---
title: "Critical position of UDL shorter than span"
subject: "Theory of Structures I"
chapter: 5
key: "semester_4/theory_of_structures_i:udl-shorter-than-span-critical-position"
source: https://www.bctengineer.com/q/semester_4/theory_of_structures_i/udl-shorter-than-span-critical-position
site: BCT Engineering
---

# Critical position of UDL shorter than span

Theory of Structures I · Chapter 5: Influence Lines for Simple Structures

- Asked in: 2079 Chaitra, 4 marks; 2077 Chaitra, 6 marks; 2071 Bhadra, 6 marks; 2071 Magh, 5 marks; 2070 Magh, 6 marks; 2066 Kartik, 6 marks (asked 6 times)
- Video: [Influence Line Diagrams for Simply Supported Beams - Problem No 2 (UDL length less than beam span)](https://www.youtube.com/watch?v=vIXTV9x7lsg) — Stan Academy
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_4/theory_of_structures_i/udl-shorter-than-span-critical-position
- Whole chapter: https://www.bctengineer.com/md/semester_4/theory_of_structures_i/chapter-5

## Question

Using influence line diagram, determine the most critical position of a stretch of uniformly distributed load shorter than the span to give maximum bending moment at a given section of a simply supported beam. (Prove that the bending moment is maximum when the section divides the span and the load in the same ratio.)

## Short answer

Place the UDL so that the section divides the load in the same ratio as it divides the span: c/l = a/L, where c is load length left of the section, l is total load length, a is distance from left support. Equating end ordinates of the ILD under the load yields this critical condition.

## Answer

A UDL shorter than the span gives maximum bending moment at a section when the load is placed so that the **section divides the span and the load in the same ratio**.

#### ILD for bending moment at section C
Simply supported beam $AB$, span $L$; section $C$ at $a$ from $A$, $b = L-a$. The ILD for $M_C$ is a triangle with peak $y_C = ab/L$ under $C$.

```text
        A      c    C   (l-c)    B
        o------+----+-------+----o
  ILD:         y1  ab/L     y2
```

Ordinate left of $C$ at distance $x$ from $A$: $y = \dfrac{xb}{L}$. Right of $C$ at distance $x$ from $B$: $y = \dfrac{xa}{L}$.

#### Proof
Let a UDL of intensity $w$ and length $l$ (< $L$) have a length $c$ on the left of $C$ and $(l-c)$ on the right. Ordinates under its ends are

$$
y_1 = \frac{(a-c)\,b}{L}, \qquad y_2 = \frac{\{b-(l-c)\}\,a}{L}
$$

$M_C = w\times(\text{area under ILD below the load})$. Shift the load by a small distance $dx$ to the right. The left end loses a strip of height $y_1$ and the right end gains a strip of height $y_2$, so

$$
\frac{dM_C}{dx} = w\,(y_2 - y_1)
$$

$M_C$ is maximum when $dM_C/dx = 0$, i.e. $y_1 = y_2$:

$$
\begin{aligned} (a-c)\,b &= (b-l+c)\,a \\ ab - cb &= ab - la + ca \\ c(a+b) &= la \Rightarrow \frac{c}{l} = \frac{a}{L} \end{aligned}
$$

Hence the part of the load on the left of $C$ is to the whole load as the left part of the span is to the whole span:

$$
\frac{c}{l} = \frac{a}{L}
$$

#### Maximum moment
With $c = la/L$ the end ordinates are equal: $y_1 = y_2 = \dfrac{ab}{L}\left(1-\dfrac{l}{L}\right)$. The area under the load is two trapezoids:

$$
M_{max} = w\,\frac{l}{2}\left(\frac{ab}{L} + y_1\right) = w\,l\,\frac{ab}{L}\left(1 - \frac{l}{2L}\right)
$$

**Result:** place the UDL so that the section divides the load in the ratio $a : b$, the same as it divides the span.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What is the shape of the ILD for bending moment at section C of a simply supported beam?
   A. A triangle with peak ab/L under C
   B. A rectangle of height ab/L
   C. A straight line from 1 at A to 0 at B
   D. A parabola with peak at mid-span
   Answer: A. M_C ILD is a triangle, zero at both supports and ab/L under the section. (Key point: ILD shape)

2. Shifting the UDL by dx changes M_C by w(y2 - y1). When is M_C maximum?
   A. When the ordinates under the two ends of the load are equal (y1 = y2)
   B. When the load is centred on the span
   C. When the load starts at the section C
   D. When y1 is zero
   Answer: A. dM/dx = 0 requires y2 = y1, the end ordinates being equal. (Key point: Condition for maximum)

3. What does y1 = y2 lead to?
   A. c/l = a/L, the section divides the load and the span in the same ratio
   B. c = l/2, the section is at the load centre
   C. c = a, the load begins at the support
   D. l = L - a
   Answer: A. Algebra of (a-c)b = (b-l+c)a gives c(a+b) = la, so c/l = a/L. (Key point: Result of proof)

4. With the load critically placed, how are the moment and ordinates described?
   A. The area under the load is two trapezoids with equal end ordinates ab/L(1 - l/L)
   B. The load area is one triangle
   C. The end ordinates are 0
   D. The end ordinates are ab/L
   Answer: A. With c = la/L, y1 = y2 = (ab/L)(1 - l/L), and M_max = w l (ab/L)(1 - l/2L). (Key point: Maximum moment)

## Related in Theory of Structures I

- [Moment area: mid-span deflection under UDL](https://www.bctengineer.com/question.md?key=semester_4%2Ftheory_of_structures_i%3Amoment-area-ss-udl-midspan) — Theory of Structures I, chapter 4
- [No bending moment under UDL in parabolic arch](https://www.bctengineer.com/question.md?key=semester_4%2Ftheory_of_structures_i%3Aarch-no-bm-udl) — Theory of Structures I, chapter 6, asked 2×
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