---
title: "Moment-area theorems with proof"
subject: "Strength of Materials"
chapter: 8
key: "semester_4/strength_of_materials_mechanical:moment-area-theorems-statement-proof"
source: https://www.bctengineer.com/q/semester_4/strength_of_materials_mechanical/moment-area-theorems-statement-proof
site: BCT Engineering
---

# Moment-area theorems with proof

Strength of Materials · Chapter 8: Deflection of Beams by Moment- area Method

- Asked in: year not given, 6 marks
- Video: [Introduction to Moment Area Method | Mohr’s Theorem Derivation | Deflection Of Beam](https://www.youtube.com/watch?v=vZUUDFQ6bCM) — Tutor Jerry Academy 
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_4/strength_of_materials_mechanical/moment-area-theorems-statement-proof
- Whole chapter: https://www.bctengineer.com/md/semester_4/strength_of_materials_mechanical/chapter-8

## Question

State and prove the two moment-area theorems. Explain how they are used to find the slope and deflection of a beam.

## Short answer

Theorem I: change in slope between two points equals the area of the M/EI diagram between them. Theorem II: vertical deviation of a point from the tangent at another equals the moment of that area about the point. Used with a tangent of known slope (fixed end or symmetry) to find slopes and deflections.

## Answer

#### Basis
For small deflections $\dfrac{d^2y}{dx^2} = \dfrac{M}{EI}$, so $\dfrac{d\theta}{dx} = \dfrac{M}{EI}$, where $\theta$ is the slope. The quantity $M/EI$ plotted along the beam is the **$M/EI$ diagram**.

```text
        tangent at A
   A ___.----__           
      \        ---.__ B     theta_AB : change in slope
 tangent at B      t_BA : deviation of B from the
                   tangent drawn at A
```

#### Theorem I (change of slope)
*The change in slope between two points A and B on the elastic curve equals the area of the $M/EI$ diagram between them.*

Proof: from $d\theta = \dfrac{M}{EI}dx$, integrate from A to B:

$$
\theta_{B} - \theta_{A} = \int_A^B \frac{M}{EI}\,dx = \text{Area}_{AB}\ \text{of the }M/EI\text{ diagram}
$$

#### Theorem II (tangential deviation)
*The vertical deviation of point B on the elastic curve from the tangent drawn at A equals the moment of the area of the $M/EI$ diagram between A and B, taken about B.*

Proof: consider a small element $dx$ at distance $x$ from B. The change in slope across the element is $d\theta = \dfrac{M}{EI}dx$. The tangents at the ends of the element intercept a vertical distance $dt = x\,d\theta$ on the vertical through B. Integrating,

$$
t_{B/A} = \int_A^B x\,\frac{M}{EI}\,dx = \text{Area}_{AB}\times\bar x_B
$$

where $\bar x_B$ is the distance of the centroid of the $M/EI$ area from B.

#### Use
1. Draw the BM diagram, divide by $EI$.
2. Choose a reference tangent where the slope is known: at the fixed end of a cantilever (zero slope) or at the centre of a symmetrically loaded beam.
3. Slope: use Theorem I from the reference point. Deflection: use Theorem II (deviation from the tangent). For a simply supported beam, find the deviation of the supports from a tangent at one support, get the slope there, then find the deflection at a section from geometry.

Sign: positive area (sagging) gives an anticlockwise rotation from A to B and B lies above the tangent at A.

## Check yourself

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

1. What does the first moment-area theorem state?
   A. The deflection at B equals the area of the M/EI diagram
   B. The change in slope between A and B equals the area of the M/EI diagram between them
   C. The change in slope equals the moment of the M/EI area about B
   D. The slope at B equals M/EI at B
   Answer: B. Integrating dθ = (M/EI)dx gives θB - θA = area of M/EI. (Key point: Theorem I)

2. What does the second theorem give?
   A. The change in slope between A and B
   B. The deviation equals the moment of M/EI area about A
   C. The deviation of B from the tangent at A equals the moment of the M/EI area about B
   D. The deviation equals the M/EI area itself
   Answer: C. t(B/A) = area × distance of its centroid from B. (Key point: Theorem II)

3. In the proof of Theorem II, how is the intercept dt for an element dx found?
   A. dt = dθ/x
   B. dt = dx dθ
   C. dt = x² dθ
   D. dt = x dθ, where x is the distance from B
   Answer: D. Small angle dθ at distance x from B subtends an intercept x dθ. (Key point: Proof of II)

4. Where is the reference tangent best chosen?
   A. Where the slope is known, such as the fixed end or the centre of a symmetric beam
   B. At the point of maximum moment
   C. At any point as the slope there is always zero
   D. At the point of zero deflection
   Answer: A. A known slope lets Theorem I give slopes directly. (Key point: Choosing reference tangent)

## Related in Strength of Materials

- [Beam with two symmetrical loads by moment-area](https://www.bctengineer.com/question.md?key=semester_4%2Fstrength_of_materials_mechanical%3Asymmetrical-beam-two-loads-moment-area) — Strength of Materials, chapter 8
- [Maximum deflection with unsymmetrical loading](https://www.bctengineer.com/question.md?key=semester_4%2Fstrength_of_materials_mechanical%3Aunsymmetrical-load-maximum-deflection-moment-area) — Strength of Materials, chapter 8

## Related in other subjects

- [State and prove moment area theorems](https://www.bctengineer.com/question.md?key=semester_4%2Ftheory_of_structures_i%3Amoment-area-theorems-prove) — Theory of Structures I, chapter 4, asked 4×
- [Moment area: slope and deflection at E and at 4 m](https://www.bctengineer.com/question.md?key=semester_4%2Ftheory_of_structures_i%3Amoment-area-e-4m-a) — Theory of Structures I, chapter 4
- [Moment area: slope and deflection under 50 kN](https://www.bctengineer.com/question.md?key=semester_4%2Ftheory_of_structures_i%3Amoment-area-12-ss-defl-4m-d) — Theory of Structures I, chapter 4
- [Moment area: overhang beam free-end deflection](https://www.bctengineer.com/question.md?key=semester_4%2Ftheory_of_structures_i%3Amoment-area-overhang-10kn-m-2078) — Theory of Structures I, chapter 4
