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Beam design, 250x475 section

Short answer

Mu=256.41 kNm. Doubly reinforced: Ast=1632 mm² (3-25+1-16 mm), Asc=664 mm² (4-16 mm). Deflection safe: L/d actual=9.3, allowable=18.7.

A simply supported RCC beam of effective span 4 m and overall dimensions 250 mm x 475 mm is subjected to superimposed load of 45 kN/m excluding its self-weight with point load 75 kN at midspan. Design the beam for limit state of collapse in flexure. Also, check whether the beam is safe in deflection or not. Consider effective cover to be 45 mm. Take M25 concrete and TMT bars. All the loads are at service level.

Given: L=4L=4 m, b=250b=250 mm, D=475D=475 mm, effective cover 45 mm, so d=430d=430 mm and d′=45d'=45 mm; superimposed load 45 kN/m and point load 75 kN at mid-span (service), M25. "TMT bars" is taken as Fe500 (fy=500f_y=500 N/mm2^2).

Step 1: Loads and moment

Self weight=0.25×0.475×25=2.97 kN/m,w=47.97 kN/mwu=1.5w=71.95 kN/m,Pu=1.5×75=112.5 kNMu=wuL28+PuL4=143.91+112.50=256.41 kN⋅m\begin{aligned} \text{Self weight}&=0.25\times0.475\times25=2.97\ \text{kN/m},\quad w=47.97\ \text{kN/m}\\ w_u&=1.5w=71.95\ \text{kN/m},\quad P_u=1.5\times75=112.5\ \text{kN}\\ M_u&=\frac{w_uL^2}{8}+\frac{P_uL}{4}=143.91+112.50=256.41\ \text{kN·m} \end{aligned}

Step 2: Limiting moment (Fe500: xu,max=0.46dx_{u,max}=0.46d)

Mu,lim=0.1336fckbd2=0.1336×25×250×4302=154.40 kN⋅m<MuM_{u,lim}=0.1336f_{ck}bd^2=0.1336\times25\times250\times430^2=154.40\ \text{kN·m}<M_u

The section is too shallow for a singly reinforced design, so it is designed as doubly reinforced.

Doubly reinforced design

Mu2=Mu−Mu,lim=256.41−154.40=102.01 kN⋅mM_{u2}=M_u-M_{u,lim}=256.41-154.40=102.01\ \text{kN·m}

Limiting depth xu,max=0.46d=197.8x_{u,max}=0.46d=197.8 mm. Strain in compression steel (similar triangles):

εsc=0.0035(1−d′xu,max)=0.0035(1−45197.8)=0.00270\varepsilon_{sc}=0.0035\left(1-\frac{d'}{x_{u,max}}\right)=0.0035\left(1-\frac{45}{197.8}\right)=0.00270

From the design stress-strain curve of Fe500 (IS 456 Fig. 23): fsc=410.2f_{sc}=410.2 N/mm2^2. Stress in the concrete displaced by the steel: fcc=0.446fck=11.15f_{cc}=0.446f_{ck}=11.15 N/mm2^2.

Asc=Mu2(fsc−fcc)(d−d′)=102.01×106(410.2−11.15)(430−45)=664 mm2A_{sc}=\frac{M_{u2}}{(f_{sc}-f_{cc})(d-d')}=\frac{102.01\times10^6}{(410.2-11.15)(430-45)}=664\ \text{mm}^2 Ast1=0.36fck b xu,max0.87fy=1023 mm2,Ast2=Asc(fsc−fcc)0.87fy=609 mm2A_{st1}=\frac{0.36f_{ck}\,b\,x_{u,max}}{0.87f_y}=1023\ \text{mm}^2,\qquad A_{st2}=\frac{A_{sc}(f_{sc}-f_{cc})}{0.87f_y}=609\ \text{mm}^2 Ast=Ast1+Ast2=1632 mm2A_{st}=A_{st1}+A_{st2}=1632\ \text{mm}^2

Provide: tension 3-25 mm + 1-16 mm dia (16741674 mm2^2, one layer in the 250 mm width) and compression 4-16 mm dia (804804 mm2^2), with 8 mm stirrups.

Check: 0.87fyAst=435×1674=7280.87f_yA_{st}=435\times1674=728 kN, which is less than the compression available at xu,maxx_{u,max}, 0.36fckbxu,max+Asc(fsc−fcc)=445+321=7660.36f_{ck}bx_{u,max}+A_{sc}(f_{sc}-f_{cc})=445+321=766 kN, so xu<xu,maxx_u<x_{u,max}, OK. (Providing far more tension steel, such as 6-20 mm = 1885 mm2^2, would make xu>xu,maxx_u>x_{u,max}.)

Step 3: Deflection check (IS 456 cl. 23.2)

pt=100Astbd=1.56%,fs=0.58fyAst,reqAst,prov=282.7 N/mm2,kt≈0.80 (Fig. 4)p_t=\frac{100A_{st}}{bd}=1.56\%,\quad f_s=0.58f_y\frac{A_{st,req}}{A_{st,prov}}=282.7\ \text{N/mm}^2,\quad k_t\approx0.80\ \text{(Fig. 4)}

Compression steel pc=100Ascbd=0.75%p_c=\dfrac{100A_{sc}}{bd}=0.75\%, modification factor kc=1.6pcpc+0.275=1.17k_c=\dfrac{1.6p_c}{p_c+0.275}=1.17.

(Ld)allow=20×kt×kc=20×0.80×1.17=18.7,(Ld)actual=4000430=9.30\left(\frac{L}{d}\right)_{allow}=20\times k_t\times k_c=20\times0.80\times1.17=18.7,\qquad \left(\frac{L}{d}\right)_{actual}=\frac{4000}{430}=9.30

Actual << allowable, so the beam is safe in deflection.

Answer: Mu=256.41M_u=256.41 kN·m; Ast=1632A_{st}=1632 mm2^2 (provide 3-25 + 1-16 mm), Asc=664A_{sc}=664 mm2^2 (provide 4-16 mm); safe in deflection.

✓ Answer checked by Claude Opus 5.5 (high effort)

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