bd}\cdot d}=\frac{2800\times10^6}{227.3\times1200}=\frac{2800\times10^6}{272760}=10\,266\ \text{mm}^2

Provide a flange plate, say 400×26 mm400\times26\ \text{mm} giving Af=10400 mm2>10266 mm2A_f=10\,400\ \text{mm}^2>10\,266\ \text{mm}^2. OK.

(Check flange outstand b/2tf=200/26=7.7<8.4εb/2t_f=200/26=7.7<8.4\varepsilon, plastic — satisfactory.)

(c) Stiffeners. Intermediate transverse stiffeners are required when: (i) the web slenderness d/twd/t_w is large (here 150>67ε150 > 67\varepsilon) so the web would buckle in shear before reaching yield; and (ii) the applied shear exceeds the shear-buckling capacity of the unstiffened web, i.e. tension-field/post-critical action must be mobilised.

Bearing (load-carrying) stiffeners are provided at supports and under concentrated point loads to transmit the reaction/load into the web, preventing web crippling and vertical buckling of the web beneath the load.

plate-girderweb-designstiffeners
5long7 marks

A bracket plate is welded to the flange of a column by two vertical fillet welds, each 300 mm300\ \text{mm} long, spaced 150 mm150\ \text{mm} apart (centre to centre). A factored vertical load of P=120 kNP = 120\ \text{kN} acts at an eccentricity of e=200 mme = 200\ \text{mm} from the weld group's vertical centroidal axis (load in the plane of the weld). Use shop welds, fu=410 MPaf_u=410\ \text{MPa}, γmw=1.25\gamma_{mw}=1.25. Determine the required fillet weld size.

Given: two vertical welds, each length l=300 mml=300\ \text{mm}; horizontal spacing =150 mm=150\ \text{mm}; P=120 kNP=120\ \text{kN}; e=200 mme=200\ \text{mm} (eccentricity from group centroid); in-plane (torsional) loading; fu=410 MPaf_u=410\ \text{MPa}, γmw=1.25\gamma_{mw}=1.25.

Work per unit throat (treat weld as line, throat t=1t=1), then size from strength.

Geometry of weld group (two vertical lines): Each line length 300 mm300\ \text{mm}; total weld length Lw=2×300=600 mmL_w=2\times300=600\ \text{mm}. Centroid is at the geometric centre. The two lines are at ±75 mm\pm75\ \text{mm} horizontally.

Polar moment of weld group (per unit throat):

Ix=2×l312=2×300312=2×27×10612=2×2.25×106=4.5×106 mm3I_x=2\times\frac{l^3}{12}=2\times\frac{300^3}{12}=2\times\frac{27\times10^6}{12}=2\times2.25\times10^6=4.5\times10^6\ \text{mm}^3 Iy=2×l×(75)2=2×300×5625=3.375×106 mm3I_y=2\times l\times(75)^2=2\times300\times5625=3.375\times10^6\ \text{mm}^3 J=Ix+Iy=4.5×106+3.375×106=7.875×106 mm3J=I_x+I_y=4.5\times10^6+3.375\times10^6=7.875\times10^6\ \text{mm}^3

Direct (vertical) shear per unit length:

qd=PLw=120×103600=200 N/mm(vertical, downward)q_d=\frac{P}{L_w}=\frac{120\times10^3}{600}=200\ \text{N/mm}\quad(\text{vertical, downward})

Twisting moment: T=Pe=120×103×200=24×106 N\cdotpmmT=P\,e=120\times10^3\times200=24\times10^6\ \text{N·mm}.

The most stressed point is the corner farthest from centroid: rr with components x=75 mmx=75\ \text{mm}, y=150 mmy=150\ \text{mm}.

Torsional shear components per unit length:

qt,x=TyJ=24×106×1507.875×106=3.6×1097.875×106=457.1 N/mm (horizontal)q_{t,x}=\frac{T\,y}{J}=\frac{24\times10^6\times150}{7.875\times10^6}=\frac{3.6\times10^9}{7.875\times10^6}=457.1\ \text{N/mm (horizontal)} qt,y=TxJ=24×106×757.875×106=1.8×1097.875×106=228.6 N/mm (vertical)q_{t,y}=\frac{T\,x}{J}=\frac{24\times10^6\times75}{7.875\times10^6}=\frac{1.8\times10^9}{7.875\times10^6}=228.6\ \text{N/mm (vertical)}

Resultant per unit length: combine vertical (qd+qt,yq_d+q_{t,y}) and horizontal (qt,xq_{t,x}):

qres=(qd+qt,y)2+qt,x2=(200+228.6)2+457.12q_{res}=\sqrt{(q_d+q_{t,y})^2+q_{t,x}^2}=\sqrt{(200+228.6)^2+457.1^2} =428.62+457.12=183698+208940=392638=626.6 N/mm=\sqrt{428.6^2+457.1^2}=\sqrt{183698+208940}=\sqrt{392638}=626.6\ \text{N/mm}

Weld strength per unit length for throat tt=0.707st_t=0.707\,s (size ss):

fwd=fu3γmw=4103×1.25=4102.1651=189.4 MPaf_{wd}=\frac{f_u}{\sqrt3\,\gamma_{mw}}=\frac{410}{\sqrt3\times1.25}=\frac{410}{2.1651}=189.4\ \text{MPa}

Strength per mm length =0.707s×189.4=133.9s N/mm=0.707\,s\times189.4=133.9\,s\ \text{N/mm}.

Required size:

133.9s626.6s626.6133.9=4.68 mm133.9\,s\ge 626.6\Rightarrow s\ge\frac{626.6}{133.9}=4.68\ \text{mm}

Provide a 6 mm fillet weld (next standard size 4.68\ge 4.68 mm and satisfying minimum size for thick flange).

Answer: fillet weld size s=6 mms = 6\ \text{mm}.

welded-connectionfillet-weldeccentric-load
B

Section B: Short Answer Questions

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6 questions
6short5 marks

A column carrying a factored axial load of 900 kN900\ \text{kN} rests on a square slab base supported on M20 grade concrete (bearing strength 0.45fck=0.45×20=9 MPa0.45 f_{ck}=0.45\times20=9\ \text{MPa}). Determine the minimum required plan size (side) of a square slab base.

Given: Pu=900 kN=900×103 NP_u=900\ \text{kN}=900\times10^3\ \text{N}; permissible bearing pressure on concrete w=0.45fck=9 MPa (N/mm2)w=0.45 f_{ck}=9\ \text{MPa (N/mm}^2).

Required bearing area:

Areq=Puw=900×1039=1.0×105 mm2=100000 mm2A_{req}=\frac{P_u}{w}=\frac{900\times10^3}{9}=1.0\times10^5\ \text{mm}^2=100000\ \text{mm}^2

For a square base of side aa:

a=Areq=100000=316.2 mma=\sqrt{A_{req}}=\sqrt{100000}=316.2\ \text{mm}

Provide a square slab base of 350 mm×350 mm350\ \text{mm}\times350\ \text{mm} (rounded up to a practical size).

Check actual pressure: wact=900×103350×350=900000122500=7.35 MPa<9 MPaw_{act}=\dfrac{900\times10^3}{350\times350}=\dfrac{900000}{122500}=7.35\ \text{MPa}<9\ \text{MPa}. Safe.

Answer: minimum side 317 mm\approx 317\ \text{mm}; adopt 350×350 mm350\times350\ \text{mm} slab base.

column-baseslab-basebearing
7short5 marks

A simply supported timber beam of span 3 m3\ \text{m} carries a working uniformly distributed load of 4 kN/m4\ \text{kN/m}. The permissible bending stress in the timber is σb=10 MPa\sigma_b = 10\ \text{MPa}. Determine the required section modulus and propose a rectangular section if the depth is to be twice the breadth.

Given: L=3 mL=3\ \text{m}, w=4 kN/mw=4\ \text{kN/m}, σb=10 MPa\sigma_b=10\ \text{MPa}, d=2bd=2b.

Maximum bending moment:

M=wL28=4×328=4×98=4.5 kN\cdotpm=4.5×106 N\cdotpmmM=\frac{wL^2}{8}=\frac{4\times3^2}{8}=\frac{4\times9}{8}=4.5\ \text{kN·m}=4.5\times10^6\ \text{N·mm}

Required section modulus:

Zreq=Mσb=4.5×10610=4.5×105 mm3=450000 mm3Z_{req}=\frac{M}{\sigma_b}=\frac{4.5\times10^6}{10}=4.5\times10^5\ \text{mm}^3=450000\ \text{mm}^3

Rectangular section (d=2bd=2b): Z=bd26=b(2b)26=4b36=2b33Z=\dfrac{b\,d^2}{6}=\dfrac{b(2b)^2}{6}=\dfrac{4b^3}{6}=\dfrac{2b^3}{3}.

2b33=450000b3=3×4500002=675000b=6750003=87.7 mm\frac{2b^3}{3}=450000\Rightarrow b^3=\frac{3\times450000}{2}=675000\Rightarrow b=\sqrt[3]{675000}=87.7\ \text{mm}

Then d=2b=175.4 mmd=2b=175.4\ \text{mm}.

Provide a section of b=100 mmb=100\ \text{mm}, d=200 mmd=200\ \text{mm} (practical, d=2bd=2b).

Check: Z=100×20026=4×1066=666667 mm3>450000 mm3Z=\dfrac{100\times200^2}{6}=\dfrac{4\times10^6}{6}=666667\ \text{mm}^3>450000\ \text{mm}^3. Safe.

Answer: Zreq=4.5×105 mm3Z_{req}=4.5\times10^5\ \text{mm}^3; adopt 100×200 mm100\times200\ \text{mm} timber beam.

timber-designbeam-bendingpermissible-stress
8short5 marks

A roof truss spans 12 m12\ \text{m} and trusses are spaced at 4 m4\ \text{m} centre to centre. The total roof dead plus live load (on plan) is 0.9 kN/m20.9\ \text{kN/m}^2. The truss has 66 equal panels along the span (panel length 2 m2\ \text{m}). Determine the load transmitted to one intermediate (interior) panel point and to an end panel point. (Consider the tributary roof area; ignore wind.)

Given: span =12 m=12\ \text{m}, truss spacing s=4 ms=4\ \text{m}, intensity q=0.9 kN/m2q=0.9\ \text{kN/m}^2 (on plan), 66 panels, panel length a=2 ma=2\ \text{m}.

Load per metre length of truss (per unit span):

w=q×s=0.9×4=3.6 kN/m of spanw=q\times s=0.9\times4=3.6\ \text{kN/m of span}

Intermediate (interior) panel point — tributary length == one full panel (a=2 ma=2\ \text{m}, half panel on each side):

Wint=w×a=3.6×2=7.2 kNW_{int}=w\times a=3.6\times2=7.2\ \text{kN}

End panel point — tributary length == half a panel (a/2=1 ma/2=1\ \text{m}):

Wend=w×a2=3.6×1=3.6 kNW_{end}=w\times\frac{a}{2}=3.6\times1=3.6\ \text{kN}

Verification (total): 55 interior points ++ 22 end points:

5×7.2+2×3.6=36+7.2=43.2 kN5\times7.2+2\times3.6=36+7.2=43.2\ \text{kN}

Total roof load =q×span×s=0.9×12×4=43.2 kN=q\times \text{span}\times s=0.9\times12\times4=43.2\ \text{kN}. Checks out.

Answer: interior panel-point load =7.2 kN=\mathbf{7.2\ kN}; end panel-point load =3.6 kN=\mathbf{3.6\ kN}.

roof-trussload-calculationpanel-point
9short5 marks

Briefly explain the block shear failure mode in a bolted tension member connection and write the IS 800:2007 expression for the block shear strength TdbT_{db}. State why this limit state often governs for angles connected through one leg.

Block shear failure: In a bolted tension connection, a block of material at the end of the member can tear out as a single unit. Failure occurs along a combined path — shear yielding/rupture along the bolt line(s) parallel to the load together with tension yielding/rupture across a plane perpendicular to the load connecting the bolt holes. It is a tearing-out of the bolted block rather than a clean net-section failure.

IS 800:2007 block shear strength — the design strength TdbT_{db} is the smaller of the two modes:

Mode 1 — shear yield + tension rupture:

Tdb1=Avgfy3γm0+0.9Atnfuγm1T_{db1}=\frac{A_{vg}\,f_y}{\sqrt3\,\gamma_{m0}}+\frac{0.9\,A_{tn}\,f_u}{\gamma_{m1}}

Mode 2 — shear rupture + tension yield:

Tdb2=0.9Avnfu3γm1+Atgfyγm0T_{db2}=\frac{0.9\,A_{vn}\,f_u}{\sqrt3\,\gamma_{m1}}+\frac{A_{tg}\,f_y}{\gamma_{m0}}

where Avg,AvnA_{vg},A_{vn} = gross/net area in shear (along bolt line) and Atg,AtnA_{tg},A_{tn} = gross/net area in tension (perpendicular to load).

Why it governs for single-leg-connected angles: When an angle is connected through only one leg, the load is transmitted eccentrically and concentrated near the connected leg. Combined with the short end distance and limited bolt arrangement, the small block of material around the bolts is prone to tearing out. The reduced effective net area and stress concentration make block shear frequently the critical (lowest) limit state, often governing over gross-section yielding and net-section rupture.

tension-memberblock-shearangle-section
10short4 marks

Differentiate between the Working Stress Method (WSM) and the Limit State Method (LSM) of structural steel design as adopted in IS 800:2007. Mention at least three points of difference.

Working Stress Method (WSM) vs Limit State Method (LSM):

AspectWorking Stress Method (WSM)Limit State Method (LSM)
BasisElastic behaviour; stresses kept within permissible (allowable) limitsConsiders both strength (ultimate) and serviceability limit states; semi-probabilistic
SafetySingle global factor of safety applied to material strength (e.g. σperm=fy/FOS\sigma_{perm}=f_y/\text{FOS})Partial safety factors applied separately to loads (γf\gamma_f) and materials (γm\gamma_m)
LoadsService (working) loads used directlyFactored (design) loads used
Material utilisationConservative; reserve strength beyond yield ignoredEconomical; uses plastic reserve and reliability-based margins
ReliabilityDeterministic, no explicit probabilityAccounts for variability of loads and materials statistically

Three key points of difference:

  1. WSM uses a single factor of safety on material strength, whereas LSM uses separate partial safety factors for loads and materials.
  2. WSM is based purely on elastic stress limitation; LSM checks multiple limit states (strength + serviceability) and exploits plastic reserve.
  3. WSM uses service loads; LSM uses factored loads, giving more rational and generally more economical designs.

IS 800:2007 adopts LSM as the primary method (WSM is retained as an alternative).

design-philosophylimit-stateworking-stress
11short5 marks

Explain lateral-torsional buckling (LTB) of a steel beam. List the main factors that influence the lateral-torsional buckling strength, and state two practical measures to prevent it.

Lateral-torsional buckling (LTB): When a slender beam is loaded about its major (strong) axis, the compression flange behaves like a column and tends to buckle sideways. Because the tension flange resists this movement, the cross-section simultaneously deflects laterally and twists. This combined out-of-plane lateral deflection and rotation, occurring before the in-plane plastic moment is reached, is lateral-torsional buckling. It reduces the moment capacity below the full plastic moment MpM_p, so a bending reduction factor χLT\chi_{LT} (or βb<1\beta_b<1) must be applied for laterally unrestrained beams.

Factors influencing LTB strength:

  1. Unsupported (effective) length of the compression flange — larger LLTL_{LT} lowers strength.
  2. Cross-sectional shape and properties — torsional constant ItI_t, warping constant IwI_w, and minor-axis moment of inertia IyyI_{yy}.
  3. Type and position of loading — point vs UDL, load applied at top flange (destabilising) vs at shear centre.
  4. End/support conditions and restraints (lateral and torsional restraint at supports).
  5. Moment gradient along the span (uniform moment is most critical).
  6. Material yield strength and residual stresses / imperfections.

Two practical measures to prevent LTB:

  1. Provide adequate lateral restraint to the compression flange — e.g. cross beams, bracing, or a connected concrete/steel deck that holds the flange in position (reduces effective length).
  2. Use sections with high torsional/lateral stiffness (e.g. wider flanges, or encasing/box sections), or reduce the unsupported length by introducing intermediate supports.
lateral-torsional-bucklingbeam-stabilityconcepts

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