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.
Last updated: August 2026

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

QuantityPositive 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:

dVdx=w(x)dMdx=V(x)\frac{dV}{dx} = -w(x) \qquad\qquad \frac{dM}{dx} = V(x)

ΔV=wdx=(area under the load diagram)\Delta V = -\int w\,dx = -(\text{area under the load diagram})

ΔM=Vdx=(area under the shear diagram)\Delta M = \int V\,dx = (\text{area under the shear diagram})

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)ConstantLinear
Constant (uniform load)LinearParabolic (2nd degree)
Linear (triangular load)ParabolicCubic (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 pointEffect on $V$Effect on $M$
Concentrated force $P$Jump of magnitude $P$Kink (slope change), no jump
Applied couple $M_0$No changeJump of magnitude $M_0$
Start/end of distributed loadSlope changeCurvature 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).

MA=0:RB(8.0)=96(4.0)+40(3.0)=384+120=504\sum M_A = 0: \quad R_B(8.0) = 96(4.0) + 40(3.0) = 384 + 120 = 504 RB=63.0 kN,RA=96+4063.0=73.0 kNR_B = 63.0\ \text{kN}, \qquad R_A = 96 + 40 - 63.0 = 73.0\ \text{kN}

Shear at key points (from the left):

V(0+)=+73.0 kNV(0^+) = +73.0\ \text{kN} V(3.0)=73.012(3.0)=73.036.0=+37.0 kNV(3.0^-) = 73.0 - 12(3.0) = 73.0 - 36.0 = +37.0\ \text{kN} V(3.0+)=37.040=3.0 kN(jump of 40 kN at the point load)V(3.0^+) = 37.0 - 40 = -3.0\ \text{kN} \quad\text{(jump of 40 kN at the point load)}

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.

Mmax=M(3.0)=73.0(3.0)12(3.0)(3.02)=219.054.0=165.0 kNmM_{\max} = M(3.0) = 73.0(3.0) - 12(3.0)\left(\frac{3.0}{2}\right) = 219.0 - 54.0 = \boxed{165.0\ \text{kN}\cdot\text{m}}

Verification from the right end, which must give the same value:

M(3.0)=63.0(5.0)12(5.0)(2.5)=315.0150.0=165.0 kNM(3.0) = 63.0(5.0) - 12(5.0)(2.5) = 315.0 - 150.0 = 165.0\ \text{kN}\cdot\text{m}\ ✓

$V_{\max} = 73.0$ 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 $A$.

MA=0:RB(6.0)=54(4.0)=216    RB=36.0 kN,RA=18.0 kN\sum M_A = 0: \quad R_B(6.0) = 54(4.0) = 216 \;\Rightarrow\; R_B = 36.0\ \text{kN}, \quad R_A = 18.0\ \text{kN}

The load intensity at distance $x$ is $w(x) = 3x$ kN/m, so the load carried up to $x$ is $\tfrac{1}{2}(3x)(x) = 1.5x^2$:

V(x)=18.01.5x2V(x) = 18.0 - 1.5x^2

Set $V = 0$:

x=18.01.5=12=3.464 mx = \sqrt{\frac{18.0}{1.5}} = \sqrt{12} = 3.464\ \text{m}

Mmax=18.0(3.464)1.5(3.464)2(3.4643)=62.351.5(12.0)(1.1547)=62.3520.78=41.6 kNmM_{\max} = 18.0(3.464) - 1.5(3.464)^2\left(\frac{3.464}{3}\right) = 62.35 - 1.5(12.0)(1.1547) = 62.35 - 20.78 = \boxed{41.6\ \text{kN}\cdot\text{m}}

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.

Test Your Knowledge

For a simply supported beam carrying a uniformly distributed load, what shapes do the shear and moment diagrams take?

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Test Your Knowledge

On a beam, where does the maximum bending moment occur?

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Test Your Knowledge

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?

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Test Your Knowledge

A cantilever beam of length 4.0 m carries a uniformly distributed load of 9.0 kN/m. What is the maximum bending moment?

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