11 Beam Deflection Formula Tables

Civil Guide

Beam Deflection Formulas

Bending and Deflection Equations

When designing beams (concrete, steel or timber), the bending and shear capacity is checked against applied bending theory.

An applied force causes the element to bend and it is subjected to bending moments and ends react to shear loads.

The bending and shear profile of a beam/element depends on the type of beam support (i.e, pinned, fixed and free ends).

Elastic Beam deflection formula

\(\frac{M}{I}=\frac{\sigma}{y}=\frac{E}{R}\)

  • M is the applied moment
  • I is the section moment of inertia
  • \(\sigma\) is the fibre bending stress
  • y is the distance from the neutral axis to the fibre and R is the radius of curvature
  • Section modulus is Z=I/y
  • Applied bending stress can be simplified to \(\sigma\) = M/Z

KEY Terms in Beam deflection formulas

  • P is Force in kN
  • L is total length in mm
  • E is young’s modulus 
  • I is the second moment of area (\(mm^2\))
  • W is total load (UDL x length)
  • w is UDL (force per unit length, kN/m)

The tables below show beam deflection formulas for simply supported, fixed beam and cantilevers for different end conditions and loadings.

Beam Deflection Formula Tables

Simple Supported Beam Deflection and Formula

Simple Supported Beams under a single Point Load – (2 pin connections at each end)

Note – pin supports cannot take moments, which is why bending at the support is zero.

Simply Supported Beam
Simply Supported Beam

Moment:

\(M_{midspan} = \frac{PL}{4}\)

Beam Deflection Equation:

\(\delta = \frac{PL^3}{48EI}\)

Shear Force and Reaction:

\(R_A=R_B=\frac{P}{2}\)

Simple Supported Beams under a single Point Load located anywhere on the beam – (2 pin connections at each end)

 

Simply Supported Beam - Point Load
Simply Supported Beam - Point Load

Moment:

\(M_{C} = \frac{Pab}{L}\)

Beam Deflection Equation:

when a>b,

\(\delta_x = \frac{Pab(L+b)}{27EIL} \sqrt{3a(L+b)}\)

at \(x=\sqrt{\frac{a(L+b)}{3}}\) from A

Shear Force and Reaction:

\(R_A= \frac{Pb}{L}\)

\(R_B= \frac{Pa}{L}\)

Simple Supported Beams under a 2 Point Load – (2 pin connections at each end)

 

Simply Supported Beam - 2 Point Loads
Simply Supported Beam - 2 Point Loads

Moment:

\(M_{C} = Pa\)

\(M = \frac{PL}{3}\)

Beam Deflection Equation:

when a>b,

\(\delta_{midspan} = \frac{PL^3}{6EI} (\frac{3a}{4L}-(\frac{a}{L})^3)\)

\(\delta = \frac{23PL^3}{648EI}\)

Shear Force and Reaction:

\(R_A = R_B = P\)

Thirdpoins: \(a=\frac{L}{3}\)

Simple Supported Beams under Uniformly distributed loads (UDL) – (2 pin connections at each end)

 

Simply Supported Beam - UDL
Simply Supported Beam - UDL

Moment:

\(M_{midpan} = \frac{wl^2}{8}\)

Beam Deflection Equation:

\(\delta_{midspan} = \frac{5wl^4}{384EI} \)

Shear Force and Reaction:

\(R_A = R_B = \frac{wL}{2}\)

Simple Supported Beams under a UDL with cantilever – (2 pin connections with a central pin)

 

Simply Supported Beam - Cantilever UDL
Simply Supported Beam - Cantilever UDL

Moment:

\(M_{B} = \frac{wb^2}{2}\)

\(M_{C} = \frac{w(a+b)^2(a+b)^2}{8a^2}\)

maximum x = \(\frac{a}{b}(1-\frac{b^2}{a^2}\)

Beam Deflection Equation:

\(\delta_{c} = \frac{wL}{24EI}(x^4-2ax^3+\frac{2b^2}{a}x^3+a^3x-2ab^2x) \)

\(\delta_{freetip} = \frac{wb}{24EI}(3b^3 + 4ab^2-a^3) \)

Shear Force and Reaction:

\(R_A  = \frac{wL}{2a}(a^2-b^2)\)

\(R_B  = \frac{wL}{2a}(a^2+b^2)\)

Simple Supported Beams under a VDL load – (2 pin connections at each end)

Simply Supported Beam - VDL
Simply Supported Beam - VDL

Moment:

\(M_{Midspan} = \frac{WL}{6}\)

Beam Deflection Equation:

\(\delta_{midspan} = \frac{WL^3}{60EI}\)

Shear Force and Reaction:

\(R_A  = R_B = \frac{W}{2}\)

Simple Supported Beams under a partial UDL – (2 pin connections at each end)

 

Simply Supported Beam - Centre UDL
Simply Supported Beam - Centre UDL

Moment:

\(M_{Max} = \frac{W}{b}(\frac{x_1^2-a^2}{2})\)

When \(x_1=a+\frac{R_Ab}{W}\)

Beam Deflection Equation:

\(\delta_{max} = \frac{W}{384EI}(8L^3-4Lb^2+b^3)\)

Shear Force and Reaction:

\(R_A  = \frac{W}{L} (\frac{b}{2}+c)\)

\(R_B  = \frac{W}{L} (\frac{b}{2}+a)\)

Fixed Beam Deflection and Formula

Fixed Beams under a single Point Load – (2 fixed connections at each end)

 

Fixed Beam - Point Load
Fixed Beam - Point Load

Moment:

\(M_{A} = \frac{-Pab^2}{L^2}\)

\(M_{B} = \frac{-Pba^2}{L^2}\)

\(M_{C} = \frac{2Pa^2b^2}{L^3}\)

Beam Deflection Equation:

\(\delta_{max} = \frac{2Pa^3b^2}{3EI(L+2a)^2}\)

when \(x=\frac{L^2}{(3L-2a)}\)

\(\delta_{c} = \frac{Pa^3b^2}{3EIL}\)

Shear Force and Reaction:

\(R_A  = \frac{Pb^2(L+2a)}{L^3}\)

\(R_B  = \frac{Pb^2(L+2b)}{L^3}\)

Fixed Beam under UDL – (2 fixed connections at each end)

Fixed Beam - UDL Load
Fixed Beam - UDL Load

Moment:

\(M_{A} = M_{B} = \frac{-wL^2}{12}\)

\(M_{C} = \frac{wL^2}{24}\)

Beam Deflection Equation:

\(\delta_{midspan} = \frac{wL^4}{384EI}\)

Shear Force and Reaction:

\(R_A  = R_B \frac{wL}{2}\)

\(R_A  = R_B \frac{wL}{2}\)

Fixed end and pinned with UDL – (1 fixed end and pinned connection at each end).

Note – pin supports cannot take moments, which is why bending at the support is zero.

Note – Fixed supports resists moment, which is why it produces a moment 

Fixed Beam and Simple Support - UDL
Fixed Beam and Simple Support - UDL

Moment:

\(M_{A} = \frac{-Pb(L^2-b^2)}{2L^2}\)

\(M_{C} = \frac{Pb}{2}(2-\frac{3b}{L}+\frac{b^3}{L^3}\)

Beam Deflection Equation:

\(\delta_{c} = \frac{Pa^3b^2}{12EIL^3}(4L-a)\)

Shear Force and Reaction:

\(R_A  = P-R_B\)

\(R_B  = \frac{Pa^2(2L+b)}{2L^3}\)

Fixed end cantilever with UDL – (2 pin connections at each end)

 

Fixed Beam - Cantilever Beam and UDL
Fixed Beam - Cantilever Beam and UDL

Moment:

\(M_{A} = \frac{-wl^2}{2}\)

Beam Deflection Equation:

\(\delta_{tip} = \frac{WL^3}{8EI}\)

Shear Force and Reaction:

\(R_A  = W\)

This Post Has One Comment

  1. Lucia Tlhoaele

    Thanks alot …this was very helpful

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