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Chapter 1 of 12 • Page 1 of 248🔒 Protected PDF • Watermarked
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CivilStructural Mechanics-II
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A simply supported beam of span l, carrying udl of w on entire span, slope at both end will be

A

Wl216EI\frac{Wl^2}{16EI}16EIWl2​

B

5wl4384EI\frac{5wl^4}{384EI}384EI5wl4​

C

wl324EI\frac{wl^3}{24EI}24EIwl3​

D

Wl348EI\frac{Wl^3}{48EI}48EIWl3​

Correct Answer

⚙️ TE • Technical Concept & PrincipleCivilStructural Mechanics-II
Option C

wl324EI\frac{wl^3}{24EI}24EIwl3​

Quick Summary:

For a simply supported beam of span lll subjected to a uniformly distributed load (udl) of www per unit length over its entire span, the maximum slope occurs at the supports. The slope (heta hetaheta) at both ends is given by the expression θ=wl324EI\theta = \frac{wl^3}{24EI}θ=24EIwl3​, where EEE is Young's Modulus and III is the Moment of Inertia.

⚙️TETechnical SolutionConcept & Principle
💡 Explanation

For a simply supported beam of span lll subjected to a uniformly distributed load (udl) of www per unit length over its entire span, the maximum slope occurs at the supports. The slope (heta hetaheta) at both ends is given by the expression θ=wl324EI\theta = \frac{wl^3}{24EI}θ=24EIwl3​, where EEE is Young's Modulus and III is the Moment of Inertia.

🔢 Key Formulas

θ=wl324EI\theta = \frac{wl^3}{24EI}θ=24EIwl3​ — Slope at the ends of a simply supported beam with UDL

δmax=5wl4384EI\delta_{max} = \frac{5wl^4}{384EI}δmax​=384EI5wl4​ — Maximum deflection at the center of a simply supported beam with UDL

⚙️ Working Principle

According to the double integration method or Macaulay's method, the governing differential equation for beam deflection is EId2ydx2=MxEI\frac{d^2y}{dx^2} = M_xEIdx2d2y​=Mx​. By integrating this equation twice and applying boundary conditions (deflection y=0y=0y=0 at x=0x=0x=0 and x=lx=lx=l), we derive the expression for the slope dydx\frac{dy}{dx}dxdy​. At the supports (x=0x=0x=0 and x=lx=lx=l), this slope reaches its maximum magnitude, resulting in the standard formula.

📌 Key Points
  • ▸

    The slope is maximum at the supports and zero at the mid-span for a symmetric UDL.

  • ▸

    The units of slope are in radians (dimensionless).

  • ▸

    Flexural rigidity (EIEIEI) inversely affects both slope and deflection.

✅ Advantages
  • ▸

    Predictable deformation behavior

  • ▸

    Standardized coefficients for structural analysis

🛠️ Applications / Uses
  • ▸

    Design of floor beams

  • ▸

    Structural analysis of simply supported girders

📄 Additional Information
  • ▸

    Option A (Wl216EI\frac{Wl^2}{16EI}16EIWl2​) is incorrect; it relates to different boundary conditions.

  • ▸

    Option B (5wl4384EI\frac{5wl^4}{384EI}384EI5wl4​) represents the maximum central deflection, not the slope.

  • ▸

    Option D (Wl348EI\frac{Wl^3}{48EI}48EIWl3​) is the maximum deflection for a simply supported beam under a central point load WWW.

📊 Diagram / Illustration
Slope at Supports
θ=wl324EI\theta = (wl^3 / 24EI)θ=24EIwl3​
w: UDL intensity, l: Span, EI: Flexural Rigidity
✅

C is correct — The slope at the ends of a simply supported beam under UDL is determined by the formula wl324EI\frac{wl^3}{24EI}24EIwl3​.

Core Concepts Used
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Beam Theory Flexural Rigidity Boundary Conditions in Structural Mechanics
💡 EXAM TIP

Remember that 'slope' terms typically contain l3l^3l3 while 'deflection' terms contain l4l^4l4 for distributed loads; use this dimensional analysis to verify your formulas during the exam.

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