Module 8 · Lesson 8.2
Restraint, moment shape, and where the load sits
Three things change the answer. One is free, one is decided by the structure, and one is a detailing choice most people never think about.
Why this matters
The 8 m beam of the last lesson lost two thirds of its capacity. All three of the things that would recover it are available to a designer, and one of them — where the load is applied relative to the shear centre — is a decision usually made without any thought at all. It is worth 26% on this beam.
By the end of this lesson you should be able to
- Calculate what a lateral restraint buys, and when it stops buying
- Explain why uniform moment is the worst case
- Quantify the load-height effect and say which way it goes
- State what a restraint must physically do to count
Restraint: the largest lever, and it saturates
Mcr depends on the length between points of lateral restraint, not on the span. So a restraint at midspan halves the length that matters.
For the 8 m beam of the last lesson, restraining the compression flange gives:
| Restraints | Segment | λ̄LT | χLT | Mb,Rd | Gain |
|---|---|---|---|---|---|
| 0 | 8.00 m | 1.69 | 0.351 | 290 kNm | — |
| 1 | 4.00 m | 0.96 | 0.727 | 600 kNm | 2.07× |
| 2 | 2.67 m | 0.66 | 0.890 | 735 kNm | 2.54× |
| 3 | 2.00 m | 0.50 | 0.960 | 793 kNm | 2.74× |
| 5 | 1.33 m | 0.34 | 1.000 | 826 kNm | 2.85× |
| 7 | 1.00 m | 0.25 | 1.000 | 826 kNm | 2.85× |
One restraint at midspan more than doubles the resistance. That is a larger gain than any change of section or grade would give, and it costs a tie and two cleats.
And then it saturates. Once χLT reaches 1 the beam has its full cross-section resistance and there is nothing left to recover — the fifth restraint achieves the last 4%, and the seventh achieves nothing at all. Restraint is worth adding until χLT approaches 1, and pointless afterwards.
Worked example
Three ways to recover the same beam
Given
- The 8 m beam from the previous lesson: Mc,Rd = 826 kNm, unrestrained Mb,Rd = 290 kNm
- The load is a UDL, so the moment is not uniform
- It is a floor beam, so the load arrives on the top flange
Find
The effect of each of the three levers, separately.
Assumptions
- C₁ = 1.13 for a UDL and C₂ = 0.45 — both calibrated and unverified here
- The restrained case assumes the restraint is effective, per the callout above
Try it
Three levers on the same beam
The 8 m beam from the worked example, at 290 kNm against a cross-section resistance of 826. Restraint, moment shape and load height all move it — and only one of them is under full control.
Moment shape
Load applied at
- Segment length
- 8.00 m
- Moment factor C₁
- 1.00
- Load height zg
- 0 mm
- Critical moment Mcr
- 290 kNm
- LTB slenderness λ̄LT
- 1.688
- Reduction χLT
- 0.351
- Design resistance Mb,Rd
- 290 kNm
- Cross-section resistance
- 826 kNm
- Gain over the reference
- 1.00 ×
- Still lost to LTB
- 65 %
Mb,Rd = 290 kNm, which is 1.00 times the unrestrained reference case and 65% short of the cross-section resistance. There is still 536 kNm to recover.
Things worth trying
- Start from the reference case — no restraints, uniform moment, load at the shear centre. 290 kNm against a cross-section resistance of 826: two thirds gone.
- Add ONE restraint. The resistance more than doubles, to about 600 kNm. That is a bigger gain than any change of section or grade, for a tie and two cleats.
- Keep adding restraints. The gains shrink fast, and by five χLT reaches 1 and they stop entirely. Restraint is worth adding until χLT approaches 1 and is wasted afterwards.
- Go back to zero restraints and switch the moment shape to double curvature. C₁ = 2.6 and the resistance nearly doubles — because with equal and opposite end moments only a short length near each end is heavily compressed on the same flange.
- Now set the moment shape to UDL and move the load between the three positions. Top flange to bottom flange is a factor of about 1.7 — from a detailing arrangement that most people never calculate.
- Try all three levers together: one restraint, UDL, load at the bottom flange. The three multiply, and the beam becomes a completely different member from the reference case despite identical section, span and total load.
Practice
An 8 m unrestrained beam has Mb,Rd = 290 kNm. One restraint is added at midspan, taking χLT from 0.351 to 0.727. What is the new Mb,Rd, in kNm? Take Mc,Rd = 826 kNm.
Practice
For a UDL, C₁ = 1.13. If Mcr under uniform moment is 290 kNm, what is it under the UDL?
Practice
Top-flange loading gives Mb,Rd = 239 kNm and bottom-flange loading 408 kNm on the same beam. By what factor do they differ?
Check yourself
A beam has χLT = 0.96 with three restraints. What does adding a fourth achieve?
Summary
- Mcr depends on the length between RESTRAINTS, not the span
- One restraint at midspan more than doubled the resistance of the 8 m beam
- Gains saturate once χLT reaches 1 — beyond that, nothing is available
- Uniform moment is the worst case; C₁ = 1 is the reference and everything else is better
- Top-flange loading is destabilising and cost 26%; bottom-flange loading gains 37%
- Top versus bottom is a factor of 1.71 on this beam, from a detailing arrangement
- The three levers multiply — a restrained UDL beam is a different member entirely
- A restraint must reach the COMPRESSION flange, which changes side over a support
This is educational material. It uses simplified examples to teach principles, and must not be relied on for real design or safety-critical decisions. Module overview and checkpoint