10.3 Shear and Moment Diagrams
Key Takeaways
- NCEES lists shear and moment diagrams as its own Strength of Materials sub-topic, separate from the stress formulas that consume their results.
- The slope of the shear diagram equals the negative of the distributed load, and the slope of the moment diagram equals the shear.
- The change in shear between two points equals the area under the load diagram, and the change in moment equals the area under the shear diagram.
- Maximum bending moment occurs where the shear diagram crosses zero, which is the fastest way to locate the critical section.
- A concentrated load causes a jump in the shear diagram and a kink in the moment diagram, while an applied couple causes a jump in the moment diagram only.
10.3 Shear and Moment Diagrams
The NCEES Strength of Materials specification lists "Shear and moment diagrams" as a distinct sub-topic, and for good reason: the bending stress formula $\sigma = Mc/I$ and the transverse shear formula $\tau = VQ/(It)$ both require $M$ and $V$ at the critical section, and finding that section is what the diagrams are for. On a CBT exam you rarely draw the full diagram — you extract one value — so learning the shortcuts matters more than learning to sketch.
Sign Conventions
| Quantity | Positive when… |
|---|---|
| Shear $V$ | The internal shear rotates the segment clockwise; equivalently, the resultant of forces to the left acts upward |
| Bending moment $M$ | The beam bends concave up (a "smile"), compressing the top fibers and stretching the bottom |
Positive moment producing tension on the bottom is why reinforcing steel goes in the bottom of a simply supported concrete beam and in the top over a continuous support.
The Differential and Integral Relationships
These four relationships are the entire toolkit:
Read them as a degree ladder. Each integration raises the polynomial degree by one:
| Load $w(x)$ | Shear $V(x)$ | Moment $M(x)$ |
|---|---|---|
| Zero (unloaded span) | Constant | Linear |
| Constant (uniform load) | Linear | Parabolic (2nd degree) |
| Linear (triangular load) | Parabolic | Cubic (3rd degree) |
This table alone answers many exam items. "What is the shape of the moment diagram for a uniformly loaded simple beam?" — parabolic, without any calculation.
The Zero-Shear Rule
Since $dM/dx = V$, the moment is stationary where $V = 0$:
The maximum bending moment occurs where the shear diagram crosses zero (or at a support, or at a point of applied couple).
This is the single most useful fact in the topic. Rather than writing $M(x)$ and differentiating, you find where $V = 0$ and take moments there.
Discontinuities
| Feature at a point | Effect on $V$ | Effect on $M$ |
|---|---|---|
| Concentrated force $P$ | Jump of magnitude $P$ | Kink (slope change), no jump |
| Applied couple $M_0$ | No change | Jump of magnitude $M_0$ |
| Start/end of distributed load | Slope change | Curvature change |
Trap: an applied couple leaves the shear diagram completely unaffected while stepping the moment diagram vertically. Candidates who put a jump in the shear diagram at an applied moment corrupt everything downstream.
Standard Results Worth Memorizing
| Beam and loading | $V_{\max}$ | $M_{\max}$ | Location |
|---|---|---|---|
| Simple span, uniform $w$ | $wL/2$ | $\dfrac{wL^2}{8}$ | Midspan |
| Simple span, central point load $P$ | $P/2$ | $\dfrac{PL}{4}$ | Midspan |
| Cantilever, uniform $w$ | $wL$ | $\dfrac{wL^2}{2}$ | At the fixed end |
| Cantilever, end point load $P$ | $P$ | $PL$ | At the fixed end |
| Simple span, point load $P$ at distance $a$ from left, $b$ from right | $\max(Pb/L,\ Pa/L)$ | $\dfrac{Pab}{L}$ | Under the load |
Note the factor-of-four difference between a simply supported beam under a central point load ($PL/4$) and a cantilever with the same load at its tip ($PL$). Support conditions matter more than load magnitude.
Worked Example 1: Simple Span with Uniform and Point Loads
A simply supported beam spans $L = 8.0$ m with a uniform load $w = 12$ kN/m over the full span plus a 40 kN point load at 3.0 m from the left support $A$. Find $V_{\max}$, the location of zero shear, and $M_{\max}$.
Reactions. Total uniform load $= 12(8.0) = 96$ kN at midspan (4.0 m).
Shear at key points (from the left):
Shear crosses zero within $0 < x < 3.0$ m, since $V$ goes from $+73.0$ to $+37.0$ and only then jumps negative. It does not cross zero before 3.0 m — it jumps through zero at the point load. So the zero crossing is at $x = 3.0$ m, at the point load itself.
Verification from the right end, which must give the same value:
$V_{\max} = 73.0$ kN at support $A$.
Worked Example 2: Locating Zero Shear Inside a Span
A simply supported beam spans 6.0 m with a load increasing linearly from zero at $A$ to 18 kN/m at $B$. Find $M_{\max}$ and its location.
Total load $= \tfrac{1}{2}(18)(6.0) = 54$ kN, acting at $\tfrac{2}{3}(6.0) = 4.0$ m from $A$.
The load intensity at distance $x$ is $w(x) = 3x$ kN/m, so the load carried up to $x$ is $\tfrac{1}{2}(3x)(x) = 1.5x^2$:
Set $V = 0$:
Note where the maximum sits: at 3.46 m, past midspan and toward the heavier end — exactly where the shear diagram's parabola crosses zero. Assuming the maximum moment is always at midspan gives $M(3.0) = 54.0 - 13.5 = 40.5$ kN·m, which is 2.6% low and offered as a distractor. For non-symmetric loading, always locate zero shear rather than assuming midspan.
For a simply supported beam carrying a uniformly distributed load, what shapes do the shear and moment diagrams take?
On a beam, where does the maximum bending moment occur?
A concentrated couple of 25 kN-m is applied at a point along a beam's span. What is its effect on the shear and moment diagrams?
A cantilever beam of length 4.0 m carries a uniformly distributed load of 9.0 kN/m. What is the maximum bending moment?