ENGR 201 — UNIT 5
Unit 5 — Internal Resultants

Shear & Moment Equations
and Diagrams

Visualize how internal shear forces and bending moments vary along a beam under any combination of loads.

📌 Most Important Note

Answering Shear & Moment equations and diagrams questions accurately is mostly dependent on drawing the FBD correctly (and obtaining support reactions accurately) and being able to transform w(x) → V(x) → M(x) correctly using the differential and integral relations. Master these two skills and the rest follows.

⚡ Interactive Diagram — choose load type and adjust parameters
The FBD → w(x) → V(x) → M(x) Chain Master This
Every shear and moment problem follows the same transformation pipeline. Understanding each step makes the whole problem routine.

The Transformation Pipeline

The workflow for any beam problem is a strict sequence:

  1. FBD of entire beam → find support reactions (Ay, By, MA…)
  2. From reactions + loading → w(x) — identify the distributed load function on each segment
  3. w(x) → V(x) via dV/dx = −w(x), or equivalently ΔV = −∫w dx
  4. V(x) → M(x) via dM/dx = V(x), or equivalently ΔM = ∫V dx
  5. Verify boundary conditions at supports and free ends
dV/dx = −w(x)   // slope of SFD = −(distributed load intensity)
dM/dx = V(x)    // slope of BMD = shear force at that point
ΔV = −∫w(x) dx  // change in V = −area under load diagram
ΔM = ∫V(x) dx   // change in M = area under shear diagram
Sign Convention Critical — Never Skip
All results are meaningless without a consistent, stated sign convention.

✅ Positive Shear V

Upward force on the left face of the cut; downward on the right face. Tends to cause clockwise rotation of the free body element.

✅ Positive Moment M (Sagging)

Concave upward bending — the beam "smiles." Compresses top fibers. This is positive in the standard beam convention.

Load Type → Diagram Shape Reference
w(x) LoadingV(x) Shape (SFD)M(x) Shape (BMD)
None (w=0)Constant (flat)Linear (sloped line)
Uniform (UDL, w=const)Linear (1st degree)Parabolic (2nd degree)
Triangular (w∝x)Parabolic (2nd degree)Cubic (3rd degree)
Concentrated force PJump of magnitude PKink (slope change)
Concentrated moment M₀No changeJump of magnitude M₀
Worked Example 1 Simply Supported + Point Load
Full FBD → w(x) → V(x) → M(x) pipeline for a simply supported beam with a single concentrated force.
Worked Example 1Simply Supported Beam — Concentrated Load P = 60 kN at x = 4 m
GIVEN: L = 10 m  |  P = 60 kN downward  |  a = 4 m from A
1

FBD of entire beam — find reactions

Apply ΣM_B = 0 (moments about B to eliminate By):

Ay × 10 = 60 × (10−4) = 360 → Ay = 36 kN ↑
ΣFy = 0: By = 60 − 36 = 24 kN ↑
A B P = 60 kN Ay=36kN By=24kN a = 4 m b = 6 m
2

Identify w(x) — no distributed load on either segment

Segment 0 < x < 4:  w(x) = 0   // no distributed load
Segment 4 < x < 10: w(x) = 0  // no distributed load
w(x) diagram A(0) x=4m B(10) w(x) = 0 everywhere P here
3

w(x) → V(x): constant in each segment, jump at point load

V(0⁺) = +Ay = +36 kN            // starts at reaction
V(4⁻) = +36 kN                   // no change (w=0)
V(4⁺) = 36 − 60 = −24 kN     // jump down by P
V(10) = −24 + 24 = 0 ✓
SFD — V(x) +36 kN −24 kN jump=60kN A(0) x=4m B(10)
4

V(x) → M(x): area under SFD accumulates moment

M(0) = 0                  // BC: pin end
M(4) = 0 + 36×4 = +144 kN·m  // area of +36 rectangle
M(10) = 144 + (−24)×6 = 0 ✓ // BC: roller end
BMD — M(x) M_max = 144 kN·m Area=36×4=144 Area=24×6=144 A(0) x=4m B(10) 0 0
5

Complete beam + SFD + BMD stacked summary

Beam P=60kN 36kN 24kN SFD +36 −24 0 4m 10m BMD 144 kN·m 0 4m 10m
Worked Example 2 Cantilever + UDL
Full pipeline for a cantilever beam with a uniform distributed load — w(x)→V(x)→M(x) with integration.
Worked Example 2Cantilever Beam — UDL w₀ = 8 kN/m over full span
GIVEN: Fixed at A (left), free at B (right)  |  L = 6 m  |  w₀ = 8 kN/m downward
1

FBD — fixed wall provides vertical force Ay and moment MA

W = w₀ × L = 8 × 6 = 48 kN (resultant at midspan x=3m)
ΣFy=0: Ay = 48 kN ↑
ΣM_A=0: MA = w₀L²/2 = 8×36/2 = 144 kN·m ↺
w₀ = 8 kN/m Ay=48kN MA 144 A B (free)
2

w(x) = 8 kN/m constant — uniform load over full span

w(x) = 8 kN/m   // constant, downward, 0 ≤ x ≤ 6 m
dV/dx = −w(x) = −8  // slope of SFD is −8 everywhere
w(x) diagram w(x) = 8 kN/m (constant) A(0) 3m B(6)
3

w(x) → V(x): V(x) = 48 − 8x (linear, slope = −8)

V(x) = Ay − w·x = 48 − 8x
V(0) = +48 kN, V(3) = +24 kN, V(6) = 0 ✓
SFD — V(x) +48 kN V = 48 − 8x (linear) 0 ✓ V(3)=+24 A(0) 3m B(6)
4

V(x) → M(x): integrate linear V → parabolic M

M(x) = MA + ∫₀ˣ V dx = 144 + 48x − 4x²
M(0) = 144 kN·m (fixed-end), M(6) = 144+288−144 = 0 ✓ (free end)
BMD — M(x) 144 kN·m (max) 0 ✓ M = 144 + 48x − 4x² (parabola) A(0) 3m B(6) free

⚠ Note: M is maximum at the fixed end A, not mid-span. For a cantilever, the wall must resist the full accumulated moment from all the distributed load.

Worked Example 3 Triangular Load → V(x) → M(x)
Non-uniform w(x) produces increasingly complex V and M — showing the full chain with integration.
Worked Example 3Simply Supported — Triangular Load (0 at A, w₀ = 12 kN/m at B)
GIVEN: L = 9 m  |  w(x) = (4/3)x kN/m  |  zero at A, 12 kN/m at B
1

FBD — resultant of triangular load acts at 2L/3 from A

w(x) = (w₀/L)·x = (12/9)x = (4/3)x kN/m
Resultant W = ½·w₀·L = ½×12×9 = 54 kN at x = 2L/3 = 6 m from A
ΣM_A=0: By×9 = 54×6 = 324 → By = 36 kN
ΣFy=0: Ay = 54−36 = 18 kN
w₀=12 kN/m 0 W=54kN at 2L/3=6m Ay=18kN By=36kN A B
2

w(x) = (4/3)x — linearly increasing load

w(x) = (4/3)x kN/m  // linear, 0 at x=0, 12 at x=9
dV/dx = −w(x) = −(4/3)x  // slope of V is also linear → V is parabolic
w(x) diagram 0 12 kN/m w(x) = (4/3)x (linear) A(0) 4.5m B(9)
3

w(x) → V(x) = 18 − (2/3)x² — parabolic SFD

V(x) = Ay − ∫₀ˣ w dx = 18 − (2/3)x²
V(0)=+18 kN, V(9)=18−54=−36+36=0 ✓
V=0 at x=√27 = 3√3 ≈ 5.20 m ← location of M_max
SFD — V(x) parabolic +By=36 +18 kN −36 kN V=0 at x=5.20m ← M_max here A(0) 5.20m B(9)
4

V(x) → M(x) = 18x − (2/9)x³ — cubic BMD

M(x) = ∫₀ˣ V dx = 18x − (2/9)x³
M(0)=0, M(9)=162−162=0 ✓
M_max at x=5.20m: M=18(5.20)−(2/9)(5.20)³ = 93.6−32.2 = ≈ 62.4 kN·m
BMD — M(x) cubic 62.4 kN·m (at x = 5.20 m) M = 18x − (2/9)x³ (cubic) A(0) 5.20m B(9) 0 0

Key insight: triangular load (linear w) → parabolic V → cubic M. Each integration raises the polynomial degree by 1.

Boundary Conditions Summary

Pin / Roller End

V = reaction
M = 0

Free End

V = 0
M = 0

Fixed End

V = reaction shear
M = reaction moment

Practice Problems
Seven problems covering FBD, w(x)→V(x)→M(x) transformations, and visual diagram identification.
Score
0 / 7
Problem 01 — FBD & Reactions

Simply Supported Beam — Find Reactions

A simply supported beam of length L = 12 m carries a concentrated load P = 72 kN at x = 3 m from the left support A. Draw the FBD and find Ay.

P=72kN A B 3m L = 12 m
kN
ΣM_B=0: Ay×12 = 72×(12−3) = 648 → Ay = 54 kN. Then By = 72−54 = 18 kN.
Problem 02 — w(x) → V(x)

Shear Force from UDL Using the Differential Relation

A simply supported beam (L=10 m) carries a uniform load w = 5 kN/m over its full length. Reactions: Ay = By = 25 kN. Using V(x) = Ay − w·x, find V at x = 3 m.

V(x) = Ay − w·x  // from integrating dV/dx = −w with V(0) = Ay
kN
V(3) = 25 − 5×3 = 25 − 15 = 10 kN.
Problem 03 — V(x) → M(x) Area Method

Bending Moment via Area Under SFD

Continuing from P2 (UDL w=5 kN/m, L=10 m, Ay=25 kN). The shear function is V(x) = 25−5x (linear). Using ΔM = ∫V dx, find M at x = 5 m (mid-span).

M(5) = ∫₀⁵ V dx = ∫₀⁵ (25−5x) dx = [25x − 2.5x²]₀⁵
kN·m
M(5) = 25(5) − 2.5(25) = 125 − 62.5 = 62.5 kN·m. Also = wL²/8 = 5×100/8 = 62.5 ✓
Problem 04 — FBD + Full Pipeline

Cantilever — Fixed-End Moment from w(x)→V(x)→M(x)

A cantilever beam is fixed at A (left), free at B (right). Length L = 5 m, uniform load w = 10 kN/m. Using the pipeline, find the magnitude of M at x = 0 (fixed end).

From free end: V(5)=0, V(0)=w×L=10×5=50kN
M(5)=0, M(0) = M(5)−∫₀⁵V dx
kN·m
Working from free end B: V(x from B) = w·s where s is distance from B. M at fixed end = ½·w·L² = ½×10×25 = 125 kN·m. Or: ∫₀⁵(50−10x)dx = [50x−5x²]₀⁵ = 250−125=125.
Problem 05 — Find Location of Maximum Moment

Position Where V(x) = 0 (Triangular Load)

A simply supported beam (L=9m) has a triangular load: w(x) = (4/3)x kN/m (zero at A, 12 kN/m at B). Reactions: Ay=18 kN, By=36 kN. The shear is V(x) = 18 − (2/3)x². Find the value of x (in m) where V(x) = 0 (maximum moment location). Round to 2 decimal places.

Set V(x) = 0: 18 − (2/3)x² = 0 → x² = 27 → x = ?
m
18 = (2/3)x² → x² = 27 → x = √27 = 3√3 ≈ 5.196 ≈ 5.20 m
Problem 06 — Visual: Identify the Correct SFD

Which SFD matches this beam?

A simply supported beam carries a uniform distributed load w over its full span. The reactions are equal (Ay = By = wL/2). Which of the four SFDs below is correct?

w (uniform)
Diagonal line
Option A
Rectangular
Option B
Trapezoid-linear
Option C
Parabola
Option D
Problem 07 — Visual: Identify the Correct BMD

Which BMD matches a simply supported beam with a single point load at mid-span?

The beam has a concentrated load P at the center (x = L/2). SFD has a jump at center. Which BMD is correct?

Parabola
Option A
Triangle peak
Option B
Constant
Option C
Step shape
Option D
Assessment — Unit 5

Shear & Moment Diagrams

12 questions · Mixed types including visual · 20 minute limit · 70% to pass

12
Questions
20:00
Time Limit
70%
To Pass
5× Multiple Choice 4× Numeric 1× True/False 2× Visual
Exam Complete