CELE Strength of Materials — Shear and Moment DiagramsStudy Notes
Thorough study notes for Shear and Moment Diagrams — the fastest path from zero to ready for CELE Strength of Materials. Structured for self-study reviewers who cannot attend a review centre, these notes cover the full concept library plus the CELE-specific twists Professional Regulation Commission (PRC) — Board of Civil Engineering adds to its questions.
Exam context
On the CELE 2026, the Strength of Materials subtest carries a "Core" weight in Professional Regulation Commission (PRC) — Board of Civil Engineering's pattern. Shear and Moment Diagrams lands at position 3rd out of 8 in the standard review order. Target score is 70% weighted average, no sub-test below 50%, and roughly a meaningful share of items come from Strength of Materials on a typical CELE paper.
Shear and Moment Diagrams - Study Notes
Shear and moment diagrams (SFD and BMD) form the foundation of structural analysis in the PRC Civil Engineer Licensure Examination. These graphical representations show how internal shear forces and bending moments vary along a beam's length, directly enabling solutions in beam design, deflection calculations, and reinforced concrete or steel structural problems. Mastering their construction and interpretation is essential — nearly every structural design question requires finding the maximum moment and its location from these diagrams. This chapter builds competency from first principles: support reactions, sign conventions, the method of sections, and the load–shear–moment relationships that permit rapid sketching without extensive calculations.
Summary
Shear and moment diagrams are the graphical and quantitative record of how internal forces and moments vary along a beam's length, enabling all downstream structural design calculations. This chapter built your competency from fundamentals: support reactions, the sign convention (positive shear = left face up; positive moment = sagging), and the method of sections for exact solutions. The load–shear–moment relationships (dV/dx = −w, dM/dx = V) allow rapid sketching without equations, saving crucial exam time. Key insights include: (1) **M_max occurs where V = 0** or at support reactions; (2) **degree rule** predicts the shape of each diagram given the load type; (3) **point loads cause shear jumps**, applied couples cause moment jumps; and (4) **overhanging beams often have maximum moment at the interior support (hogging), not the span**. Mastery requires practice: solve 10–15 problems, memorize standard formulas, verify reactions and boundary conditions, and develop speed. The diagrams are the foundation for design under NSCP 2015, ACI 318, and AISC 360. Every structural professional must construct these diagrams accurately and interpret them without hesitation.
Sections
A beam is a structural member carrying transverse (perpendicular) loads and resisting them primarily through bending and shear. Understanding support types, reaction components, and load classifications is the prerequisite for drawing accurate diagrams. **Support Types and Reactions:** Each support type provides a specific number and type of reaction force or moment: - **Roller Support:** Provides one vertical reaction; restrains vertical translation only. The beam may rotate and translate horizontally freely. - **Pinned (Hinge) Support:** Provides two reactions (vertical and horizontal); restrains both translations but permits rotation. - **Fixed (Cantilever) Support:** Provides three reactions (vertical force, horizontal force, and moment); fully restrains the beam end against translation and rotation. **Load Classifications:** 1. **Concentrated (Point) Load, P:** A single force applied at a discrete point. Units: N, kN. Creates an immediate discontinuity (jump) in the shear diagram. 2. **Uniformly Distributed Load (UDL), w:** Constant load intensity over a length. Units: N/m, kN/m. The resultant force is W = wL, acting at the midpoint of the loaded region. Produces linear variation in shear and parabolic variation in moment. 3. **Uniformly Varying Load (UVL) / Triangular Load:** Load intensity varies linearly from zero at one end to w₀ at the other. Resultant force is (1/2)w₀L, positioned at the centroid of the triangle — critically, at L/3 from the larger-intensity end, not L/2. Results in parabolic shear and cubic moment. 4. **Applied Moment (Couple), M:** A concentrated rotational effect applied without translation. Creates a jump in the moment diagram but no change in shear. **Beam Classification:** - **Statically determinate beams** (simply supported, cantilever, overhanging): solvable using three equilibrium equations alone. - **Statically indeterminate beams** (fixed, propped cantilever, continuous): require additional methods beyond statics (discussed in Structural Theory). For the Civil Engineer Licensure Examination, emphasis is placed on determinate cases, particularly simply supported and cantilever beams.
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1. Fundamental Concepts: Beams, Supports, and Loads
Examples
Identifying Support Reactions
A simply supported beam (L = 8 m) at points A and B carries a UDL of 10 kN/m over its entire length. Find the vertical reactions.
Solution
Total load: W = wL = 10 × 8 = 80 kN. By symmetry: Rₐ = Rᵦ = 80/2 = 40 kN (both upward). Check: ΣFᵧ = 40 + 40 − 80 = 0 ✓
Locating UVL Resultant
A triangular load on a 6 m beam varies from 0 at the left to 12 kN/m at the right. Where does the resultant act, and what is its magnitude?
Solution
Magnitude: W = (1/2) × 12 × 6 = 36 kN. Location from left: x = (2/3) × 6 = 4 m (at the centroid, 2 m from the larger-intensity right end). Verify: 6 − 4 = 2 = 6/3 ✓
Key Points
- Roller provides 1 reaction (vertical); pin provides 2 (vertical + horizontal); fixed provides 3 (vertical + horizontal + moment)
- UDL resultant acts at midspan; triangular load resultant acts at 1/3 from the larger end
- Point loads create shear discontinuities; applied moments create moment discontinuities only
- Always verify static equilibrium (ΣFₓ = 0, ΣFᵧ = 0, ΣM = 0) before drawing diagrams
When a beam is cut at any section and one side is isolated as a free body, internal forces and moments emerge at the cut surface to maintain equilibrium. These internal effects are the shear force V and bending moment M. **Definition by the Method of Sections:** Make an imaginary cut perpendicular to the beam axis at distance x from a reference point. Isolate one side and apply equilibrium: - **Shear Force V(x):** The sum of all transverse (vertical) forces on one side of the cut, or equivalently, the internal vertical force pair at the section that prevents relative sliding. - **Bending Moment M(x):** The sum of all moments (about the section) from external loads on one side, or equivalently, the internal couple that prevents rotation of one part relative to the other. Mathematically: V(x) = Σ(transverse forces on isolated side) M(x) = Σ(moments about the section on isolated side) **Physical Interpretation:** - Shear represents the beam's resistance to sliding failure; maximum shear often governs design for lateral-torsional instability and web yielding in steel beams (per AISC 360-16). - Bending moment represents the beam's resistance to flexural failure; maximum moment governs flexural capacity, determines reinforcement in concrete beams (ACI 318), and is the primary design criterion for most beam problems. **Internal Stress Relationship:** At a given section, if the material behaves elastically: - Shear stress τ = V / A_shear (varies across the section; used for shear reinforcement design in concrete) - Bending stress σ = M·y / I (varies linearly from neutral axis; governs selection of steel grade and concrete compressive strength) For licensed engineers, the stress-strain relationship underlies all design codes (NSCP 2015 for concrete, AISC 360-16 for steel).
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2. Internal Shear Force and Bending Moment
Examples
Extracting Shear and Moment by Free-Body Method
A simply supported beam (L = 6 m) with reaction Rₐ = 30 kN at the left carries no additional load. Cut the beam at x = 2 m and find V and M.
Solution
Isolate the left portion (0 to 2 m). Vertical equilibrium: V = 30 kN (upward on the left face). Moment equilibrium about the cut: M = 30 × 2 = 60 kN·m (clockwise, positive sagging). With no distributed load, V is constant and M is linear.
Moment Calculation Under a Point Load
A cantilever beam (L = 4 m) fixed at the left, free at the right, carries a downward point load P = 20 kN at the free end. Find the moment at the fixed end.
Solution
Taking the moment of the load about the fixed support: M = −P·L = −20 × 4 = −80 kN·m (negative = hogging, tension at the top). At the fixed support, the reaction moment must be +80 kN·m to balance external moment equilibrium.
Key Points
- Shear force: internal transverse resistance to external loads; maximum at or near supports
- Bending moment: internal rotational resistance; typically maximum away from supports in simply supported beams
- V and M vary continuously along the beam and must be computed at every segment
- Sign convention errors are the leading cause of wrong diagrams — commit the convention to memory
The sign convention for shear and moment diagrams is standardized in structural mechanics and must be memorized exactly — sign errors are among the most common board-exam mistakes. **Shear Force Sign Convention:** Consider an element of the beam with a cut at each end. Internal shear forces act on the cut faces. - **Positive Shear V > 0:** The internal shear on the left cut face acts upward (equivalently, on the right face acts downward). Visualize this: the left portion tends to slide upward relative to the right. The internal couple formed by these opposite forces rotates the element **clockwise** — the positive rotational sense. - **Negative Shear V < 0:** The internal shear on the left face acts downward. The element tends to rotate **counterclockwise** — negative. **Mnemonic:** Positive shear "climbs up and to the left" — like a hand grasping the left face and pulling it upward. **Bending Moment Sign Convention:** - **Positive Moment M > 0 (Sagging):** The beam bends with curvature concave upward (smiles). The top fibers experience compression, the bottom fibers tension. Positive moment acts on the right cut face in the **counterclockwise direction** (top pulls, bottom pushes). Common in the interior of simply supported beams. - **Negative Moment M < 0 (Hogging):** The beam bends with curvature concave downward (frowns). The top fibers experience tension, the bottom fibers compression. Negative moment acts on the right cut face in the **clockwise direction**. Common over interior supports and along cantilevers. **Mnemonic:** Positive moment = a smile (happy beam, compression on top). Negative moment = a frown. **Sign Convention Applied to Free-Body Equilibrium:** When isolating the left portion of a cut beam and applying moment equilibrium about the cut section: - If you sum moments clockwise as positive, the internal moment M on the right face of the isolated left portion appears with a sign that follows the convention above. - Always be consistent: some engineers sum counterclockwise as positive; others use the convention stated here. Choose one and stick to it. **Critical Rule for the Exam:** Draw a small free-body diagram of a beam element at the section where you are computing shear and moment. Show the external loads and reactions on that element. Then show the internal shear and moment using the standard symbols. This discipline prevents sign errors.
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3. Sign Convention (Standard Beam Convention)
Examples
Applying Sign Convention to a Cantilever
A cantilever (L = 3 m) fixed at the left, free at the right, carries a downward point load P = 10 kN at the free end. At x = 1 m from the free end (i.e., 2 m from the fixed end), determine the shear and moment, with correct signs.
Solution
Isolate the right portion (from x = 1 m to the free end, a 1 m long segment). External load on this segment: P = 10 kN downward. Shear equilibrium: the cut face must provide an upward shear of 10 kN to balance. On the right face of the right segment, shear acts downward (internal action = reaction); on the left face (the cut), it acts upward. By convention, shear on the left face up = positive shear: V = +10 kN. Moment equilibrium about the cut: external moment = 10 × 1 = 10 kN·m clockwise (hogging). The internal moment on the cut must be −10 kN·m (counterclockwise by convention, = negative moment). So M(x=1 m) = −10 kN·m. The diagram bends downward (hogging) — correct for a cantilever loaded at the free end.
Sign Check in Simply Supported Beam
A simply supported beam (L = 6 m) with Rₐ = 18 kN, Rᵦ = 12 kN, carries no distributed load. At x = 2 m, find V and M with sign.
Solution
Isolate the left portion (0 to 2 m). Vertical forces: Rₐ = 18 kN up. Shear equilibrium: V = +18 kN (positive, left face up). Moment about the cut: M = 18 × 2 = +36 kN·m (sagging). The beam bends upward (concave up, smiles) — correct for a simply supported beam with load results concentrated near the left.
Key Points
- Positive shear: left face up, right face down → clockwise element rotation
- Negative shear: left face down, right face up → counterclockwise element rotation
- Positive moment: sagging (smile) → compression on top, tension on bottom
- Negative moment: hogging (frown) → tension on top, compression on bottom
- Always draw a free-body diagram of the isolated section; do not rely on memory alone
The method of sections is the exact, always-works procedure for deriving shear and moment equations V(x) and M(x) along the beam. While more time-consuming than using relationships (Section 5), it is essential for complex loadings and verifying results. **Step-by-Step Procedure:** 1. **Compute all reactions using global equilibrium:** - Apply ΣFₓ = 0, ΣFᵧ = 0, ΣM = 0 to the entire beam. - Verify: ΣFᵧ (up) = ΣFᵧ (down); this check prevents errors that propagate through all subsequent calculations. 2. **Identify segment boundaries:** - Divide the beam into segments at every discontinuity: each support, each point load, each applied couple, and at the start and end of each distributed load or load change. - Example: a beam from 0 to 10 m with supports at 0 and 10 m, a point load at 3 m, and a UDL from 4 to 8 m has segment boundaries at 0, 3, 4, 8, and 10 m → **five segments**. 3. **For each segment, cut at distance x and isolate one side:** - Choose the simpler side (fewer loads). Write equations for V(x) and M(x) from equilibrium. - V(x) = Σ(transverse forces on isolated side) - M(x) = Σ(moments about the section on isolated side) - Retain x as a variable; do not substitute numbers yet. 4. **Check continuity at segment boundaries:** - At boundaries without a point load or applied couple, V and M should match from either segment (continuous). - A point load causes V to jump by the load magnitude. - An applied couple causes M to jump by the couple magnitude (V unchanged). 5. **Plot V(x) and M(x):** - Use the equations to evaluate shear and moment at a few key points (supports, boundaries, load positions). - Sketch curves between points, noting the degree of each curve (constant, linear, parabolic, cubic). - Shade or label positive (above axis) and negative (below axis) regions. **Degree of Polynomial:** - **Point load only:** V is piecewise constant (degree 0, horizontal lines); M is piecewise linear (degree 1, straight lines). - **UDL:** V is piecewise linear (degree 1, straight lines); M is piecewise parabolic (degree 2, curved). - **Triangular (UVL) load:** V is piecewise parabolic (degree 2); M is piecewise cubic (degree 3). Each integration increases the degree by one.
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4. Method of Sections: The Systematic Procedure
Examples
Simply Supported Beam with Point Load — Method of Sections
A simply supported beam (L = 6 m) carries a point load P = 30 kN at x = 2 m. Draw SFD and BMD.
Solution
Step 1: Reactions. Taking moments about A: Rᵦ × 6 = 30 × 2 = 60 ⟹ Rᵦ = 10 kN. Then Rₐ = 30 − 10 = 20 kN. Check: ΣM_B = 20 × 6 − 30 × 4 = 120 − 120 = 0 ✓ Step 2: Segments: 0 to 2 m (left of load), and 2 to 6 m (right of load). Step 3a: Segment 0 ≤ x ≤ 2 (isolate left, simpler). No intermediate loads. V = Rₐ = 20 kN (constant). M = Rₐ · x = 20x (linear). At x = 0, M = 0; at x = 2, M = 40 kN·m. Step 3b: Segment 2 ≤ x ≤ 6 (isolate right, see load and right reaction). V = 10 kN (constant, positive shear on left face of the right portion). M = 10(6 − x) = 60 − 10x (linear). At x = 2, M = 40 kN·m; at x = 6, M = 0. Step 4: Continuity check. At x = 2⁻, M = 40; at x = 2⁺, M = 40. Shear jumps from 20 to 10 by ΔV = −30 = −P ✓ Step 5: Plot. SFD: horizontal line at +20 from 0 to 2, then at +10 from 2 to 6. BMD: linear rise from 0 to 40 kN·m over 0 to 2, then linear fall from 40 to 0 over 2 to 6. Peak moment: 40 kN·m at x = 2 m (under the load).
Cantilever with Distributed Load — Method of Sections
A cantilever (L = 4 m) fixed at the left, carries a UDL of w = 6 kN/m over its entire length. Find V(x) and M(x), and the maximum values.
Solution
Step 1: Reactions. Reaction at the fixed end: Rₐ = 6 × 4 = 24 kN (upward). Applied moment: M_A = 6 × 4 × 2 = 48 kN·m (hogging, to balance the moment of the load about the fixed support). Step 2: Single segment: 0 ≤ x ≤ 4 (no load change along the span). Step 3: Isolate the right portion (x to 4). Load on this portion: w(4 − x) = 6(4 − x) kN, distributed, resultant acting at the midpoint of the segment. Shear equilibrium: V(x) + 6(4 − x) = 0 ⟹ V(x) = 6(4 − x) = 24 − 6x. At x = 0, V = 24; at x = 4, V = 0. Moment equilibrium about the cut: M(x) + 6(4 − x) · [(4 − x)/2] = 0 ⟹ M(x) = −3(4 − x)². At x = 0, M = −3(16) = −48 kN·m. At x = 4, M = 0. Alternatively, from the fixed end (isolation): V(x) = 6x = 24 − 6x (no, error). Correct: isolate right, V = −w(4−x) on the right face; on the left cut face (by convention), V(x) acts upward if the beam section is in equilibrium. V(x) = 6(4 − x) (positive upward on left face). This is consistent. Step 5: SFD: straight line from 24 kN at x = 0 to 0 at x = 4 (V decreases linearly). BMD: parabola from −48 kN·m at x = 0 to 0 at x = 4 (opening downward). Maximum hogging moment is 48 kN·m at the fixed end.
Key Points
- Reactions first — every diagram error traces to incorrect reactions
- Identify segment boundaries at all load changes and supports
- Always isolate the simpler side to minimize algebra
- Check equilibrium: ΣFᵧ (up) must equal ΣFᵧ (down) for the whole beam
- Polynomial degree: point load adds 0 to V degree and 1 to M degree; UDL adds 1 to both
The relationships between load, shear, and moment are derived from differential equilibrium of an infinitesimal beam element. These are the key to rapid, accurate diagram sketching without writing equations — essential for time-pressured board exams. **Differential Relationships:** Consider an element of beam of length dx with load w(x) acting downward. Applying equilibrium: dV/dx = −w(x) [Slope of shear diagram = negative of load intensity] dM/dx = V(x) [Slope of moment diagram = shear] **Integrated Form (Areas and Changes):** Integrating over a distance from point A to point B: ΔV = V_B − V_A = −∫[A to B] w(x) dx = −(area under load diagram from A to B) ΔM = M_B − M_A = ∫[A to B] V(x) dx = (area under shear diagram from A to B) **Practical Interpretation for Board Exams:** 1. **Slope of SFD = negative load intensity at that point:** - No load (w = 0): shear is horizontal (flat). - Downward UDL (w > 0): shear has negative slope (line slopes downward to the right). - Upward load (w < 0): shear has positive slope. 2. **Slope of BMD = shear at that point:** - When V > 0 (positive shear): moment diagram has positive slope (rising to the right). - When V < 0: moment diagram has negative slope (falling). - When V = 0: moment diagram is horizontal (stationary) — **this is where M reaches a local extremum (maximum or minimum).** 3. **Change in shear = negative area under load diagram:** - A downward UDL from A to B reduces shear by the area w·(B−A). - A point load P at position C causes shear to drop by P. 4. **Change in moment = area under shear diagram:** - A positive (above-axis) shear region adds area to moment. - A negative shear region subtracts area. - The magnitude of moment change equals the area magnitude. **Key Insight for Finding M_max:** Locate the point where V = 0 or changes sign. At that point, the slope of M becomes zero (horizontal tangent) → **M is a local extremum there.** For simply supported beams with downward loads, where shear crosses from positive to negative, that crossing point is M_max (sagging). Over interior supports of continuous beams, where shear crosses from negative to positive, that crossing is M_max (hogging in magnitude). **Degree Rule (from Calculus):** Each integration raises the polynomial degree by 1: - If load is piecewise constant (degree 0), then V is piecewise linear (degree 1) and M is piecewise parabolic (degree 2). - If load is piecewise linear (degree 1, triangular), then V is piecewise parabolic (degree 2) and M is piecewise cubic (degree 3). **Discontinuities (Jumps):** - **Point load P at position c:** Shear diagram jumps by −P (downward load causes downward jump). - **Applied couple M_c at position c:** Moment diagram jumps by M_c (no effect on shear). **Sketching Without Equations (the "fast method"):** 1. Draw reaction arrows and label magnitudes (use method of sections if needed). 2. Start at the left support with V = R_A. Follow the load diagram: as you move right, reduce V by the area under the load. Mark where V crosses zero (M_max is here). 3. Start moment at M = 0 (at a support, usually). Follow the shear: as you move right, add area under shear to moment. Where shear crosses zero, mark the moment value — this is M_max. 4. Use the degree rule to sketch curves: straight lines between point loads; parabolas under UDL; no curves where w = 0. 5. Check: at the far end, V and M should match the known reaction and support moment (if fixed) — this verifies correctness.
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5. Load–Shear–Moment Relationships and Rapid Sketching
Examples
Using Load–Shear–Moment Relationships to Sketch Diagrams
A simply supported beam (L = 8 m) with reactions Rₐ = Rᵦ = 20 kN carries a UDL of 5 kN/m over its entire length. Use relationships to sketch the SFD and BMD without equations.
Solution
Step 1: Reactions verified. Rₐ = (5 × 8) / 2 = 20 kN; Rᵦ = 20 kN. Step 2: SFD. Start at A: V = +20 kN (upward reaction). As we move right, the load diagram is constant at 5 kN/m downward. The slope of the SFD is dV/dx = −5 (negative). Moving right, V decreases linearly: V(x) = 20 − 5x. At the midspan (x = 4), V = 0. Continuing, at x = 8, V = 20 − 40 = −20 kN. This matches −Rᵦ ✓ Step 3: Locate M_max. V crosses zero at x = 4 m → M is maximum there. Step 4: BMD. Start at A: M = 0 (simply supported). The area under the SFD from 0 to 4 is a triangle: (1/2) × 4 × 20 = 40 kN·m. So M(4) = 0 + 40 = 40 kN·m (M_max). From 4 to 8, the shear is negative (below axis), so moment decreases. Area from 4 to 8: (1/2) × 4 × (−20) = −40 kN·m. So M(8) = 40 − 40 = 0 ✓ (at support B). The BMD is a parabola (degree 2, since load is constant), symmetric about the midspan. Final Answer: V_max = 20 kN at the supports; M_max = 40 kN·m at midspan (x = 4 m).
Finding M_max Under a Triangular Load
A simply supported beam (L = 6 m) carries a triangular load varying from 0 at the left to 12 kN/m at the right. Without writing V(x), find the location and magnitude of M_max.
Solution
Step 1: Reactions. Total load: W = (1/2) × 12 × 6 = 36 kN at x = 4 m (centroid, 2/3 of 6 from left). Taking moments about A: Rᵦ × 6 = 36 × 4 ⟹ Rᵦ = 24 kN. Then Rₐ = 36 − 24 = 12 kN. Step 2: SFD. Start at A: V = 12 kN. The load intensity at x is w(x) = 2x (since it varies from 0 to 12 over 6 m). The area of the load diagram from 0 to x is the integral (1/2) × x × 2x = x². So V(x) = 12 − x². Setting V = 0: x² = 12 ⟹ x = 3.46 m. This is where M peaks. Step 3: M_max magnitude. The area under the SFD from A to x = 3.46 m is found by integrating the shear (which is parabolic due to the triangular load). V(x) = 12 − x², so ∫[0 to 3.46] (12 − x²) dx = [12x − x³/3]|₀^3.46 = 12(3.46) − (3.46)³/3 = 41.5 − 13.8 = 27.7 kN·m. Final Answer: M_max = 27.7 kN·m at x = 3.46 m (not at midspan, because the load is unsymmetrical).
Key Points
- Slope of SFD at any point = negative of load intensity there (dV/dx = −w)
- Slope of BMD at any point = shear at that point (dM/dx = V)
- M reaches extremum (max or min) where V = 0 — this is the gold standard for locating M_max
- Change in V between two points = negative area under load diagram
- Change in M between two points = positive area under shear diagram
- Point load causes shear jump; applied couple causes moment jump only
- Use degree rule: no load → V const, M linear; UDL → V linear, M parabolic; triangular → V parabolic, M cubic
For the board exam, memorizing these standard results allows instant verification and rapid problem-solving. Use them as a first check; if your answer differs significantly, re-examine your calculation. **Simply Supported Beam, Central Point Load P (symmetric):** - Span: L - Reactions: R_A = R_B = P/2 - Maximum shear: V_max = P/2 (at supports) - Maximum moment: M_max = PL/4 (at midspan, x = L/2) - Shear diagram: two horizontal lines, one above (P/2) and one below (−P/2), stepping at midspan - Moment diagram: two triangles meeting at the center, symmetric, with peak pointing up **Simply Supported Beam, Uniformly Distributed Load w over Entire Span:** - Total load: W = wL - Reactions: R_A = R_B = wL/2 - Maximum shear: V_max = wL/2 (at supports) - Maximum moment: M_max = wL²/8 (at midspan) - Shear diagram: straight line from +wL/2 at A to −wL/2 at B, crossing zero at L/2 - Moment diagram: parabola opening downward (concave down in shape) with peak at L/2. The curvature matches the load diagram (also parabolic by the degree rule). **Simply Supported Beam, Point Load P at Distance a from Left (b = L − a):** - Reactions: R_A = Pb/L (downward load closer to B → smaller R_A); R_B = Pa/L - Maximum moment: M_max = Pab/L (at x = a, directly under the load, provided a < b) - Shear diagram: positive constant (+Pb/L) from A to the load, then negative constant (−Pa/L) from the load to B - Moment diagram: linear rise from 0 to M_max over distance a, then linear fall to 0 over distance b - **Key:** M_max always occurs **under the point load**, regardless of symmetry **Cantilever Beam, Point Load P at the Free End:** - Maximum shear: V = P (constant along the beam, in the direction of the load) - Maximum moment: M_max = −PL (at the fixed end, negative = hogging). Magnitude: |M| = PL - Shear diagram: horizontal line at P (if P is downward, show as negative by convention, V = −P; but magnitude is P) - Moment diagram: straight line from 0 at the free end to −PL at the fixed end **Cantilever Beam, Uniformly Distributed Load w over Entire Length:** - Maximum shear: V_max = wL (at the fixed end) - Maximum moment: M_max = −wL²/2 (at the fixed end, hogging, magnitude wL²/2) - Shear diagram: straight line from 0 at the free end to −wL at the fixed end (negative because w is downward) - Moment diagram: parabola, concave down, from 0 at the free end to −wL²/2 at the fixed end **Overhanging Beam: Two Supports at A and B, Overhang Beyond B:** - Critical consideration: **M_max can occur at the interior support (hogging), not within the span.** Always check both interior and exterior regions. - Use the method of sections or load–shear–moment relationships to find V = 0 points (candidates for M_max). - Typical issue on board exams: students find sagging moment in the span but miss the larger hogging moment at the support. **Propped Cantilever (Fixed at A, Roller Support at B):** - Indeterminate structure: requires superposition or other advanced methods (beyond scope of simple diagrams). - However, SFD and BMD can be sketched once reactions are known (from Structural Theory course or provided).
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6. Standard Formulas: Ready Reference for Common Cases
Examples
Applying Standard Formula — Simply Supported with Point Load at Midspan
A simply supported beam (L = 10 m) carries P = 50 kN at the midspan. Verify M_max using the formula.
Solution
Using M_max = PL/4 = 50 × 10 / 4 = 125 kN·m at x = 5 m. Check by method of sections: Rₐ = Rᵦ = 25 kN (by symmetry). At x = 5, moment = 25 × 5 = 125 kN·m ✓
Cantilever Verification — Standard Formula
A cantilever (L = 5 m) carries UDL w = 8 kN/m. Verify M_max at the fixed end using the formula.
Solution
Using M_max = wL²/2 = 8 × 5² / 2 = 8 × 25 / 2 = 100 kN·m (hogging). By sections: isolate the whole beam from the right, resultant load 8 × 5 = 40 kN at 2.5 m from fixed. Moment = −40 × 2.5 = −100 kN·m ✓ (hogging)
Key Points
- M_max under a point load occurs at the load location, not necessarily at midspan
- For UDL on simply supported span, M_max = wL²/8 at midspan always
- Cantilever M_max = −wL²/2 (parabolic moment) or −PL (linear moment), both at the fixed end
- Overhanging beams: check both interior (sagging) and support (hogging) regions for M_max
- Store these formulas in a quick-reference table for exam use; they catch calculation errors
- Reactions first: if reactions are wrong, all subsequent work is wrong
These examples demonstrate the full process from reactions to final diagrams, at the level expected in the PRC Civil Engineer Licensure Examination.
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7. Worked Examples: Board-Level Problems
Examples
Example 1: Simply Supported Beam with Multiple Point Loads
A simply supported beam (L = 12 m) carries point loads: P₁ = 20 kN at x = 3 m, P₂ = 30 kN at x = 7 m, and P₃ = 10 kN at x = 10 m. Draw the SFD and BMD, and identify M_max.
Solution
**Step 1: Reactions.** Total downward load: W = 20 + 30 + 10 = 60 kN. By global equilibrium: ΣM_A = 0: Rᵦ(12) = 20(3) + 30(7) + 10(10) = 60 + 210 + 100 = 370 Rᵦ = 370 / 12 = 30.83 kN Rₐ = 60 − 30.83 = 29.17 kN **Step 2: Segment boundaries:** At x = 0, 3, 7, 10, 12 m → five segments. **Step 3: Shear in each segment** (no distributed load, so V is constant in each region): - 0 ≤ x < 3: V = Rₐ = 29.17 kN (positive) - 3 ≤ x < 7: V = 29.17 − 20 = 9.17 kN (positive) - 7 ≤ x < 10: V = 9.17 − 30 = −20.83 kN (negative, drops across P₂) - 10 ≤ x ≤ 12: V = −20.83 − 10 = −30.83 kN (negative, drops across P₃) **Step 4: Moment in each segment** (using M(x) = M(prev) + ΔM, where ΔM = area under SFD): - At x = 0: M = 0 (support) - At x = 3: ΔM = 29.17(3) = 87.5 kN·m → M = 87.5 kN·m - At x = 7: ΔM = 9.17(7−3) = 36.7 kN·m → M = 87.5 + 36.7 = 124.2 kN·m (this is M_max) - At x = 10: ΔM = −20.83(10−7) = −62.5 kN·m → M = 124.2 − 62.5 = 61.7 kN·m - At x = 12: ΔM = −30.83(12−10) = −61.7 kN·m → M = 61.7 − 61.7 = 0 ✓ (support, as expected) **Step 5: Diagrams.** SFD: horizontal at +29.17 from 0 to 3; jump down to +9.17 at x = 3; jump down to −20.83 at x = 7; jump down to −30.83 at x = 10. BMD: connected linear segments, starting at 0, rising to 87.5 (x = 3), rising to 124.2 (x = 7), falling to 61.7 (x = 10), falling to 0 (x = 12). All corners are straight (no curves, as there is no distributed load). **Result:** M_max = 124.2 kN·m at x = 7 m (under the largest load, P₂).
Example 2: Simply Supported Beam with UDL and Point Load
A simply supported beam (L = 10 m) carries a UDL of w = 6 kN/m over the entire length, plus a concentrated load P = 20 kN at x = 6 m. Find M_max and its location.
Solution
**Step 1: Reactions.** Total distributed load: W_d = 6(10) = 60 kN at x = 5 m. Total load: W_total = 60 + 20 = 80 kN. Taking moments about A: Rᵦ(10) = 60(5) + 20(6) = 300 + 120 = 420 Rᵦ = 42 kN Rₐ = 80 − 42 = 38 kN **Step 2: Segments:** Two regions, 0 to 6 m (UDL only) and 6 to 10 m (UDL + point load). **Step 3: Shear equations.** - 0 ≤ x ≤ 6: V(x) = 38 − 6x (linear, UDL causes negative slope) At x = 0: V = 38 kN At x = 6: V = 38 − 36 = 2 kN - 6 ≤ x ≤ 10: V(x) = 2 − 20 = −18 kN at x = 6⁺ (jump by −20 at the point load) Wait, recalculate. At x = 6⁻ (just before load), V = 38 − 6(6) = 2 kN. At x = 6⁺ (just after), the load P = 20 kN is now on the right side (isolated), so V decreases by 20: V = 2 − 20 = −18 kN. But this is wrong; the point load is on the cut. Correct approach: at x = 6⁻, shear from distributed load alone: V = 38 − 6(6) = 2 kN. The point load P = 20 kN now acts downward on the right segment. So V(6⁺) = 2 − 20 = −18 kN. Continue with UDL: V(x) = −18 − 6(x − 6) for 6 < x ≤ 10. At x = 10: V = −18 − 6(4) = −42 kN... but this should be −42 kN (the right reaction, which should be 42 kN downward on the right side of the cut, i.e., −42 from the left perspective). Error: reactions verified above: Rᵦ = 42 kN (upward). At x = 10⁻, V = −18 − 24 = −42 kN... but the reaction is upward, so shear on the left face of the support is downward (negative). This is a sign check: V(10⁻) = −42 kN, and the reaction (upward) on the right face of the left segment is +42 kN, so the net is 0 ✓ (equilibrium of the right edge). Let me recalculate the second segment more carefully. Isolate the right portion (x to 10). Downward load: 6(10 − x) + 20 (point load is part of the section's loads). Shear on the left face of the right segment: V(x) = 6(10 − x) + 20 = 60 − 6x + 20 = 80 − 6x. At x = 6: V = 80 − 36 = 44 kN... this doesn't match the left segment result of 2 kN. There is an issue with segment boundaries. Actually, the point load is at x = 6, so it acts on both segments at the boundary. When isolating the left portion up to x = 6, the load P is NOT included; when isolating the right portion from x = 6 onward, the load IS included. So there's a jump in shear at x = 6 equal to −P = −20 kN. Recalculate: - 0 ≤ x ≤ 6: V(x) = 38 − 6x (UDL only). At x = 6⁻: V = 2 kN. - 6 < x ≤ 10: The point load is now active. Isolate the right portion (x to 10): load is 6(10 − x) from UDL + 20 from the point. Total: 60 − 6x + 20 = 80 − 6x... but wait, this gives V = 80 − 6x at x = 6⁺ = 80 − 36 = 44 kN, not 2 − 20 = −18 kN. The error is in the free-body. Let me redo. Isolate the **left** portion including the point load (0 to x, where x > 6): V(x) = Rₐ − 6x − 20 = 38 − 6x − 20 = 18 − 6x. At x = 6⁺: V = 18 − 36 = −18 kN. At x = 10: V = 18 − 60 = −42 kN ✓ (matches −Rᵦ as expected). So the corrected segments are: - 0 ≤ x ≤ 6: V(x) = 38 − 6x - 6 < x ≤ 10: V(x) = 18 − 6x (point load included) At x = 6: V jumps from 2 to −18, a drop of −20 = −P ✓ **Step 4: Find M_max.** From the first segment, V = 38 − 6x = 0 at x = 6.33 m... but x = 6.33 is not in the first segment (which ends at 6). At x = 6, V = 2 kN (still positive). In the second segment, V = 18 − 6x = 0 at x = 3 m... but x = 3 is not in the second segment (which starts at 6). At x = 10, V = −42 kN. So V crosses zero somewhere in the second segment... Wait, at x = 6, V = −18, and at x = 10, V = −42. V does not cross zero in the second segment; it stays negative. Therefore, V never crosses zero after x = 6. Conclusion: **M_max occurs at x = 6 m (at the boundary, where V changes sign most abruptly)** or within the first segment where V is positive. But within 0 to 6, V > 0 always, so M is increasing. At x = 6, M reaches a local peak (though V does not zero there). So let's compute moment to see. **Step 5: Moment equations.** - 0 ≤ x ≤ 6: M(x) = Rₐ·x − (1/2)·6·x² = 38x − 3x² At x = 6: M = 38(6) − 3(36) = 228 − 108 = 120 kN·m To find the extremum in this segment, take dM/dx = dV/dx: dM/dx = 38 − 6x = 0 at x = 6.33 m. But x = 6.33 is outside [0, 6], so the extremum is not in this segment. M is increasing throughout [0, 6]. - 6 < x ≤ 10: M(x) = Rₐ·x − (1/2)·6·x² − 20(x − 6) = 38x − 3x² − 20x + 120 = 18x − 3x² + 120 dM/dx = 18 − 6x = 0 at x = 3 m (not in this segment). At x = 6⁺: M = 18(6) − 3(36) + 120 = 108 − 108 + 120 = 120 kN·m ✓ (continuous). At x = 10: M = 18(10) − 3(100) + 120 = 180 − 300 + 120 = 0 ✓ (support). In the second segment [6, 10], dM/dx = 18 − 6x is negative (since 18 − 6x < 18 − 36 = −18 < 0 for all x ≥ 6). So M is decreasing in [6, 10]. **Result:** M_max = 120 kN·m at x = 6 m (at the point load location, where shear transitions from positive to negative). **SFD:** Start at 38 kN at x = 0. Linear decrease (slope −6) to 2 kN at x = 6. Jump down to −18 kN at x = 6. Continue linear decrease (slope −6) to −42 kN at x = 10. **BMD:** Parabolic rise from 0 to 120 kN·m over [0, 6] (concave down, since w > 0). Linear fall from 120 to 0 over [6, 10] (no distributed load in the second segment, so M is linear)... Wait, there IS a distributed load in the second segment (the UDL continues). So M should be parabolic there too. Let me reconsider. The moment equation in the second segment is M(x) = 18x − 3x² + 120, which is parabolic (degree 2). So the BMD is parabolic throughout. At x = 6, the parabola has a corner? No, the function M(x) is continuous and smooth. The first parabola is M = 38x − 3x² and the second is M = 18x − 3x² + 120. They have the same derivative at x = 6: dM/dx = 38 − 12(6) = −34 from the first; dM/dx = 18 − 12(6) = −54 from the second. These differ, so there's a kink in the derivative (the BMD has a corner in slope at x = 6). This is caused by the point load. **Final Answer:** M_max = 120 kN·m at x = 6 m.
Example 3: Cantilever with Combined Loading
A cantilever (L = 6 m) fixed at the left, carries a UDL of w = 4 kN/m over its entire length and a point load P = 15 kN at the free end. Find V_max, M_max, and sketch the diagrams.
Solution
**Step 1: Reactions at the fixed support.** Vertical reaction: R = wL + P = 4(6) + 15 = 24 + 15 = 39 kN (upward at the fixed end). Applied moment at the fixed end: M = −[wL·(L/2) + P·L] = −[4(6)(3) + 15(6)] = −[72 + 90] = −162 kN·m (hogging). **Step 2: Shear equation.** For a cantilever, isolate the right portion (from x to the free end at 6 m). Load on this segment: w(6 − x) from UDL + P from point. Total: 4(6 − x) + 15 = 24 − 4x + 15 = 39 − 4x. Shear on the left face of the right segment: V(x) = 39 − 4x. At x = 0 (fixed end): V = 39 kN. At x = 6 (free end): V = 39 − 24 = 15 kN... wait, at the free end there should be only the point load, so V = 15 kN ✓ Actually, the shear at the free end is the point load itself: V = P = 15 kN ✓ Wait, I need to reconsider the sign. The point load P = 15 kN acts downward (typical). If we isolate the right portion and apply vertical equilibrium, the internal shear on the left face must balance the downward load. So V = 15 kN (upward on the left face, positive by convention). But as we move left, the distributed load increases. Let's recalculate. Isolate the right portion (x to 6): load is 4(6 − x) + 15 downward. Shear on the left face (upward, positive): V(x) = 4(6 − x) + 15 = 24 − 4x + 15 = 39 − 4x. At x = 6: V = 15 kN ✓. At x = 0: V = 39 kN ✓. But for a cantilever with loads, we typically report shear as positive downward (since the cantilever sags under load). Let me use the standard sign convention: positive shear means left face up, right face down. In a cantilever, this becomes confusing. Instead, use the magnitude and remember that for a cantilever loaded downward, the internal shear at the support is equal to the total load (upward reaction). For this problem, |V_max| = 39 kN at the fixed end. **Step 3: Moment equation.** M(x) = −[4(6 − x)·(6 − x)/2 + 15(6 − x)] = −[2(6 − x)² + 15(6 − x)] = −[(6 − x)[2(6 − x) + 15]] = −[(6 − x)(12 − 2x + 15)] = −[(6 − x)(27 − 2x)] Let u = 6 − x, then M = −[u(27 − 2(6 − u))] = −[u(27 − 12 + 2u)] = −[u(15 + 2u)] = −[15u + 2u²] = −[15(6 − x) + 2(6 − x)²] = −[90 − 15x + 2(36 − 12x + x²)] = −[90 − 15x + 72 − 24x + 2x²] = −[162 − 39x + 2x²] = −162 + 39x − 2x². At x = 0: M = −162 kN·m (hogging) ✓ At x = 6: M = −162 + 39(6) − 2(36) = −162 + 234 − 72 = 0 ✓ (free end, no moment) To find extremum: dM/dx = 39 − 4x = 0 at x = 9.75 m... but this is beyond the beam length (6 m). So the extremum is at a boundary. Since dM/dx = 39 − 4x > 0 for x < 6, M is increasing from x = 0 to x = 6. But M(0) = −162 < M(6) = 0, so M increases from negative to zero. The maximum (least negative) moment is at x = 6 (M = 0), and the **magnitude maximum** is at x = 0 (|M| = 162 kN·m, hogging). For design purposes, **M_max = 162 kN·m (hogging, at the fixed support).** **Step 4: Diagrams.** SFD: Linear from 39 kN at x = 0 to 15 kN at x = 6 (slope = −4 from the UDL). No jumps (the point load is distributed with the UDL in the load diagram). BMD: Parabolic (degree 2, from the UDL) from −162 kN·m at x = 0 to 0 at x = 6. The parabola opens downward (concave down), with the curvature matching the UDL diagram. Moment is always negative (hogging), typical for a cantilever. **Final Answer:** V_max = 39 kN, M_max = 162 kN·m (hogging) both at the fixed support.
Example 4: Triangular Load and Finding M_max at Zero Shear
A simply supported beam (L = 8 m) carries a triangular load varying from 12 kN/m at the left to 0 at the right. Find the location and magnitude of M_max using the load–shear–moment relationships.
Solution
**Step 1: Reactions.** Total load: W = (1/2)·12·8 = 48 kN, acting at the centroid of the triangle, 1/3 from the larger end (left): x = 8/3 ≈ 2.67 m. Taking moments about A: Rᵦ·8 = 48·(8/3) = 128 Rᵦ = 16 kN Rₐ = 48 − 16 = 32 kN **Step 2: Shear equation.** The load intensity at distance x is w(x) = 12(1 − x/8) = 12 − 1.5x kN/m (decreases from 12 at x=0 to 0 at x=8). Shear at x: V(x) = Rₐ − ∫[0 to x] w(ξ) dξ = 32 − ∫[0 to x] (12 − 1.5ξ) dξ = 32 − [12ξ − 0.75ξ²]|₀^x = 32 − 12x + 0.75x² Alternatively, from the right: V(x) = Rᵦ + ∫[x to 8] w(ξ) dξ = 16 + ∫[x to 8] (12 − 1.5ξ) dξ = 16 + [12ξ − 0.75ξ²]|ₓ^8 = 16 + (96 − 48) − (12x − 0.75x²) = 16 + 48 − 12x + 0.75x² = 64 − 12x + 0.75x²... Wait, this doesn't match. Let me recalculate. Isolate the right portion (x to 8 m): load is ∫[x to 8] (12 − 1.5ξ) dξ. Compute: [12ξ − 0.75ξ²]|ₓ^8 = (96 − 48) − (12x − 0.75x²) = 48 − 12x + 0.75x². Shear on the left face of this segment: V(x) = 48 − 12x + 0.75x². At x = 0: V = 48 kN... but from the left, V = 32 kN. Error. Let me reconsider. The load w(x) is the downward intensity. The resultant from x to 8 is ∫[x to 8] w dξ = 48 − 12x + 0.75x². This is downward. So on the left face of the right segment (isolating that segment as a free body), the internal shear V must balance this load: V + (48 − 12x + 0.75x²) = 0... no, that's not right either. Correct approach: Isolate the right segment. External forces: distributed load (downward) = 48 − 12x + 0.75x² (computed above). Support reaction at B: Rᵦ = 16 kN (upward). Internal shear at the left cut face of the segment: V(x) (positive if upward). Equilibrium: V(x) + 16 − (48 − 12x + 0.75x²) = 0 ⟹ V(x) = 48 − 12x + 0.75x² − 16 = 32 − 12x + 0.75x². At x = 0: V = 32 kN ✓. At x = 8: V = 32 − 96 + 48 = −16 kN (the upward reaction at B is 16, so shear on the left face of B is downward, −16) ✓. So V(x) = 32 − 12x + 0.75x² (parabolic, opens upward). **Step 3: Find where V = 0.** 32 − 12x + 0.75x² = 0 0.75x² − 12x + 32 = 0 Multiply by 4/3: x² − 16x + 42.67 = 0 Using the quadratic formula: x = [16 ± √(256 − 170.67)] / 2 = [16 ± √85.33] / 2 = [16 ± 9.24] / 2 x = 12.62 m or x = 3.38 m Only x = 3.38 m is within the beam span [0, 8]. So **M_max occurs at x = 3.38 m.** **Step 4: Moment at x = 3.38 m.** M(x) = Rₐ·x − ∫[0 to x] [integral of load] = Rₐ·x − ∫[0 to x] w·(x − ξ) dξ This is complex. Easier to use: M(x) = Rₐ·x − [area under load curve from 0 to x], where the area is evaluated with the lever arm of the centroid. Load from 0 to x: W(x) = ∫[0 to x] w(ξ) dξ = 12x − 0.75x². Centroid of this load: x_c = ∫[0 to x] ξ·w(ξ) dξ / W(x). This is getting complicated. Alternatively, use M(x) = Rₐ·x − ∫[0 to x] V(ξ) dξ... no, that's circular (M' = V). Simplest: integrate V to get M: M(x) = ∫[0 to x] V(ξ) dξ = ∫[0 to x] (32 − 12ξ + 0.75ξ²) dξ = [32ξ − 6ξ² + 0.25ξ³]|₀^x = 32x − 6x² + 0.25x³ At x = 3.38: M = 32(3.38) − 6(3.38)² + 0.25(3.38)³ = 108.16 − 68.52 + 9.73 = 49.37 kN·m **Verification at boundaries:** At x = 0: M = 0 ✓ At x = 8: M = 32(8) − 6(64) + 0.25(512) = 256 − 384 + 128 = 0 ✓ **Final Answer:** M_max = 49.37 kN·m (approximately 49.4 kN·m) at x = 3.38 m (approximately 1/3 from the left, near the load centroid but not exactly). This example shows why the "Where V = 0" rule is powerful: once V is known, the location of M_max follows immediately without deriving the moment equation explicitly. The moment magnitude still requires integration, but the location is found with just algebra.
Key Points
- Always find and verify reactions before drawing diagrams
- Identify segment boundaries at every load change
- Locate M_max at points where V = 0
- Check your diagrams: at far end, V and M should match support conditions
- Use both method of sections and load–shear–moment relationships for verification
Board exams frequently test understanding through trick questions and common misconceptions. Awareness of these pitfalls improves accuracy dramatically. **Pitfall 1: Forgetting the Shear Jump at a Point Load** A point load creates a discontinuity (jump) in the shear diagram equal to the load magnitude. Many students draw a smooth curve through the load point, forgetting the step. This error cascades: if the shear diagram is wrong, the moment diagram location of zero shear (and thus M_max) is also wrong. *Prevention:* Always mark point load locations on the shear diagram. Draw a vertical line at the load; shear jumps by −P (for downward P). **Pitfall 2: Misunderstanding the Sign Convention** Confusing which direction is "positive" shear or moment causes diagrams to be flipped. A simply supported beam with downward loads should show positive moment in the interior (sagging, smile). If your BMD is inverted (frown in the interior), your sign convention is backwards. *Prevention:* Draw a small free-body element with forces and moments labeled. Enforce the convention consistently throughout. **Pitfall 3: Wrong Centroid of Triangular Load** A triangular load with intensity 0 at the left and w_o at the right has its resultant (1/2)w_o·L acting at x = L/3 from the left, NOT at L/2. Students often place the resultant at the geometric midpoint. *Prevention:* Memorize: "centroid of triangle is at 1/3 from the **larger** end." Verify by integration: centroid = ∫x·w(x)dx / ∫w(x)dx. **Pitfall 4: Ignoring Applied Couples** An applied couple (external moment) creates a jump in the moment diagram but **no change in shear**. Students sometimes mistakenly add it to shear. *Prevention:* Remember: couples affect moment only. Check the SFD for continuity across an applied-couple location. **Pitfall 5: Maximum Moment in Overhanging Beams** In an overhanging beam, the maximum moment can occur at the interior support (hogging), not within the main span (sagging). Many students find the sagging moment within the span and miss the larger hogging moment at the support. *Prevention:* Check all regions: interior span (sagging), at supports (hogging), and overhang. Compute M at critical points: where V = 0, at supports, at load positions. Compare magnitudes. **Pitfall 6: Not Verifying Reactions** Reactions set the starting point for all diagrams. A wrong reaction propagates to every subsequent calculation. Yet, many students skip equilibrium checks. *Prevention:* Always verify: ΣF_y (up) = ΣF_y (down), and take moments about two different points to double-check R_A and R_B. **Pitfall 7: Confusing Cantilever Fixed Support Moment** A cantilever fixed at one end has a reaction moment at the fixed end (usually hogging). This reaction moment is not an externally applied couple; it's the internal moment required to balance the loads. Students sometimes forget to include it when drawing the BMD. *Prevention:* For a cantilever, always compute the reaction moment: M_fixed = −Σ(moment of external loads about fixed end). Include this as the BMD value at x = 0. **Pitfall 8: Forgetting Boundary Conditions in SFD and BMD** At a simply supported end, V ≠ 0 (there's a reaction) but M = 0. At a cantilever fixed end, V and M are both non-zero. At a free end, both V and M are typically zero unless there's a load or couple right at the end. *Prevention:* Sketch the support symbols and reactions before drawing diagrams. Use them as anchoring points. **Pitfall 9: Polynomial Degree Mistakes** A constant load (no UDL, only point loads) should produce a linear moment diagram, not parabolic. Students sometimes confuse the degree rule. *Prevention:* Point load → V constant, M linear. UDL → V linear, M parabolic. UVL → V parabolic, M cubic. Sketch only straight lines or the appropriate curve.
Heading
8. Common Pitfalls and Exam Errors
Examples
Pitfall Example 1: Forgetting the Shear Jump
A beam carries a 20 kN downward point load at midspan. A student draws the SFD as a smooth line without a jump at the load. Explain the error.
Solution
At a point load, shear must drop suddenly by the load magnitude. If the student drew a smooth curve, they implicitly assumed the load is distributed over a small region, not concentrated. The correct SFD has a vertical jump (the load acts at a single point, creating an instantaneous change in internal shear). The erroneous smooth curve would lead to a wrong location for M_max (where the (incorrectly smooth) SFD crosses zero).
Pitfall Example 2: Wrong Triangular Load Centroid
A beam carries a triangular load: 0 at the left, 10 kN/m at the right, over a 6 m span. A student places the resultant at x = 3 m (midspan). The correct centroid is at what location?
Solution
Resultant = (1/2)(10)(6) = 30 kN. Centroid from the left (larger end at right): x = (2/3)(6) = 4 m, NOT 3 m. The student's placement at the midpoint is a common error. Using the wrong centroid location leads to incorrect reaction magnitudes and thus wrong diagrams throughout.
Pitfall Example 3: Overhanging Beam Maximum Moment
An overhanging beam spans 6 m (A to B) and overhangs 2 m to C, carrying UDL 4 kN/m everywhere. A student finds the sagging moment in the span as 6 kN·m but forgets to check the hogging moment at B. What is the true M_max?
Solution
Check the hogging moment at the interior support B. Total load on the overhang: 4(2) = 8 kN at 1 m from B. Moment at B (from the right): M_B = −4(2)(1) = −8 kN·m (hogging). This exceeds the 6 kN·m sagging moment in the span. **True M_max = 8 kN·m (hogging), not 6 kN·m.** The student missed the interior support by focusing only on the span.
Key Points
- Point load causes shear jump; applied couple causes moment jump only
- Triangular load centroid is at 1/3 from the larger-intensity end, not 1/2
- Always verify reactions: ΣF = 0 and ΣM = 0 for the whole beam
- Check overhanging beams for hogging moment at the support, not just sagging in the span
- Use the degree rule: constant load → linear M; UDL → parabolic M; triangular → cubic M
- Cantilever fixed support has both reaction force and reaction moment; include the moment in BMD
Mastery of shear and moment diagrams is foundational for Civil Engineer licensure success. These diagrams appear in nearly every structural design problem: reinforced concrete beams (ACI 318), steel beams (AISC 360), and Filipino design standards (NSCP 2015). The following summary and strategy guide your preparation. **Core Competencies You Must Demonstrate:** 1. **Reaction Calculation:** Using ΣF = 0 and ΣM = 0, find all support reactions. Verify your answer by checking equilibrium about a second point or summing forces in the opposite direction. 2. **Segment Identification:** Identify all boundaries (supports, point loads, load changes) and classify each segment (uniform load, point load only, etc.). 3. **Shear Diagram Sketching:** Use either the method of sections (exact) or the load–shear–moment relationships (fast). Mark shear at key points, show jumps at point loads, and use the degree rule (constant → V const, UDL → V linear, etc.). 4. **Moment Diagram Sketching:** Plot moment at segment boundaries. Use the load–shear–moment relationship: area under SFD = change in moment. Identify where V = 0 (extremum of M). 5. **Locating M_max:** Search for V = 0 or V crossing zero. At such points, M reaches a local extremum. Compare M at all critical points: supports, load positions, V = 0 locations. Report the largest magnitude as M_max. 6. **Verification:** Check boundary values (M = 0 at simply supported ends; M and V non-zero at fixed ends; both zero at free ends unless loaded there). Verify continuity (except at point loads and applied couples). **Time Management During the Exam:** - **First 1 minute:** Read the problem, sketch the beam, mark supports and loads. - **Next 2 minutes:** Compute reactions using global equilibrium. Double-check. - **Next 3 minutes:** Draw the SFD using the load–shear–moment relationships (faster than method of sections). - **Next 2 minutes:** Mark V = 0 locations on the SFD. - **Next 2 minutes:** Draw the BMD, using the SFD to find slopes and areas. - **Final 1 minute:** Verify M_max location and magnitude. Check boundary conditions. - **Total: ~11 minutes per beam problem** (typical exam problem). **What the PRC Examiners Test:** Examiners expect you to: - Find M_max quickly (it's the design driver). - Sketch diagrams that are qualitatively correct (shapes, signs, continuity). - Identify critical sections for design (where M is maximum, where V is maximum, where combined stress is worst). - Apply the diagrams to downstream design (e.g., "find the required beam section given M_max"). **Recommended Resources for Practice:** - Work 10–15 problems of varying complexity: simply supported with UDL, cantilever with point load, overhanging with triangular load, etc. - For each, draw both diagrams; find V_max and M_max; verify reactions and boundary conditions. - Compare your results with a solutions manual or instructor feedback. - Memorize the standard formulas (Section 6) and use them as sanity checks. **Red Flags — If You Can't Do These, Review the Chapter:** 1. Can you identify the sign of shear at a point without hesitation? 2. Can you sketch the SFD for a cantilever with both distributed and point loads in under 2 minutes? 3. Can you locate M_max without writing equations, using only the load–shear–moment relationships? 4. Can you explain why the moment diagram under a UDL is parabolic (degree rule)? 5. Can you identify the centroid of a triangular load correctly? If you struggle with any of these, revisit the corresponding section before moving to the next chapter.
Heading
9. Summary and Exam Strategy
Examples
Key Points
- Reactions first: ΣF = 0, ΣM = 0, verify by a second moment equation
- Segment identification: mark all load boundaries
- Sketch SFD using slopes = −w(x); mark jumps at point loads
- Sketch BMD using areas under SFD; find M_max where V = 0
- Verify: boundary conditions (M=0 at simple support), continuity except at loads/couples
- Time target: ~11 minutes per problem; practice to speed up
- Use standard formulas as sanity checks
- Examiners prioritize M_max location and magnitude — the design driver
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