Cantilevers
A cantilever is fixed at one end and free at the other. With a point load at the free end, the tip deflects most:
δmax =P·L³3·E·I
- δ
- deflection
- m
- P
- point load
- N
- L
- length
- m
- E
- Young's modulus
- Pa
- I
- second moment of area
- m⁴
- M
- bending moment
- N·m
- b
- section width
- m
- h
- section depth
- m
- θ
- slope
- rad
- w
- load per length
- N/m
| I = bh³/12 | 1.71 × 10⁶ mm⁴ |
| Mwall = PL | 1 kN·m |
| θtip = PL²/2EI | 1.46 mrad |
| δmax = PL³/3EI | 0.977 mm |
Worked example
Uses the values in Fig. 2.4-1. Change them and the working updates.
Given
- Ppoint load at the free end1 kN
- Llength from the wall1 m
- Esteel200 GPa
- b×hrectangular section40 × 80 mm
Find
The deflection δ at the free end.
Solution
I = bh³/12 = 1.707 × 10⁻⁶ m⁴
δ = PL³/3EI
= 1,000 N × (1 m)³ / (3 × 2 × 10¹¹ Pa × 1.707 × 10⁻⁶ m⁴)
= 9.77 × 10⁻⁴ m
Answer
δ = 0.977 mm
Length over tip deflection: L/1,024.
Other load cases
Same symbols. δ and θ are at the free end; M is at the wall.
-
Uniform load
δ = wL⁴8EIM = wL²2θ = wL³6EI
-
Point load at a from the wall
δtip = Pa²(3L − a)6EIM = Pa
-
End moment M0
δ = M0L²2EIθ = M0LEI
Assumptions
- The root is fully fixed: no movement or rotation at the wall. Real fixings rotate a little, which adds deflection.
- The beam is straight, prismatic and made of one linear-elastic material.
- Deflections are small compared with the length, so the slope squared is negligible.
- Shear deformation and the beam's own weight are ignored.
Derivation
Measure x from the wall, with y positive upwards. An end load gives a hogging moment M = −P(L − x) at x.
- Start from the bending equation:
EI·y″ = −P(L − x). - Integrate once:
EI·y′ = −P(Lx − x²/2) + C₁. The slope is zero at the wall, soC₁ = 0. - Integrate again:
EI·y = −P(Lx²/2 − x³/6) + C₂. The deflection is zero at the wall, soC₂ = 0. - At the tip,
x = L:EI·y = −PL³/3.
So δ = PL³/3EI, sixteen times the mid-span deflection of the same beam simply supported over the same length with a central load. The tip slope is θ = PL²/2EI.