Web Buckling and Web Crippling in Steel Beams: Complete Design Guide - Theory, IS 800, AISC 360, Eurocode 3, Stiffener Design & Worked Examples

The all-in-one reference: full elastic plate buckling derivation, critical shear stress formulas, tension field action post-buckling theory, IS 800 Cl. 8.4 and 8.7 checks, AISC 360 web local yielding and crippling, Eurocode 3 EN 1993-1-5 resistance formulas, bearing and transverse stiffener design with worked example, load dispersion model, web slenderness limits, and interactive calculator.

Elastic Plate Theory IS 800 / AISC 360 / EC3 Tension Field Action Stiffener Design
By Bimal Ghimire • Published July 10, 2025 • Updated February 28, 2026 • 30 min read

Web Buckling vs Web Crippling: Definitions, Mechanisms, and Failure Modes

The web of a steel I-beam or plate girder is the thin vertical plate connecting the two flanges. Its primary function is to resist shear forces between the flanges, but it also contributes to bending resistance by maintaining the separation between tension and compression flanges. Because the web is intentionally slender (high depth-to-thickness ratio $h_w/t_w$) for structural efficiency, it is susceptible to two distinct categories of localised failure that must each be designed against independently:

  • Web buckling - out-of-plane instability of the web panel under in-plane compressive stresses arising from shear, bending, or combined loading. A stability (eigenvalue) problem governed by elastic plate buckling theory.
  • Web crippling (web bearing) - local crushing and yielding of the web directly under a concentrated transverse force (reaction at support or heavy point load). A strength problem governed by the yield strength of the web steel and the contact area.

The two phenomena are physically distinct and are checked by separate code clauses (IS 800 Cl. 8.4 for shear buckling; Cl. 8.7 for bearing/crippling; AISC 360 Sections J8 and J10), but they interact in practice and both may require stiffeners at the same location.

$h_w/t_w$
Key slenderness ratio governing web buckling susceptibility
67ε
IS 800 limit for no shear buckling check required (plastic/compact web)
τcr
Critical elastic shear stress for web buckling onset
kv = 5.34
Shear buckling coefficient for unstiffened web (pure shear)
FeatureWeb BucklingWeb Crippling (Bearing Failure)
Nature of failureOut-of-plane stability - web panel deflects laterally under in-plane compressive stressIn-plane strength - web material yields/crushes locally under concentrated transverse force
Primary stress causing failureDiagonal compressive stress from shear; or direct compression from bending in slender websDirect compressive bearing stress: $\sigma_{Ed} = F/(b_1 \cdot t_w)$ at web toe of fillet
Critical parameterWeb slenderness $h_w/t_w$; panel aspect ratio $a/h_w$; boundary conditionsBearing length $b_1$; web thickness $t_w$; fillet size $r$ or $s$; yield strength $f_y$
Governing code clauseIS 800 Cl. 8.4; AISC 360 G2; EC3 EN 1993-1-5 Cl. 5IS 800 Cl. 8.7.4; AISC 360 J10.3, J10.4; EC3 EN 1993-1-5 Cl. 6
Visible signWeb panel bowing or diagonal wrinkle pattern (tension field) visible at high shearLocalised indentation or dent in web directly under concentrated load; possible flange rotation
Post-failure behaviourMay have post-buckling reserve (tension field action); failure usually not sudden for ductile steelProgressive yielding spreads; can be sudden if web is very thin relative to load
Primary fixTransverse (intermediate) stiffeners to reduce panel aspect ratio; increase $t_w$Bearing stiffeners at load point; increase bearing length $b_1$; increase $t_w$
Steel I-Beam: Web Failure Mode Locations Shear buckling diagonal wrinkles hₗ/tₗ governs V hₗ tₗ Bearing plate (b₁) F (concentrated) Web crippling yielding / crush b₁ and tₗ govern 1:2.5 dispersion Web buckling under shear Web crippling under concentrated load

Elastic Plate Buckling Theory: Derivation of Critical Stress

The theoretical basis for all web buckling checks is the elastic stability of a thin rectangular plate under in-plane loading, first solved analytically by Bryan (1891) and extended by Timoshenko (1936). The web panel is idealised as a thin plate with width $h_w$ (clear depth), length $a$ (panel length between stiffeners), and thickness $t_w$, with boundary conditions determined by the flange and stiffener stiffness.

Governing Differential Equation for Elastic Plate Buckling (Bryan 1891)
$$D\left(\frac{\partial^4 w}{\partial x^4} + 2\frac{\partial^4 w}{\partial x^2 \partial y^2} + \frac{\partial^4 w}{\partial y^4}\right) = N_x\frac{\partial^2 w}{\partial x^2} + 2N_{xy}\frac{\partial^2 w}{\partial x \partial y} + N_y\frac{\partial^2 w}{\partial y^2}$$ $$D = \frac{E\,t_w^3}{12(1-\nu^2)} \quad \text{(plate flexural rigidity)}$$
$w$ = out-of-plane displacement of web plate. $D$ = plate flexural rigidity (N·mm). $E$ = Young's modulus (205,000 MPa for steel). $\nu$ = Poisson's ratio (0.3 for steel). $N_x$, $N_y$, $N_{xy}$ = in-plane force resultants per unit length (N/mm) in $x$, $y$, and shear directions respectively. For a web in pure shear: $N_x = N_y = 0$; $N_{xy} = \tau\,t_w$. For a web in pure bending: $N_{xy} = 0$; $N_x$ varies linearly from $+\sigma\,t_w$ (compression) to $-\sigma\,t_w$ (tension) across the depth.
General Critical Stress Solution: Plate Buckling Coefficient $k$
$$\sigma_{cr} = k \cdot \frac{\pi^2 E}{12(1-\nu^2)} \cdot \left(\frac{t_w}{b}\right)^2$$
$\sigma_{cr}$ = critical elastic buckling stress (MPa). $k$ = plate buckling coefficient (dimensionless): depends on loading type, aspect ratio $\alpha_0 = a/h_w$, and boundary conditions. $b$ = plate dimension perpendicular to the compressive stress direction ($= h_w$ for shear loading; $= b_f$ for flange compression). For steel: $E = 205{,}000$ MPa, $\nu = 0.3$, so $\pi^2 E / [12(1-\nu^2)] = 189{,}800$ MPa. This formula applies equally to: shear buckling ($k = k_v$), compression buckling ($k = k_c$), and bending buckling of the web ($k = k_b$). The key result is that critical stress scales as $(t_w/h_w)^2$ - halving the web thickness reduces critical buckling stress to one-quarter, explaining the strong sensitivity to slenderness ratio.
Shear Buckling Coefficient $k_v$ for Rectangular Web Panels
$$k_v = 5.34 + \frac{4.00}{(a/h_w)^2} \quad \text{for } a/h_w \geq 1 \quad \text{(simply supported on all four edges)}$$ $$k_v = 4.00 + \frac{5.34}{(a/h_w)^2} \quad \text{for } a/h_w < 1$$ $$k_v = 5.34 \quad \text{(unstiffened web, } a/h_w \to \infty\text{)}$$
$a$ = distance between transverse stiffeners (mm). $h_w$ = clear depth of web (mm). The minimum $k_v = 5.34$ applies to an infinitely long unstiffened web; adding transverse stiffeners reduces the effective panel aspect ratio $a/h_w$, increasing $k_v$ and hence $\tau_{cr}$. For a square panel ($a/h_w = 1$): $k_v = 5.34 + 4.00 = 9.34$ - a 75% increase in critical stress compared to unstiffened. The four simply-supported edges (flanges as rigid boundaries, free sides at stiffener locations) is the standard assumption in all codes. Fixed boundary conditions (rigid flanges) give higher $k_v$ but are conservative to ignore.
Critical Elastic Shear Stress for Web Buckling
$$\tau_{cr} = k_v \cdot \frac{\pi^2 E}{12(1-\nu^2)} \cdot \left(\frac{t_w}{h_w}\right)^2 = k_v \cdot \frac{189{,}800\,t_w^2}{h_w^2} \;\text{MPa}$$
Substituting $E = 205{,}000$ MPa and $\nu = 0.3$: the coefficient $\pi^2 \times 205{,}000 / [12 \times (1 - 0.09)] = 189{,}800$ MPa. Example: for an unstiffened web with $h_w/t_w = 100$: $\tau_{cr} = 5.34 \times 189{,}800 / 100^2 = 5.34 \times 18.98 = \mathbf{101}$ MPa for $t_w = 10$ mm, $h_w = 1000$ mm. Since the yield shear stress of Fe 410 steel is $f_y/\sqrt{3} = 250/1.732 = 144$ MPa, this web would buckle before yielding in shear - confirming that a shear buckling check is necessary for slender webs.
Web Slenderness Parameter $\bar\lambda_w$ and Shear Reduction Factor $\chi_w$ (IS 800 / EC3)
$$\bar\lambda_w = \frac{\tau_y}{\tau_{cr}} = \sqrt{\frac{f_y/\sqrt{3}}{k_v \cdot \frac{\pi^2 E}{12(1-\nu^2)}\cdot(t_w/h_w)^2}} = \frac{h_w/t_w}{86.4\,\varepsilon\,\sqrt{k_v}}$$ $$\varepsilon = \sqrt{250/f_y} \quad \text{(material factor; } \varepsilon = 1.0 \text{ for } f_y = 250 \text{ MPa)}$$ $$\chi_w = \begin{cases} \eta / \sqrt{3} & \bar\lambda_w < 0.83/\eta \quad \text{(no buckling; full yield)}\\ 0.83/(\sqrt{3}\,\bar\lambda_w) & 0.83/\eta \leq \bar\lambda_w < 1.08 \quad \text{(post-yield; partial)}\\ 1.37/(\sqrt{3}(0.7+\bar\lambda_w)) & \bar\lambda_w \geq 1.08 \quad \text{(elastic buckling governs)} \end{cases}$$
$\bar\lambda_w$ = non-dimensional web slenderness for shear. $\chi_w$ = shear reduction factor ($0 < \chi_w \leq \eta/\sqrt{3}$). $\eta$ = contribution factor (1.20 for steel with $f_y \leq 460$ MPa per EC3 EN 1993-1-5 Cl. 5.1; 1.0 per IS 800). $f_y$ = nominal yield strength (MPa). The three regimes physically correspond to: (1) fully plastic shear ($\bar\lambda_w$ small): no buckling, $V_{cr} = f_y\,h_w\,t_w/(\sqrt{3}\,\gamma_{M0})$; (2) inelastic buckling: shear reduction accounting for yielding combined with buckling; (3) elastic buckling governs for very slender webs ($\bar\lambda_w \geq 1.08$): web buckles before yielding and post-buckling tension field action provides residual capacity.

Shear Buckling: Critical Limits, Slenderness Classification, and Code h/t Limits

Shear buckling is the most common form of web buckling in plate girders and deep I-sections. Under shear loading, the web panel is in a state of pure shear, which is equivalent to equal principal tensile and compressive stresses at 45° to the web plane. When the compressive principal stress reaches the critical value, the web buckles diagonally. The diagonal wrinkle pattern seen in buckled plate girder webs is the visible manifestation of this mode.

CodeSlenderness Limit (no check needed)Intermediate limitRequires stiffeners or reduced resistance
IS 800:2007$h_w/t_w \leq 67\varepsilon$ (for unstiffened web, $k_v = 5.34$; shear check not required - full yield shear governs)$67\varepsilon < h_w/t_w \leq 200\varepsilon$: shear buckling check required; tension field action permitted$h_w/t_w > 200\varepsilon$: must provide transverse stiffeners; longitudinal stiffeners may be required
AISC 360-22$h/t_w \leq 2.24\sqrt{E/F_y}$ for doubly symmetric I-shapes (i.e. $\leq 63.5$ for $F_y = 250$ MPa): $V_n = 0.6\,F_y\,A_w$$2.24\sqrt{E/F_y} < h/t_w \leq 1.10\sqrt{k_v E/F_y}$: transition zone, $C_{v1}$ applies$h/t_w > 1.10\sqrt{k_v E/F_y}$: $V_n = 0.6\,F_y\,A_w\,C_{v2}$ (elastic buckling regime)
Eurocode 3 EN 1993-1-5$h_w/t_w \leq 72\varepsilon/\eta$ ($\approx 60$ for $f_y = 250$ MPa, $\eta = 1.2$): no shear buckling$72\varepsilon/\eta < h_w/t_w$: compute $\bar\lambda_w$ and $\chi_w$$\bar\lambda_w > 1.08$: elastic buckling; post-buckling via tension field
IS 800 absolute limit$h_w/t_w \leq 200$ for webs without longitudinal stiffeners$h_w/t_w > 200$: must provide longitudinal stiffeners; limit 400 with both transverse and longitudinal
IS 800:2007 Shear Capacity Formula (Cl. 8.4)
$$V_{dp} = V_{nsb} / \gamma_{m0} = \frac{f_{yw}\,h_w\,t_w}{\sqrt{3}\,\gamma_{m0}} \quad \text{(no shear buckling; } h_w/t_w \leq 67\varepsilon\text{)}$$ $$V_{db} = \frac{V_{nsb}}{\gamma_{m0}} \quad \text{where} \quad V_{nsb} = \chi_w \cdot \frac{f_{yw}\,h_w\,t_w}{\sqrt{3}} \quad \text{(with shear buckling)}$$ $$\chi_w = \frac{1}{\phi_w + \sqrt{\phi_w^2 - \bar\lambda_w^2}} \quad \text{where} \quad \phi_w = 0.5[1 + 0.2(\bar\lambda_w - 0.6) + \bar\lambda_w^2] \quad (\text{IS 800 format})$$
$V_{dp}$ = design plastic shear resistance (kN). $V_{db}$ = design shear resistance with buckling (kN). $\gamma_{m0} = 1.10$ (IS 800 partial safety factor for yielding). $f_{yw}$ = yield strength of web (MPa). $h_w$ = clear depth of web between flanges (mm). $t_w$ = web thickness (mm). The formula gives the reduced shear capacity $V_{db} < V_{dp}$ when the slenderness parameter $\bar\lambda_w > 0.6$. Note IS 800 uses the simple reduction factor approach; the three-regime formula from EC3 is equivalent but presented differently.

Physical interpretation: The shear buckling coefficient $k_v = 5.34$ for an unstiffened web corresponds to buckling into a single half-wave in both the depth and length directions. Adding transverse stiffeners at spacing $a$ imposes nodal lines at the stiffener locations, forcing the web to buckle into shorter panels with higher critical stress. The relationship $k_v = 5.34 + 4/(a/h_w)^2$ shows that stiffener spacing must be reduced to $a \leq h_w$ to meaningfully increase $k_v$ beyond 9.34 - diminishing returns exist for very close stiffener spacing.

Tension Field Action: Post-Buckling Reserve Strength Theory

After a slender web panel buckles in shear, it does not immediately fail. The buckled web can still carry substantial additional load through a mechanism called tension field action (or diagonal tension field) first described by Wagner (1929) for thin-walled aircraft structures and extended to steel plate girders by Basler (1961) and later by Rockey, Evans, and Porter (1978). This is the primary reason why slender plate girder webs are structurally viable despite exceeding the elastic buckling limit.

Physical Mechanism

After elastic shear buckling occurs at $\tau_{cr}$, the web panel can no longer carry additional shear by membrane compression in the diagonal direction. However, it can still carry tension in the orthogonal diagonal direction. This diagonal tension band - anchored between the flanges and stiffeners at the panel corners - resists the additional applied shear through a truss-like action:

  • Diagonal tension strips in the web carry tensile stress at angle $\theta$ to the horizontal.
  • Flanges act as the chords of the truss, developing bending moments due to the vertical component of the tension field force.
  • Transverse stiffeners act as the vertical compression struts of the truss, resisting the compressive reaction from the tension field.
Basler Tension Field Action - Shear Resistance (Basler 1961)
$$V_{TF} = \frac{f_{yw}\,h_w\,t_w}{\sqrt{3}}\left(\tau_{cr}/\tau_y + \frac{1-\tau_{cr}/\tau_y}{1+\phi_t^2}\right)$$ $$\phi_t = \sqrt{1 + (a/h_w)^2} \approx 1 + 0.5(a/h_w)^2 \quad \text{(simplified for } a/h_w \leq 1.5\text{)}$$
$V_{TF}$ = total shear resistance including tension field (kN). $\tau_y = f_{yw}/\sqrt{3}$ = shear yield stress of web (MPa). $\tau_{cr}$ = critical elastic shear stress from plate buckling theory (MPa). $\phi_t$ = panel geometry factor. Basler's formula shows that as $\tau_{cr}/\tau_y \to 0$ (very slender web), the tension field contribution approaches $f_{yw}\,h_w\,t_w/(\sqrt{3}(1+\phi_t^2))$ - still substantial strength beyond elastic buckling. The post-buckling-to-buckling capacity ratio for typical plate girders ($h_w/t_w \approx 200$, $a/h_w = 1$) is approximately 2 to 3, meaning the post-buckling capacity is 2 to 3 times the elastic buckling load.
Eurocode 3 EN 1993-1-5 Tension Field Shear Resistance (Cl. 5.3)
$$V_{bw,Rd} = \frac{\chi_w\,f_{yw}\,h_w\,t_w}{\sqrt{3}\,\gamma_{M1}}$$ $$V_{bf,Rd} = \frac{0.25\,b_f\,t_f^2\,f_{yf}}{\gamma_{M1}} \cdot \left[\frac{1}{(c/h_w)^2}\right] \quad \text{(flange contribution)}$$ $$c = \frac{a}{2}\left(1 - \frac{V_{Ed}}{V_{bw,Rd} + V_{bf,Rd}}\right)^{0.5} \quad \text{(iterative)}$$ $$V_{b,Rd} = V_{bw,Rd} + V_{bf,Rd} \leq \frac{\eta\,f_{yw}\,h_w\,t_w}{\sqrt{3}\,\gamma_{M1}}$$
$V_{bw,Rd}$ = web contribution to shear resistance (kN). $V_{bf,Rd}$ = flange contribution to shear resistance via plastic hinge formation at panel ends (kN). $b_f$, $t_f$ = flange width and thickness (mm). $f_{yf}$ = flange yield strength (MPa). $c$ = distance of plastic hinge from stiffener (mm). $\gamma_{M1} = 1.10$ (partial factor for instability). The flange contribution $V_{bf,Rd}$ is significant when flanges are stocky: for $b_f = 300$ mm, $t_f = 25$ mm, $f_{yf} = 355$ MPa, $V_{bf,Rd} \approx 80$ to 120 kN - non-negligible for lightly loaded webs. IS 800 does not explicitly include the flange contribution (conservative).
Tension Field Action in a Stiffened Web Panel V V Tension field (diagonal tension) Buckled panel (out-of-plane) Tension field Stiffener (compression strut) θ Post-buckling diagonal tension band anchored between flanges and stiffeners

Why IS 800 permits tension field action (Cl. 8.4.2.2): IS 800:2007 permits the designer to use the higher post-buckling capacity from tension field action, provided rigid end posts (flanged stiffeners at girder ends) are present to anchor the tension field. Without rigid end posts, only the buckling resistance $\chi_w\,f_{yw}\,h_w\,t_w/\sqrt{3}$ can be used. Permitting tension field action typically reduces the number of transverse stiffeners required or allows a thinner web - significant economy for long-span plate girders.

Web Crippling: Mechanisms, Bearing Stress Distribution, and Capacity Formulas

Web crippling (also called web bearing failure or patch loading) occurs when a concentrated transverse force applied through the flange causes the web material directly below to yield in compression or undergo combined local bending and compression. It can occur at three locations in a beam:

  • At an end support (reaction force $R$ transmitted through bearing plate over length $b_1$)
  • Under a point load (interior loading point, load spreads both ways)
  • At column flanges bearing onto beam webs in moment connections

The distinction between web local yielding and web crippling in AISC 360 is important: yielding is ductile and involves web material reaching $f_y$ over the bearing length; crippling is more localised and involves combined stress plus inelastic buckling of the web near the flange-web junction, and is typically more critical for thin webs with small fillets.

IS 800 Web Bearing Capacity (Cl. 8.7.4 - Web Crippling / Local Bearing)
$$F_{cdw} = \frac{(b_1 + n_1)\,t_w\,f_{yw}}{\gamma_{m0}}$$ $$n_1 = 2.5\,(t_f + r) \quad \text{(at end support or concentrated load)}$$ $$n_1 = 5\,(t_f + r) \quad \text{(at interior point load, dispersion both sides)}$$
$F_{cdw}$ = design web bearing capacity (kN). $b_1$ = stiff bearing length (mm): the length over which the load is applied to the flange, assumed to have zero rotation (e.g. bearing plate length, width of supporting member flange). $n_1$ = length of dispersion at 1:2.5 through the flange thickness and root radius to the web toe of fillet. $t_f$ = flange thickness (mm). $r$ = root radius (fillet radius) of rolled section or weld size for built-up section. $t_w$ = web thickness (mm). $f_{yw}$ = web yield strength (MPa). $\gamma_{m0} = 1.10$. Critical check: if $F_{Ed} > F_{cdw}$, a bearing stiffener is mandatory - IS 800 Cl. 8.7.1.
IS 800 Web Buckling Under Concentrated Load (Cl. 8.7.3)
$$F_{cdw,b} = \frac{(b_1 + n_2)\,t_w\,f_{cd}}{\gamma_{m0}}$$ $$n_2 = 2.5\,\left(\frac{h_w}{2}\right) \quad \text{(45° dispersion half depth to neutral axis; conservative)}$$ $$f_{cd} = \frac{\chi\,f_{yw}}{\gamma_{m0}} \quad \text{using column-buckling curve for slenderness } \bar\lambda = \frac{h_w\sqrt{2.5}}{t_w \cdot \sqrt{E/f_{yw}}}$$
The web between the load point and the neutral axis is treated as a strut of length $0.7\,h_w$ (effective length factor 0.7 for fixed-free conditions at web mid-depth under concentric load), width $(b_1 + n_2)$, and thickness $t_w$. $f_{cd}$ = design compressive strength of the web strut computed from IS 800 Cl. 7.1.2 (column buckling curves) for the equivalent slenderness of the web strut. This clause captures the stability (buckling) component of web failure under concentrated load - distinct from the purely strength-based Cl. 8.7.4 check.
AISC 360 Web Local Yielding (Section J10.2) and Web Crippling (Section J10.3)
$$R_n^{WLY} = \begin{cases} (5k + l_b)\,t_w\,F_y & \text{(end reaction, distance} \leq d\text{)} \\ (2.5k + l_b)\,t_w\,F_y & \text{(end reaction)} \end{cases}$$ $$R_n^{WC} = 0.80\,t_w^2\!\left[1 + 3\!\left(\frac{l_b}{d}\right)\!\!\left(\frac{t_w}{t_f}\right)^{1.5}\right]\!\sqrt{\frac{EF_y t_f}{t_w}} \quad \text{(end reaction, } d/2 \text{ from end)}$$
AISC 360 web local yielding ($R_n^{WLY}$): $k$ = distance from outer face of flange to web toe of fillet (mm); $l_b$ = bearing length (mm); $d$ = full depth of member (mm); $F_y$ = yield strength (MPa); $t_w$ = web thickness (mm). The factor 5 applies at interior loading; 2.5 at end reaction. AISC 360 web crippling ($R_n^{WC}$): uses an empirically calibrated formula based on test data from Roberts (1981) and Elgaaly (1983). The $\sqrt{EF_y t_f/t_w}$ term reflects the fact that crippling is a buckling-type failure sensitive to both stiffness (E, $t_f$) and strength ($F_y$). Capacity reduction factor $\phi = 0.75$, so design strength = $0.75\,R_n^{WC}$.

Concentrated Load Dispersion: 1:2.5 Model and Effective Bearing Length

The load dispersion model is the geometric simplification used in all codes to convert the localised contact force at the flange surface into a distributed bearing stress on the web at the toe of the fillet (the critical cross-section for web crippling). The principle is that the load spreads through the flange and root radius at a slope of 1 horizontal : 2.5 vertical (1:2.5 dispersion), giving an effective bearing length at the web toe that is larger than the stiff bearing length $b_1$ at the flange surface.

Load Dispersion Through Flange to Web (IS 800 / EC3 Model) End Reaction b₁ (stiff bearing) R (reaction) b₁ + n₁ t ⁵ + r 1:2.5 slope Interior Point Load F b₁ b₁ + 2n₁ n₁=2.5(t ⁵+r) each side Web toe of fillet is the critical cross-section for both web bearing (crippling) and web buckling checks
Effective Bearing Length at Web Toe of Fillet
$$b_{eff} = b_1 + n_1 \quad \text{(end reaction, IS 800 Cl. 8.7.4)}$$ $$b_{eff} = b_1 + 2\,n_1 \quad \text{(interior point load, dispersion both sides)}$$ $$n_1 = 2.5\,(t_f + r) \quad \text{(rolled sections)}$$ $$n_1 = 2.5\,(t_f + s) \quad \text{(built-up/welded sections; } s = \text{weld size or leg length)}$$
The 1:2.5 dispersion ratio corresponds to a dispersion angle of $\arctan(1/2.5) = 21.8^\circ$ from the vertical - a conservative simplification of the actual stress bulb that spreads through the flange. Eurocode 3 uses a slightly different notation: $s_s$ for stiff bearing length and $s_y$ for the yield resistance length at the web-to-flange junction. Both codes give nearly identical results for standard rolled sections. For built-up plate girders: $r = 0$ (no root radius; flat flange-to-web weld) so $n_1 = 2.5\,t_f + 2.5\,s$ where $s$ is the fillet weld size, typically 6 to 10 mm. This means built-up girders generally have shorter effective bearing lengths and are more susceptible to web crippling than rolled sections of the same dimensions.

IS 800:2007 Design Checks: Clauses 8.4 and 8.7 Step by Step

#CheckIS 800 ClauseFormulaPass Criterion
1Web slenderness classificationCl. 8.4.1 / Table 2$h_w/t_w$ vs $67\varepsilon$, $200\varepsilon$If $\leq 67\varepsilon$: no buckling check. If $> 67\varepsilon$: proceed to check 2.
2Shear buckling check (slender web)Cl. 8.4.2$V_{Ed} \leq V_{db} = \chi_w\,f_{yw}\,h_w\,t_w/(\sqrt{3}\,\gamma_{m0})$$V_{Ed}/V_{db} \leq 1.0$
3High shear plus bending interactionCl. 9.2.2 (if $V > 0.6\,V_d$)$M_d^* = M_{dv} = M_{fd} + M_{wd}(1-(2V/V_d - 1)^2)$$M_{Ed} \leq M_{dv}$: reduced moment capacity under high shear
4Web bearing (crippling) checkCl. 8.7.4$F_{Ed} \leq F_{cdw} = (b_1+n_1)\,t_w\,f_{yw}/\gamma_{m0}$$F_{Ed}/F_{cdw} \leq 1.0$; else provide bearing stiffener
5Web buckling under concentrated loadCl. 8.7.3$F_{Ed} \leq F_{cdw,b} = (b_1+n_2)\,t_w\,f_{cd}/\gamma_{m0}$$F_{Ed}/F_{cdw,b} \leq 1.0$; else provide stiffener or increase $t_w$
6Shear + bending combined (plate girder)Cl. 9.2.1$\left(\frac{V_{Ed}}{V_{bd}}\right)^2 + \left(\frac{M_{Ed}-M_{fd}}{M_{wd}}\right)^2 \leq 1.0$Interaction check for girders where flanges alone resist moment ($M_{fd}$) and web resists shear

IS 800 Slenderness limits summary ($\varepsilon = \sqrt{250/f_y}$): $h_w/t_w \leq 67\varepsilon$ - full plastic shear capacity, no buckling check; $67\varepsilon < h_w/t_w \leq 200\varepsilon$ - shear buckling must be checked; tension field action permitted. $h_w/t_w > 200\varepsilon$ - transverse stiffeners mandatory at spacing $a \leq 1.5\,h_w$; $h_w/t_w > 400$ (with both longitudinal and transverse stiffeners) - absolute maximum per IS 800. For IS 2062 Fe 410 ($f_y = 250$ MPa): $\varepsilon = 1.0$ and the limits are simply 67, 200, and 400.

AISC 360-22 Web Limit States: Shear, Local Yielding, and Web Crippling

Limit StateSectionFormula$\phi$Notes
Shear yielding (compact web)G2.1$V_n = 0.6\,F_y\,A_w\,C_{v1}$; $C_{v1}=1.0$ for $h/t_w \leq 2.24\sqrt{E/F_y}$1.00$A_w = d\cdot t_w$ (gross shear area). No buckling for standard W-shapes.
Shear buckling (slender web)G2.2$V_n = 0.6\,F_y\,A_w\,C_{v2}$; $C_{v2} = \frac{1.51\,k_v\,E}{(h/t_w)^2\,F_y}$ for $h/t_w > 1.37\sqrt{k_v E/F_y}$0.90$k_v = 5.34 + 4/(a/h)^2$ for stiffened; $k_v = 5.34$ unstiffened
Web local yielding (end reaction)J10.2$R_n = (2.5k+l_b)\,t_w\,F_y$1.00$k$ = dist. outer flange face to web toe of fillet
Web local yielding (interior load)J10.2$R_n = (5k+l_b)\,t_w\,F_y$1.00Higher factor 5k for interior loads (dispersion both sides)
Web crippling (end reaction)J10.3$R_n=0.80t_w^2[1+3(l_b/d)(t_w/t_f)^{1.5}]\sqrt{EF_yt_f/t_w}$0.75Empirical; based on Roberts (1981) test data; governs thin webs
Web crippling (interior)J10.3$R_n=0.80t_w^2[1+(l_b/d)(t_w/t_f)^{1.5}/(4)]\sqrt{EF_yt_f/t_w}$0.75Slightly higher than end crippling
Web sidesway bucklingJ10.4$R_n = \frac{C_r\,t_w^3\,t_f}{h^2}[1+0.4(h\,t_w^3/(L_b\,t_f^3))^3]$0.85Governs when compression flange is not braced against rotation at load point; $C_r = 6.62\times10^6$ MPa$^3$
Bearing stiffener requirementJ10.8Stiffener required if any of the above checks failStiffener designed as column; area = stiffener plates + portion of web ($25t_w$ each side)

Eurocode 3 EN 1993-1-5: Shear Resistance and Patch Loading

CheckEN 1993-1-5 ClauseFormula$\gamma_M$
Shear resistance (web contribution)Cl. 5.2$V_{bw,Rd} = \chi_w\,f_{yw}\,h_w\,t_w/(\sqrt{3}\,\gamma_{M1})$; $\chi_w$ from Table 5.1 based on $\bar\lambda_w$$\gamma_{M1}=1.10$
Flange contribution to shearCl. 5.4$V_{bf,Rd} = b_f\,t_f^2\,f_{yf}/(c\,\gamma_{M1})$ where $c = \frac{a}{2}[1 - V_{Ed}/(V_{bw,Rd}+V_{bf,Rd})]^{0.5}$$\gamma_{M1}=1.10$
Minimum web area for shearCl. 5.1 note$h_w/t_w \leq 72\varepsilon/\eta$ ($\eta = 1.2$ for $f_y \leq 460$ MPa): no buckling
Patch loading resistance (crippling)Cl. 6.2$F_{Rd} = f_{yw}\,l_{eff}\,t_w/\gamma_{M1}$; $l_{eff} = \chi_F\,l_y$$\gamma_{M1}=1.10$
Yield resistance length $l_y$Cl. 6.4$l_y = s_s + 2t_f(1 + \sqrt{m_1 + m_2})$ for long bearings; $m_1 = f_{yf}b_f/(f_{yw}t_w)$; $m_2 = 0.02(h_w/t_f)^2$ if $\bar\lambda_F > 0.5$
Reduction factor for patch loading $\chi_F$Cl. 6.3$\chi_F = 0.5/\bar\lambda_F \leq 1.0$; $\bar\lambda_F = \sqrt{l_y\,t_w\,f_{yw}/F_{cr}}$; $F_{cr} = 0.9\,k_F\,E\,t_w^3/h_w$
Buckling coefficient for patch loading $k_F$Cl. 6.4$k_F = 6 + 2(h_w/a)^2$ (rigid end post); $k_F = 3.5 + 2(h_w/a)^2$ (non-rigid end post)

Key EC3 innovation: the $\chi_F$ reduction factor for patch loading explicitly captures the buckling component of web crippling, making the check more physically consistent than the empirical AISC formula. The non-dimensional slenderness $\bar\lambda_F = \sqrt{l_y\,t_w\,f_{yw}/F_{cr}}$ parallels the column slenderness concept: low $\bar\lambda_F$ (stocky web) means $\chi_F = 1.0$ (full yield governs); high $\bar\lambda_F$ (slender web) means $\chi_F < 1.0$ (combined yielding plus buckling). This is conceptually consistent with the EC3 shear buckling reduction factor $\chi_w$ for panels.

Stiffener Design: Bearing, Transverse (Intermediate), and Longitudinal Stiffeners

Stiffeners are flat plates or angles welded to the web of a beam to prevent web buckling or web crippling. Three types are used: bearing stiffeners (at concentrated loads and supports), transverse (intermediate) stiffeners (along the span to reduce shear buckling), and longitudinal stiffeners (for very slender webs in deep plate girders to prevent bending buckling of the compression zone).

Stiffener Types on a Plate Girder Web Bearing stiffener Transverse stiffener (intermediate) → Long. stiffener a (panel spacing) F

Bearing Stiffener Design (IS 800 Cl. 8.7.1 / AISC 360 J10.8)

Bearing Stiffener: Outstand Width and Buckling Check
$$b_s/t_s \leq 14\varepsilon \quad \text{(IS 800 Cl. 8.7.1.2 - local buckling of stiffener outstand)}$$ $$A_{eff,stiff} = 2\,b_s\,t_s + 25\,t_w^2 \quad \text{(AISC: effective strut area = 2 stiffener plates + } 25t_w \text{ web each side)}$$ $$A_{eff,stiff} = 2\,b_s\,t_s + 20\,t_w^2 \quad \text{(EC3 / IS 800 format)}$$ $$l_{eff,strut} = 0.7\,h_w \quad \text{(effective length for column buckling check)}$$ $$r_{strut} = \sqrt{I_{stiff}/A_{eff,stiff}} \quad \Rightarrow \quad \bar\lambda = \frac{l_{eff,strut}}{r_{strut}} \cdot \frac{1}{93.9\,\varepsilon}$$ $$F_{Ed} \leq P_{cd} = A_{eff,stiff} \cdot f_{cd}(\bar\lambda) / \gamma_{m0}$$
$b_s$ = outstand width of one stiffener plate (mm). $t_s$ = stiffener plate thickness (mm). $A_{eff,stiff}$ = effective cross-sectional area of the bearing stiffener strut (stiffener plates + central web strip). The $25t_w$ (AISC) or $20t_w$ (IS 800) web strip accounts for the portion of web that acts with the stiffener as a column. $l_{eff,strut} = 0.7\,h_w$ = effective length of the stiffener treated as a column: 0.7 factor reflects that the web provides partial fixity at top and bottom. $\bar\lambda$ = non-dimensional slenderness of the stiffener strut. $f_{cd}(\bar\lambda)$ = design compressive strength from IS 800 column buckling curves (Table 9c for welded stiffeners). The bearing stiffener must also transmit the bearing force directly: contact bearing check $F_{Ed}/(b_s\,t_s\,f_y/\gamma_{m0}) \leq 1.0$.

Transverse Intermediate Stiffener Design (IS 800 Cl. 8.7.2)

Minimum Stiffener Rigidity and Axial Force in Transverse Stiffener
$$\frac{I_{st}}{t_w^3\,h_w} \geq 1.5\,\left(\frac{h_w}{a}\right)^2 - 0.707 \quad \text{(IS 800 Cl. 8.7.2.4 minimum rigidity criterion)}$$ $$N_{st} = V_{Ed} - \chi_w\,V_{dp} \quad \text{(axial compressive force in stiffener from tension field)}$$ $$A_{st,min} \geq \frac{N_{st}}{f_{yst}/\gamma_{m0}} - \frac{V_{Ed}}{f_{yw}/(\sqrt{3}\,\gamma_{m0})} \cdot t_w \cdot a$$
$I_{st}$ = second moment of area of transverse stiffener (plus contributing web strip) about the web centreline (mm$^4$). $h_w$, $a$ = web depth and panel spacing. The minimum rigidity requirement ensures the stiffener can act as a nodal line for the buckled web panel (i.e. it does not deflect significantly under the tension field reaction forces, which would invalidate the $k_v$ enhancement). $N_{st}$ = axial force in the stiffener from the tension field reaction. For design, transverse stiffeners are typically sized as $b_s \geq h_w/30 + t_f/2$ (outstand), $t_s \geq b_s/(15\varepsilon)$ (AISC guideline), and checked for minimum $I_{st}$ rigidity. Intermediate stiffeners are not in contact with the tension flange at the bottom - they stop 4$t_f$ short of the tension flange to avoid fatigue notch at the weld toe.

Longitudinal Stiffener (IS 800 Cl. 8.7.13)

Longitudinal Stiffener Position and Minimum Rigidity
$$y_1 = 0.2\,h_w \quad \text{(optimum position from compression flange for bending buckling prevention)}$$ $$\frac{I_{st,L}}{t_w^3\,a} \geq 4 \quad \text{(minimum rigidity for single longitudinal stiffener; IS 800)}$$
Longitudinal stiffeners are placed in the compression zone of the web (within the top 20% of depth from the compression flange for a simply supported beam under uniform load). They subdivide the compression zone, reducing the effective height subject to compressive bending stress and dramatically increasing the bending buckling coefficient $k_b$. For a web under linear stress distribution (bending only), $k_b$ increases from 23.9 (unstiffened plate) to approximately 39.6 with one longitudinal stiffener at $0.2h_w$. Longitudinal stiffeners are rarely required for standard rolled sections but are common in very deep plate girders ($h_w > 1500$ mm) used in bridge girders where $h_w/t_w$ may reach 300 to 400.

IS 800 vs AISC 360 vs Eurocode 3: Side-by-Side Comparison

ParameterIS 800:2007AISC 360-22Eurocode 3 EN 1993-1-5
Shear capacity formula$V_{db} = \chi_w f_{yw} h_w t_w/(\sqrt{3}\gamma_{m0})$$V_n = 0.6 F_y A_w C_{v1}$ or $C_{v2}$$V_{b,Rd} = V_{bw,Rd} + V_{bf,Rd}$
Slenderness no-buckling limit$h_w/t_w \leq 67\varepsilon$$h/t_w \leq 2.24\sqrt{E/F_y}$ ($\approx 63$)$h_w/t_w \leq 72\varepsilon/\eta$ ($\approx 60$)
Partial safety factor for shear$\gamma_{m0} = 1.10$ (on yield)$\phi_v = 1.00$ (yield); $0.90$ (buckling)$\gamma_{M0} = 1.00$; $\gamma_{M1} = 1.10$ (buckling)
Tension field actionPermitted (Cl. 8.4.2.2) with rigid end postsNot explicitly in shear chapter; included implicitly via $C_{v2}$ for stiffened websExplicitly included as $V_{bf,Rd}$ flange contribution (Cl. 5.4)
Web bearing (crippling) capacity$F_{cdw} = (b_1+n_1)t_w f_{yw}/\gamma_{m0}$; Cl. 8.7.4$R_n = 0.80t_w^2[1+3(l_b/d)(t_w/t_f)^{1.5}]\sqrt{EF_yt_f/t_w}$; $\phi=0.75$$F_{Rd} = f_{yw}l_{eff}t_w/\gamma_{M1}$; $l_{eff} = \chi_F l_y$ from patch loading model
Dispersion ratio1:2.5 through flange+root (Cl. 8.7.1.3)$k$ = distance outer flange face to web toe$s_y$ via $m_1$, $m_2$ parameters (Cl. 6.4)
Bearing stiffener effective strut area$2b_s t_s + 20t_w^2$ (IS 800)$2b_s t_s + 25t_w^2$ (AISC)$2b_s t_s + 15\varepsilon t_w^2$ (EC3)
Intermediate stiffener rigidity$I_{st}/(t_w^3 h_w) \geq 1.5(h_w/a)^2 - 0.707$$I_{st} \geq at_w^3/(10.92)$ (simplified)$I_{st} \geq 1.5h_w^3 t_w^3/a^2$ (Cl. 9.3)
Max $h_w/t_w$ (no longitudinal stiffener)200 ($f_y = 250$ MPa)260 (practical limit; no code max)$\approx 200/\varepsilon$ typical; no hard limit but checks intensify
Material $\varepsilon$ factor$\varepsilon = \sqrt{250/f_y}$$\sqrt{E/(0.6F_y)} \cdot 1/\sqrt{k_v}$ used in limits$\varepsilon = \sqrt{235/f_y}$ (based on 235 MPa reference)

Key difference in web crippling approach: IS 800 uses a straightforward bearing yield formula with dispersion ($F_{cdw}$) plus a separate strut buckling check ($F_{cdw,b}$) - simple and transparent. AISC uses a single empirical formula calibrated to test data, which inherently combines yielding and buckling effects but is less physically transparent. EC3 uses the most physically rigorous approach with the $\chi_F$ reduction factor explicitly capturing the buckling component, analogous to column buckling theory. For normal rolled sections, all three codes give results within 10 to 15% of each other; differences become more significant for very thin built-up webs ($t_w < 8$ mm) where buckling governs over yielding.

Worked Examples: Web Check for ISMB 500 and Plate Girder

Example 1 - ISMB 500 rolled beam, IS 800:2007: Beam: ISMB 500 ($h = 500$ mm, $b_f = 180$ mm, $t_f = 17.2$ mm, $t_w = 10.2$ mm, $r = 17$ mm). Steel: IS 2062 Fe 410, $f_y = 250$ MPa. Applied end reaction $F_{Ed} = 350$ kN (bearing length $b_1 = 100$ mm). Check (a) shear buckling; (b) web bearing; (c) web buckling under concentrated load.

Example 1 - Step by Step (IS 800:2007)

1

Web slenderness check:
$h_w = h - 2t_f = 500 - 2\times17.2 = 465.6$ mm
$h_w/t_w = 465.6/10.2 = \mathbf{45.6}$
$\varepsilon = \sqrt{250/250} = 1.0$; limit $= 67\varepsilon = 67$
$45.6 < 67$ → No shear buckling check required. Full plastic shear capacity governs.
$V_{dp} = f_y\,h_w\,t_w/(\sqrt{3}\,\gamma_{m0}) = 250\times465.6\times10.2/(\sqrt{3}\times1.10) = 625{,}267\,\text{N} = \mathbf{625}$ kN

2

Web bearing capacity (Cl. 8.7.4):
$n_1 = 2.5(t_f + r) = 2.5(17.2 + 17) = 2.5\times34.2 = 85.5$ mm (end reaction, dispersion one side only)
$b_{eff} = b_1 + n_1 = 100 + 85.5 = \mathbf{185.5}$ mm
$F_{cdw} = b_{eff}\times t_w\times f_y/\gamma_{m0} = 185.5\times10.2\times250/1.10 = 429{,}295\,\text{N} = \mathbf{429.3}$ kN
$F_{Ed} = 350$ kN $< 429.3$ kN → Web bearing OK (ratio = 0.815)

3

Web buckling under concentrated load (Cl. 8.7.3):
$n_2 = 2.5\,(h_w/2) = 2.5\times232.8 = 582$ mm (45° dispersion to neutral axis; capped at available length)
Strut slenderness: $\bar\lambda = \frac{0.7\,h_w}{\pi\,t_w}\sqrt{12(1-\nu^2)/k} \approx \frac{0.7\times465.6}{3.46\times10.2} = \mathbf{9.26}$ (treating web as strut, IS 800 Cl. 8.7.3 simplified $\bar\lambda = \frac{h_w\sqrt{2.5}}{t_w}\cdot\frac{1}{\sqrt{E/f_y}} = \frac{465.6\times1.581}{10.2}\times\frac{1}{\sqrt{820}} = \mathbf{2.51}$)
From IS 800 column curve c (welded sections): at $KL/r \approx 2.51$ → $f_{cd} \approx 248$ MPa (nearly full yield; very stocky strut)
$F_{cdw,b} = (b_1 + n_2)\times t_w\times f_{cd}/\gamma_{m0} = (100+582)\times10.2\times248/1.10 = 1{,}574{,}400\,\text{N} = 1{,}574$ kN
$350 \ll 1{,}574$ kN → Web buckling under load OK

4

Summary for ISMB 500: All three checks pass. The ISMB 500 is a compact rolled section with $h_w/t_w = 45.6$ well below 67 - typical for standard rolled beams which are deliberately sized to avoid web buckling. Stiffeners are not required for this loading. If the reaction were increased to $> 429$ kN, a bearing stiffener would be required.

Example 2 - Welded plate girder, IS 800:2007: Plate girder: $h_w = 1200$ mm, $t_w = 10$ mm, $b_f = 400$ mm, $t_f = 25$ mm (welded, $r = 0$, fillet weld $s = 8$ mm). Steel: IS 2062 Fe 410, $f_y = 250$ MPa. Transverse stiffeners at $a = 1000$ mm. End reaction $F_{Ed} = 800$ kN. Bearing length $b_1 = 150$ mm. Check all web limit states.

Example 2 - Plate Girder Web Checks

1

Web slenderness:
$h_w/t_w = 1200/10 = \mathbf{120}$
$67\varepsilon = 67$; $200\varepsilon = 200$
$67 < 120 < 200$ → Shear buckling check required; tension field action permitted

2

Shear buckling coefficient and critical stress:
$a/h_w = 1000/1200 = 0.833 < 1.0$ → use $k_v = 4.00 + 5.34/(a/h_w)^2 = 4.00 + 5.34/0.694 = 4.00 + 7.70 = \mathbf{11.70}$
$\tau_{cr} = k_v\times\frac{189{,}800\,t_w^2}{h_w^2} = 11.70\times\frac{189{,}800\times100}{1{,}440{,}000} = 11.70\times13.18 = \mathbf{154.3}$ MPa
$\tau_y = f_y/\sqrt{3} = 250/1.732 = 144.3$ MPa
Note: $\tau_{cr} = 154.3 > \tau_y = 144.3$ MPa → this panel actually yields before elastic buckling (closely stiffened panel). $\bar\lambda_w = \sqrt{\tau_y/\tau_{cr}} = \sqrt{144.3/154.3} = \mathbf{0.967}$

3

Shear reduction factor and capacity:
$\bar\lambda_w = 0.967$; $0.83 \leq 0.967 < 1.08$ → inelastic range: $\chi_w = 0.83/(\sqrt{3}\times0.967) = 0.83/1.675 = \mathbf{0.496}$
$V_{db} = \chi_w\times f_y\times h_w\times t_w/(\sqrt{3}\times\gamma_{m0}) = 0.496\times250\times1200\times10/(\sqrt{3}\times1.10)$
$= 0.496\times250\times12{,}000/1.905 = 781{,}626\,\text{N} = \mathbf{782}$ kN
Applied $V_{Ed} = 800$ kN $>$ 782 kN → Shear buckling marginal FAIL (ratio = 1.023). Options: (a) reduce stiffener spacing $a$ to increase $k_v$; (b) increase $t_w$ to 11 mm; (c) invoke tension field action.

4

Web bearing capacity (Cl. 8.7.4):
$n_1 = 2.5(t_f + s) = 2.5(25 + 8) = 82.5$ mm (welded plate girder; $r = 0$, $s = 8$ mm weld)
$b_{eff} = b_1 + n_1 = 150 + 82.5 = \mathbf{232.5}$ mm
$F_{cdw} = 232.5\times10\times250/1.10 = 528{,}409\,\text{N} = \mathbf{528}$ kN
$F_{Ed} = 800$ kN $>$ 528 kN → Web bearing FAILS (ratio = 1.515). Bearing stiffener required.

5

Bearing stiffener design (Cl. 8.7.1):
Required force $= F_{Ed} - F_{cdw} = 800 - 528 = 272$ kN to be resisted by stiffener.
Try stiffener: $b_s = 140$ mm, $t_s = 12$ mm (two plates, one each side of web):
Outstand check: $b_s/t_s = 140/12 = 11.7 < 14\varepsilon = 14$ → OK (no local buckling)
Effective strut area: $A_{eff} = 2\times140\times12 + 20\times10^2 = 3{,}360 + 2{,}000 = 5{,}360$ mm$^2$
$I_{stiff} = 2\times[12\times140^3/12 + 12\times140\times(70+5)^2] = 2\times[3{,}073{,}333 + 9{,}450{,}000] = 24{,}047{,}000$ mm$^4$
$r_{stiff} = \sqrt{I/A} = \sqrt{24{,}047{,}000/5{,}360} = \sqrt{4{,}486} = 67.0$ mm
Effective length: $l_{eff} = 0.7\times1200 = 840$ mm; $KL/r = 840/67.0 = 12.5$
From IS 800 Table 9c (curve c): $f_{cd} \approx 226$ MPa at $KL/r = 12.5$
$P_{cd} = 5{,}360\times226/1.10 = 1{,}100{,}727\,\text{N} = 1{,}101$ kN $> F_{Ed} = 800$ kN → Bearing stiffener OK

Web Buckling & Web Crippling Check Calculator (IS 800:2007)

Web Check Calculator - IS 800:2007

Enter beam and loading parameters to check shear buckling (Cl. 8.4), web bearing (Cl. 8.7.4), and web buckling under concentrated load (Cl. 8.7.3).

Section type
Web depth hₗ (mm)
Web thickness tₗ (mm)
Flange thickness tₘ (mm)
Root radius r / weld s (mm)
Stiffener spacing a (mm)
Yield strength fₘ (MPa)
Design shear Vₚᵈ (kN)
Concentrated load Fₚᵈ (kN)
Bearing length b₁ (mm)
Load position
γₘ₀ (partial safety factor)

Frequently Asked Questions

1. What is web buckling and what causes it in steel beams?

Web buckling is an out-of-plane stability failure of the thin web plate of a steel I-beam or plate girder. It occurs when in-plane compressive stresses in the web reach the critical elastic buckling stress of the plate. The compressive stresses arise from two sources: shear forces (shear buckling - the dominant mode in most beams), where the pure shear state is equivalent to equal diagonal tension and compression at 45°, and the compression component can buckle the web diagonally; and bending (flexural/bending buckling of the web compression zone), relevant only in very deep slender webs where the web itself carries significant bending compression. Web buckling is governed by the web slenderness ratio h_w/t_w (clear web depth divided by web thickness) and the panel aspect ratio a/h_w (stiffener spacing divided by web depth). Higher h_w/t_w means lower critical buckling stress (which scales as (t_w/h_w)^2 from elastic plate theory), making thin webs highly susceptible. IS 800:2007 requires a shear buckling check when h_w/t_w exceeds 67*epsilon where epsilon = sqrt(250/f_y).

2. What is web crippling and how does it differ from web buckling?

Web crippling (also called web bearing failure or web crushing) is a localised strength failure of the web directly under a concentrated transverse force at a support or point load location. It involves the web material yielding in direct compression within the bearing length, sometimes combined with local instability of the web near the flange-web junction. The critical parameters are the stiff bearing length b_1 (the length over which the load contacts the flange), the web thickness t_w, and the web yield strength f_y. The difference from web buckling is fundamental: web buckling is a stability (eigenvalue) problem governed by the elastic plate buckling theory and the E*(t_w/h_w)^2 stiffness term; web crippling is primarily a strength problem governed by f_y*t_w*b_eff. Web buckling can involve a large panel of the web and gives a wrinkle or bulge pattern over the panel; web crippling is strictly localised to the bearing region and gives a visible dent or crush at the web toe of fillet. Both can occur simultaneously and both are checked at support and load points - IS 800 uses Cl. 8.4 for shear buckling and Cl. 8.7 for web bearing.

3. What is the h_w/t_w slenderness limit in IS 800 and what happens if it is exceeded?

IS 800:2007 classifies web slenderness as follows, where epsilon = sqrt(250/f_y): h_w/t_w <= 67*epsilon - compact or plastic web; no shear buckling check required; full plastic shear capacity V_dp = f_y*h_w*t_w/(sqrt(3)*gamma_m0) applies. 67*epsilon < h_w/t_w <= 200*epsilon - semi-compact to slender; shear buckling check required per Cl. 8.4.2; reduced capacity V_db = chi_w*f_y*h_w*t_w/(sqrt(3)*gamma_m0) where chi_w is the shear reduction factor based on the non-dimensional slenderness lambda_w; tension field action may be invoked to recover post-buckling capacity. h_w/t_w > 200*epsilon - transverse stiffeners mandatory at spacing a <= 1.5*h_w; with stiffeners the effective h/t is reduced for each panel. h_w/t_w > 400 - both transverse and longitudinal stiffeners are required. For IS 2062 Fe 410 steel (f_y = 250 MPa), epsilon = 1.0 and the limits are simply 67, 200, and 400. Most standard rolled I-sections (ISMB series) have h_w/t_w in the range 30 to 55, well below 67, so no buckling check is needed. Plate girders typically have h_w/t_w of 100 to 200, requiring full buckling checks.

4. What is tension field action and when can it be used?

Tension field action (also called diagonal tension field or post-buckling reserve) is the additional shear resistance that a web panel develops after elastic shear buckling has occurred. After the web buckles at tau_cr, it can no longer carry shear by membrane compression in the diagonal direction, but the orthogonal diagonal tension can still be mobilised. This diagonal tension band - anchored between the flanges and transverse stiffeners at the panel corners - acts like the diagonal tension members of a Pratt truss. The additional shear capacity from tension field action can be 2 to 3 times the elastic buckling load for very slender webs. IS 800:2007 Cl. 8.4.2.2 explicitly permits tension field action to be used in design, provided rigid end posts (full-depth stiffeners with flanged end plates at the girder ends) are provided to anchor the tension field. Without rigid end posts, only the elastic buckling capacity chi_w*V_dp is available. Permitting tension field action allows significantly more economical plate girder designs by reducing the required number of intermediate stiffeners or allowing thinner webs. Eurocode 3 includes the flange contribution V_bf,Rd as an additional term capturing the moment capacity of the flanges in resisting the horizontal component of the tension field force.

5. How do I calculate the effective bearing length for web crippling checks?

The effective bearing length b_eff at the web toe of fillet is computed by adding the stiff bearing length b_1 (the length of direct contact between the flange and the supporting/loaded element) to the dispersion length n_1 through the flange thickness and root radius. The IS 800 dispersion model uses a 1:2.5 slope (1 horizontal : 2.5 vertical): n_1 = 2.5*(t_f + r) for rolled sections, or n_1 = 2.5*(t_f + s) for welded sections where s is the fillet weld size. For end reactions (dispersion on one side only): b_eff = b_1 + n_1. For interior point loads (dispersion on both sides): b_eff = b_1 + 2*n_1. Example for ISMB 500 (t_f = 17.2 mm, r = 17 mm) with b_1 = 100 mm at end: n_1 = 2.5*(17.2+17) = 85.5 mm; b_eff = 100 + 85.5 = 185.5 mm. The web bearing capacity is then F_cdw = b_eff * t_w * f_y / gamma_m0. The physical basis of the 1:2.5 slope is that the stiff flange plate distributes the concentrated bearing force at a shallow angle through its depth, and the 1:2.5 ratio (21.8 degrees from vertical) is a conservative lower bound on the actual stress bulb angle.

6. When is a bearing stiffener required and how is it designed?

A bearing stiffener is required when the concentrated transverse force at a support or load point exceeds either the web bearing capacity F_cdw (IS 800 Cl. 8.7.4) or the web buckling capacity under the concentrated load F_cdw,b (IS 800 Cl. 8.7.3). In practice, bearing stiffeners are almost always required for plate girder supports and for column connections to beams carrying heavy loads. Design of a bearing stiffener per IS 800: (1) Determine the stiffener force = F_Ed - F_cdw (the force in excess of the unstiffened web capacity). (2) Proportion the stiffener plates: outstand b_s and thickness t_s must satisfy b_s/t_s <= 14*epsilon to prevent local buckling of the stiffener outstand itself. (3) Compute the effective strut cross-section: A_eff = 2*b_s*t_s + 20*t_w^2 (stiffener plates plus a 20t_w wide web strip acting as a column). (4) Compute the effective length of the strut: l_eff = 0.7*h_w (0.7 factor for partial end fixity from web and flanges). (5) Find the slenderness ratio KL/r of the effective strut and read the design compressive strength f_cd from IS 800 Table 9 (curve c for welded stiffeners). (6) Check P_cd = A_eff * f_cd / gamma_m0 >= F_Ed. The bearing stiffener should be welded to both flanges but must not be welded to the tension flange (weld the end of the stiffener to a cleat or leave a small gap) to avoid fatigue issues at the tension flange weld toe.

7. What is the plate buckling coefficient k_v and how does it depend on stiffener spacing?

The plate buckling coefficient k_v is a dimensionless factor that captures the effect of boundary conditions and aspect ratio on the critical shear buckling stress of a web panel. It enters the critical stress formula as tau_cr = k_v * pi^2 * E / [12*(1-nu^2)] * (t_w/h_w)^2. For a simply-supported rectangular plate under pure shear, k_v depends on the panel aspect ratio alpha_0 = a/h_w (stiffener spacing / web depth): for a/h_w >= 1: k_v = 5.34 + 4.00/(a/h_w)^2; for a/h_w < 1: k_v = 4.00 + 5.34/(a/h_w)^2. For an unstiffened web (a/h_w approaching infinity): k_v = 5.34 (minimum value). For a square panel (a/h_w = 1): k_v = 9.34 (75% higher critical stress). For a/h_w = 0.5: k_v = 4.00 + 5.34/0.25 = 25.4 (very high; closely stiffened). The practical implication: adding transverse stiffeners at spacing a = h_w converts k_v from 5.34 to 9.34, nearly doubling the critical shear buckling stress for the same web dimensions. However, reducing spacing further to a = 0.5*h_w gives k_v = 25.4 - a further 172% increase - but with twice as many stiffeners. Engineers balance the economy of fewer stiffeners (lower fabrication cost) against the higher web thickness needed (higher material cost).

8. What is the shear buckling coefficient chi_w and how is it related to lambda_w?

The shear reduction factor chi_w (0 < chi_w <= 1) represents the ratio of the actual shear resistance to the full plastic shear resistance, accounting for elastic or inelastic buckling of the web. It is a function of the non-dimensional web slenderness lambda_w = sqrt(tau_y/tau_cr) = h_w/(86.4*epsilon*sqrt(k_v)*t_w). Three regimes exist: (1) lambda_w <= 0.6 (stocky web): chi_w = 1.0; full shear yield governs; no buckling. (2) 0.6 < lambda_w < 1.08 (inelastic buckling): chi_w reduces from 1.0 to about 0.77; both yielding and buckling interact; the curve follows chi_w = 0.83/(sqrt(3)*lambda_w) per IS 800 simplified form. (3) lambda_w >= 1.08 (elastic buckling governs): chi_w = 1.37/(sqrt(3)*(0.7 + lambda_w)); further reduction as slenderness increases. The resulting design shear resistance is V_db = chi_w * f_y * h_w * t_w / (sqrt(3) * gamma_m0). For a plate girder with h_w/t_w = 150 (unstiffened, k_v = 5.34): lambda_w = 150/(86.4*1.0*sqrt(5.34)) = 150/199.6 = 0.75; chi_w = 0.83/(1.732*0.75) = 0.639; V_db = 0.639 * V_dp - the unstiffened web can only carry 64% of its plastic shear capacity.

9. How do AISC 360, IS 800, and Eurocode 3 differ in their web crippling checks?

The three codes use fundamentally different approaches, though giving similar results for standard cases. IS 800 uses a two-step approach: first a bearing (yield) check F_cdw = b_eff * t_w * f_y / gamma_m0 (direct bearing yield at the web toe), then separately a buckling check treating the web as a strut using column buckling curves. This is physically transparent but involves two separate calculations. AISC 360 uses a single empirical formula R_n = 0.80*t_w^2*[1+3*(l_b/d)*(t_w/t_f)^1.5]*sqrt(E*F_y*t_f/t_w) with phi = 0.75. This formula was calibrated against laboratory test data and implicitly combines yielding and buckling effects. It is convenient for calculation but less physically transparent. Eurocode 3 EN 1993-1-5 uses the most physically rigorous approach: the patch loading model with a non-dimensional slenderness lambda_F = sqrt(l_y*t_w*f_y/F_cr) and a reduction factor chi_F = 0.5/lambda_F (capped at 1.0), exactly analogous to the column buckling model but calibrated for patch loading. F_cr = 0.9*k_F*E*t_w^3/h_w captures the elastic buckling component. For standard rolled sections all three give results within 10 to 15% of each other. For thin welded plate girder webs the EC3 and IS 800 buckling checks become more critical and give more conservative results than the AISC empirical formula.

10. What is web sidesway buckling and when does it govern?

Web sidesway buckling (AISC 360 Section J10.4) is a lateral buckling mode that involves the compression flange rotating sideways relative to the tension flange at the point of a concentrated load, with the web deforming laterally in a sway mode rather than in the classical shear wrinkle pattern. It occurs when the compression flange is not restrained against rotation at the concentrated load point - for example, when a heavy point load is applied mid-span on a beam with good lateral restraint at the supports but none at the load point. The governing slenderness parameter is (h/t_w)/(L_b/b_f) where L_b is the distance between points of lateral restraint of the compression flange. When this ratio is small (relatively rigid web, closely braced), sidesway buckling is not critical. When (h*t_w^3)/(L_b*t_f^3) is large, the capacity is substantially reduced. Web sidesway buckling is relevant primarily for long-span beams with widely spaced bracing and concentrated mid-span loads - crane runway girders and transfer beams are typical cases. IS 800 and EC3 do not have a specific web sidesway buckling clause; designers using these codes typically address it through lateral restraint requirements at load points (IS 800 Cl. 8.3.1 on lateral-torsional buckling restraint).

11. Why is web crippling more critical for welded plate girders than for rolled sections?

Web crippling capacity at a support or load point depends on the effective bearing length b_eff = b_1 + n_1, where n_1 = 2.5*(t_f + r) for rolled sections (with root radius r) or n_1 = 2.5*(t_f + s) for welded sections (with weld size s). For a rolled section like ISMB 500 with t_f = 17.2 mm and r = 17 mm: n_1 = 2.5*(17.2+17) = 85.5 mm - the root radius adds 42.5 mm to the dispersion length. For a welded plate girder with the same t_f = 17.2 mm but only an 8 mm fillet weld (s = 8 mm): n_1 = 2.5*(17.2+8) = 63.0 mm - only 22.5 mm from the weld, roughly 26% less dispersion. The larger root radius of rolled sections thus provides substantially more bearing area at the web toe, giving higher F_cdw capacity. Additionally, plate girder webs are intentionally thinner than equivalent rolled section webs (higher h_w/t_w ratios are economical for long spans), meaning both t_w (directly in the F_cdw formula) and the dispersion area are smaller. The combination typically means welded plate girders always require bearing stiffeners at supports while rolled section beams may not, depending on the reaction magnitude.

12. What is the role of transverse stiffeners in plate girder design?

Transverse (intermediate) stiffeners serve two distinct functions in plate girder design: (1) Shear buckling control: by dividing the long web into shorter panels, transverse stiffeners increase the panel aspect ratio h_w/a (or equivalently reduce a/h_w), which increases the shear buckling coefficient k_v = 5.34 + 4/(a/h_w)^2 (for a/h_w >= 1). A smaller panel has a higher critical shear buckling stress, allowing the web to carry more shear before buckling. (2) Tension field action anchoring: in post-buckled panels, transverse stiffeners act as the compression struts in the diagonal tension truss mechanism, resisting the compressive reaction from the diagonal tension bands. Without transverse stiffeners there is no anchor for tension field action, and the web behaves as an unstiffened panel limited to k_v = 5.34. Design requirements: (a) Minimum rigidity: I_st/(t_w^3*h_w) >= 1.5*(h_w/a)^2 - 0.707 per IS 800 Cl. 8.7.2.4, ensuring the stiffener acts as a nodal line without excessive deflection. (b) Axial force from tension field: N_st = V_Ed - chi_w*V_dp must be carried by the stiffener. (c) Outstand limit: b_s/t_s <= 14*epsilon to prevent local buckling of the stiffener plate. (d) Intermediate stiffeners must not be welded to the tension flange - stop 4*t_f short to avoid fatigue notch.

13. What are the absolute h_w/t_w limits in Indian practice and why?

IS 800:2007 sets the following absolute limits on web slenderness. For webs without any longitudinal stiffener: h_w/t_w <= 200*epsilon (for Fe 410: 200). This is the practical maximum for a web relying only on transverse stiffeners for shear buckling control. For webs with a single longitudinal stiffener at 0.2*h_w from the compression flange: h_w/t_w <= 250*epsilon. For webs with two longitudinal stiffeners: h_w/t_w <= 400*epsilon. The physical basis for these limits relates to fabrication and handling: very thin webs with h_w/t_w > 200 are difficult to weld without distortion, have significant initial geometric imperfections from welding, are sensitive to minor out-of-plumb of stiffeners, and behave in a complex interaction between shear buckling and bending buckling modes that is difficult to analyse reliably. In Indian bridge practice (IRC 24 for steel bridges, which references IS 800), plate girder webs with h_w/t_w of 150 to 180 are common, with longitudinal stiffeners provided for deeper girders. The Bandra-Worli Sea Link and major railway bridges use plate girders with h_w/t_w of 120 to 160 and two sets of transverse stiffeners.

14. How does the combination of high shear and high bending affect web design?

When a cross-section is simultaneously subjected to high shear force and high bending moment, the two interact and reduce the capacity for each. IS 800:2007 Cl. 9.2.2 specifies a moment-shear interaction for the case where V_Ed > 0.6*V_d (shear exceeds 60% of shear capacity): the design moment capacity is reduced from M_d to M_dv = M_fd + M_wd*(1 - (2*V/V_d - 1)^2), where M_fd = moment capacity of the flanges alone (flanges carry all the bending without web contribution) and M_wd = moment capacity contribution from the web alone. For a plate girder specifically (Cl. 9.2.1), the interaction check is: (V_Ed/V_bd)^2 + (M_Ed - M_fd)/M_wd <= 1.0. Physical basis: under combined high shear and bending, the von Mises yield criterion limits the simultaneous stress components. In the web: bending stress sigma = (M/I)*y and shear stress tau = V*Q/(I*t_w) must satisfy sqrt(sigma^2 + 3*tau^2) <= f_y. This interaction is most critical at the neutral axis (maximum tau, zero sigma) and at the web-flange junction (maximum sigma, moderate tau). High-shear zones in long-span plate girders (near supports) rarely coincide with high-bending zones (near mid-span), so interaction effects are usually small for simply supported beams. However, in continuous beams and frames, regions near interior supports have both high shear and high negative bending, making interaction checks critical.

15. What is the minimum web thickness recommended for steel beams in IS 800?

IS 800:2007 does not specify an absolute minimum web thickness directly, but practical minimums emerge from multiple requirements: Corrosion protection: for exposed structures without protective coatings, IS 800 Cl. 15.9.2 recommends a corrosion allowance of 1 to 2 mm, suggesting a practical minimum of t_w >= 6 to 8 mm for exposed outdoor structures. Web buckling control: requiring h_w/t_w <= 200 for a web without longitudinal stiffeners sets t_w >= h_w/200. For h_w = 1000 mm: t_w >= 5 mm; for h_w = 2000 mm: t_w >= 10 mm. Web bearing at supports: for typical reactions on plate girders, F_cdw = b_eff*t_w*f_y/gamma_m0 must be adequate or stiffeners provided. Thin webs may require bearing stiffeners at every support even for moderate reactions. Weld-to-thickness ratio: AWS D1.1 and IS 816 limit the minimum weld size to a function of the thicker connected part; very thin webs limit the achievable weld strength. Fabrication: webs thinner than 6 mm are prone to welding distortion that is difficult to correct. In practice for rolled sections: minimum t_w is 5.7 mm (ISJB 150, lightest standard section); for plate girders: 8 to 10 mm is practical minimum. Highway bridge plate girders per IRC 24 typically use t_w >= 10 mm.

16. What are the consequences of ignoring web buckling or crippling in design?

Ignoring web buckling or crippling checks in steel beam design can lead to several progressive failure consequences: web buckling - the first sign is visible diagonal wrinkling or bulging of the web panel under service loads, which may go unnoticed in concealed construction. As load increases, the buckled web panel loses stiffness; deflections increase disproportionately; eventually the tension field in adjacent panels becomes overloaded; a fracture-line type plastic hinge mechanism forms across the web; the beam loses shear capacity suddenly or progressively. For ductile failure (gradual progression), some warning exists; for slender high-strength steel webs, failure can be more sudden. Web crippling - initial sign is a visible dent or indentation at the bearing point; the web begins to yield and crush; without redistribution, the beam loses vertical support at that point; settlement of the supported structure occurs; progressive collapse of the loading system is possible. In structural assessments, both failures have been observed in light industrial buildings, crane runway girders, and cold-formed steel purlins (where the thin gauge makes crippling critical). All major codes (IS 800, AISC 360, Eurocode 3, BS 5950) have mandatory checks for these limit states - non-compliance is not a conservative simplification but a genuine safety hazard.

17. What is patch loading and how is it treated in Eurocode 3?

Patch loading is the EC3 terminology for web crippling under a concentrated transverse force applied through the flange over a finite length. It is treated in EN 1993-1-5 Chapter 6 using a buckling-based reduction approach: the resistance is F_Rd = f_yw * l_eff * t_w / gamma_M1 where l_eff = chi_F * l_y is the effective loaded length. The yield resistance length l_y is the length of web at the web-to-flange junction that would yield under the applied force (computed from l_y = s_s + 2*t_f*(1 + sqrt(m_1 + m_2)) where m_1 = f_yf*b_f/(f_yw*t_w) and m_2 = 0.02*(h_w/t_f)^2 for lambda_F > 0.5). The reduction factor chi_F = 0.5/lambda_F (capped at 1.0) is based on the non-dimensional slenderness lambda_F = sqrt(l_y*t_w*f_yw/F_cr) where F_cr = 0.9*k_F*E*t_w^3/h_w. The buckling coefficient k_F = 6 + 2*(h_w/a)^2 for end-supported panels with a rigid end post, or 3.5 + 2*(h_w/a)^2 without rigid end post. The EC3 patch loading model is the result of extensive research at Cardiff University (Roberts, Rockey) and Luleå University of Technology (Lagerqvist, Johansson) and is considered the most comprehensive and physically consistent model available for patch loading resistance of plate girder webs.

18. How does flange thickness affect web crippling resistance?

Flange thickness affects web crippling resistance through multiple mechanisms in all three codes. Direct dispersion: the IS 800 effective bearing length n_1 = 2.5*(t_f + r) increases linearly with flange thickness, directly increasing b_eff and hence F_cdw. For a 10 mm increase in t_f: n_1 increases by 25 mm, adding approximately 25*t_w*f_y/gamma_m0 kN to F_cdw (for t_w = 10 mm, f_y = 250 MPa: approximately +56.8 kN per 10 mm increase in flange thickness). AISC 360: the web crippling formula R_n = 0.80*t_w^2*[...]*sqrt(E*F_y*t_f/t_w) increases as sqrt(t_f) - thicker flanges give higher crippling resistance, reflecting the role of the flange in distributing load and providing rotational restraint at the web-flange junction. Eurocode 3: the parameter m_1 = f_yf*b_f/(f_yw*t_w) in the yield resistance length l_y is independent of t_f, but m_2 = 0.02*(h_w/t_f)^2 decreases with increasing t_f (thicker flanges reduce the correction for intermediate slenderness). Additionally, thicker flanges provide more rotational rigidity at the web-flange junction, which effectively increases the boundary condition stiffness for the web panel from simply-supported toward partially fixed, increasing the buckling coefficient and hence k_F. In practical design, providing thicker flanges is one effective way to improve web crippling resistance without changing the web dimensions.

19. What is the difference between a bearing stiffener and a transverse stiffener?

Bearing stiffeners and transverse intermediate stiffeners both consist of flat plates welded to the web, but they serve different functions, are located at different positions, and are designed differently. Bearing stiffeners are provided specifically at concentrated load points and at end supports. Their primary function is to resist web crippling and web buckling under the concentrated force. They must be welded to both flanges (or to cleats bolted to flanges) to transfer the concentrated load directly from flange to stiffener without relying on the web alone. They are designed as columns (struts) under the full concentrated load, treating an effective strut section of 2*b_s*t_s + 20*t_w^2 with effective length 0.7*h_w. The outstand must satisfy b_s/t_s <= 14*epsilon to prevent local buckling. Transverse intermediate stiffeners are provided along the span between support stiffeners to divide the web into shorter panels and increase the shear buckling coefficient k_v. They carry axial compression from tension field action (N_st = V_Ed - chi_w*V_dp) but not direct vertical forces from external loads. They need only satisfy the minimum rigidity criterion I_st/(t_w^3*h_w) >= 1.5*(h_w/a)^2 - 0.707 and must not be welded to the tension flange. They are lighter and simpler than bearing stiffeners. In a typical plate girder design: bearing stiffeners are always required at the end supports; intermediate stiffeners are added as needed to achieve adequate shear capacity along the span, with spacing chosen to balance fabrication cost against material savings.

Key References

Bryan, G.H. (1891). On the stability of a plane plate under thrusts in its own plane, with applications to the buckling of the sides of a ship. Proceedings of the London Mathematical Society, 22(1), 54 to 67.

Timoshenko, S.P. and Gere, J.M. (1961). Theory of Elastic Stability, 2nd edition. McGraw-Hill, New York.

Basler, K. (1961). Strength of plate girders in shear. Journal of the Structural Division, ASCE, 87(ST7), 151 to 180.

Wagner, H. (1929). Flat sheet metal girders with very thin webs. Zeitschrift fur Flugtechnik und Motorluftschiffahrt, 20, 200 to 314 (translated as NACA TM 604 to 606, 1931).

Roberts, T.M. (1981). Slender plate girders subjected to edge loading. Proceedings of the Institution of Civil Engineers, 71(2), 805 to 819.

Rockey, K.C., Evans, H.R. and Porter, D.M. (1978). A design method for predicting the collapse behaviour of plate girders. Proceedings of the Institution of Civil Engineers, 65(1), 85 to 112.

BIS (2007). IS 800: General Construction in Steel - Code of Practice (3rd revision). Bureau of Indian Standards, New Delhi.

AISC (2022). Specification for Structural Steel Buildings (AISC 360-22). American Institute of Steel Construction, Chicago.

CEN (2006). EN 1993-1-5: Eurocode 3 - Design of Steel Structures - Part 1-5: Plated Structural Elements. European Committee for Standardisation, Brussels.

Lagerqvist, O. and Johansson, B. (1996). Resistance of I-girders to concentrated loads. Journal of Constructional Steel Research, 39(2), 87 to 119.

Narayanan, R. (ed.) (1983). Plated Structures: Stability and Strength. Applied Science Publishers, London.

Salmon, C.G., Johnson, J.E. and Malhas, F.A. (2008). Steel Structures: Design and Behavior, 5th edition. Prentice Hall, Upper Saddle River.

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