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3 m wall under wind: fixed top and bottom

Short answer

A half-brick wall of 115 mm thickness satisfies stress requirements (slenderness ratio 19.6 < 27), but for practical stability use a 230 mm one-brick wall. Use bricks of 3.5 N/mm² with cement mortar M1 (1:5). Stresses are negligible: σmax=0.062 N/mm².

Design a wall 3 m high to resist a wind load. The wall is fixed at top and bottom supports. Assume uniformly distributed wind pressure of 16 N/m2^2.

Data and assumptions

  • The wall is fixed at top and bottom, so hef=0.75H=2.25h_{ef}=0.75H=2.25 m (full restraint, Table 4 Sl. 1). No vertical load other than self weight is given. The pressure is taken as stated, 16 N/m2^2 (0.016 kN/m2^2) [reading: a very small wind pressure, so stresses are tiny and slenderness controls the thickness].
  • End moment of a wall fixed at both ends under uniform load: M=wH2/12M=wH^2/12 at each end (sagging wH2/24wH^2/24 at mid-height). Section checked at the base, where self weight is the largest.
  • Design by IS 1905:1987 cl. 5.4.1, 5.4.2, 5.5.2, 5.5.3 (NBC 109 follows the same method). Unit weight of masonry 19 kN/m3^3. Per metre run of wall.
  ======+===========  fixed (top)
        |<-- wind w
        |  wall H=3 m
        |  M = wH^2/12 at ends
  ======+===========  fixed (bottom)

Step 1: Wind moment

w=0.016 kN/m (per m of wall)M=0.016×3.02/12=0.012 kNm/m\begin{aligned} w &= 0.016\ \text{kN/m (per m of wall)}\\ M &= 0.016\times3.0^2/12 = 0.012\ \text{kNm/m} \end{aligned}

Step 2: Trial thickness 115 mm, load and slenderness

Self weight of wall=0.115×3.00×19=6.56 kN/mN (at base)=6.56 kN/mhef=0.75×3.0=2.25 mSR=2.2500.115=19.57 (<27)\begin{aligned} \text{Self weight of wall} &= 0.115\times3.00\times19 = 6.56\ \text{kN/m}\\ N\ (\text{at base}) &= 6.56\ \text{kN/m}\\ h_{ef} &= 0.75\times3.0=2.25\ \text{m} \\ SR &= \frac{2.250}{0.115} = 19.57\ (<27) \end{aligned}

Step 3: Stresses at the base section

σa=NA=6.56×103115×103=0.0570 N/mm2σb=6Mt2=6×0.012×1061000×1152=0.0054 N/mm2σmax=σa+σb=0.0624,σmin=σa−σb=0.0516 N/mm2\begin{aligned} \sigma_a &= \frac{N}{A}=\frac{6.56\times10^3}{115\times10^3} = 0.0570\ \text{N/mm}^2\\ \sigma_b &= \frac{6M}{t^2} = \frac{6\times0.012\times10^6}{1000\times115^2} = 0.0054\ \text{N/mm}^2\\ \sigma_{max} &= \sigma_a+\sigma_b = 0.0624,\qquad \sigma_{min} = \sigma_a-\sigma_b = 0.0516\ \text{N/mm}^2 \end{aligned}

σmin>0\sigma_{min}>0: the whole section is in compression, no tension (the resultant eccentricity e=M/N=0.0018e=M/N=0.0018 m, e/t=0.016<1/6e/t=0.016<1/6).

Step 4: Required basic compressive stress

Resultant eccentricity ratio e/t=M/(Nt)=0.016e/t = M/(Nt) = 0.016. From Table 9: ks=0.619k_s=0.619 (SR=19.57SR=19.57). ka=1k_a=1, kp=1k_p=1.

fb≥σakskakp×1.00=0.05700.619×1.00=0.092 N/mm2f_b \ge \frac{\sigma_a}{k_sk_ak_p\times1.00} = \frac{0.0570}{0.619\times1.00} = 0.092\ \text{N/mm}^2

Step 5: Brick and mortar (IS 1905 Table 8)

Mortar (IS 1905 Table 1)Min. unit strength (N/mm²)Table 8 fbf_b (N/mm²)
M2 (cement:sand 1:6)3.50.35
M1 (cement:sand 1:5)3.50.35
H2 (cement:sand 1:4)3.50.35
H1 (cement:sand 1:3)3.50.35

Answer: a half-brick wall of 115 mm is sufficient for stress (SR = 19.6 < 27), but for stability and practical robustness adopt a 230 mm (one-brick) wall; bricks of 3.5 N/mm2^2 with cement mortar M1 (1:5). Stresses are very small: σmax=0.0624\sigma_{max}=0.0624, σmin=0.0516\sigma_{min}=0.0516 N/mm2^2, far below the permissible values.

✓ Answer checked by Claude Opus 5.5 (high effort)

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