Simply Supported Beam — Multiple Distributed Loads

Add any number of trapezoidal line loads. Each load begins at a and extends a length b, varying linearly from wa at x=a to wb at x=a+b.

Simply supported beam with multiple distributed loads over [a, a+b], varying linearly from wₐ to w_b; reactions and diagrams indicated

Global units

These selections apply to all inputs and results on this page.

Input parameters

Unit: ft
Unit: ft
Unit: ksi
Unit: inch
Unit: in⁴

Distributed loads

Enter one row per load segment. Positive w acts downward.

wₐ (lbf/ft) w_b (same) a (ft) b (ft) Actions
  • Load varies linearly from wa at x=a to wb at x=a+b.
  • All rows must satisfy 0 ≤ a, 0 ≤ b, and a + b ≤ L.
Numbers and units update together.

Results

ParameterValue
Reaction Force R₁ --- lbf
Reaction Force R₂ --- lbf
Shear @ x (Vₓ) --- lbf
Max Shear (Vmax) --- lbf
Moment @ x (Mₓ) --- lbf·in
Max Moment (Mmax) --- lbf·in
Slope @ x (θₓ) --- radian
Max Slope (θmax) --- radian
End Slope Left (θ₁) --- radian
End Slope Right (θ₂) --- radian
Deflection @ x (yₓ) --- inch
Max Deflection (ymax) --- inch
Bending Stress @ x (σₓ) --- psi
Max Bending Stress (σmax) --- psi

How the multiple distributed-load solver works

This calculator handles any number of trapezoidal (linear) distributed loads on a simply supported beam by superposition. Every row you enter defines a load that starts at position a, spans a length b, and varies from wa at x=a to wb at x=a+b. Internally, each trapezoid is decomposed into two patches so closed-form expressions for reactions, shear, moment, slope, and deflection can be summed along the span.

Resultant of a trapezoidal line load

For one segment (length b, intensities wawb):

  • Equivalent resultant: W = ((w_a + w_b)/2) · b
  • Line of action (from left support): x_c = a + b · (w_a + 2 w_b) / (3 (w_a + w_b))

With several segments, total vertical reaction at the right support follows global equilibrium, R₂ = (Σ W_i · x_{c,i}) / L, and R₁ = Σ W_i − R₂, where L is the beam length. Shear/moment diagrams are obtained by integrating the piecewise line-load functions; slopes and deflections follow the Euler–Bernoulli relation EI·y''(x) = M(x).

Assumptions & sign convention

  • Small-deflection Euler–Bernoulli theory; constant E and I.
  • Positive w acts downward; reactions are positive upward.
  • Bending moment is positive when it compresses top fibers. Shear/deflection positive upward.
  • Supports are ideal simple supports; self-weight can be modeled as an additional distributed load.

Related calculators & references

Charts

Moment, shear, slope, and deflection plots update after calculation.