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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┬▓}{16EI}16EIWl2тАЛ

B

5wl4384EI\frac{5wlтБ┤}{384EI}384EI5wl4тАЛ

C

wl324EI\frac{wl┬│}{24EI}24EIwl3тАЛ

D

Wl348EI\frac{Wl┬│}{48EI}48EIWl3тАЛ

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleCivilStructural Mechanics-II
Option C

wl324EI\frac{wl┬│}{24EI}24EIwl3тАЛ

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 ╬╕=wl324EI\theta = \frac{wl┬│}{24EI}╬╕=24EIwl3тАЛ, where EEE is Young's Modulus and III is the Moment of Inertia.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб 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 ╬╕=wl324EI\theta = \frac{wl┬│}{24EI}╬╕=24EIwl3тАЛ, where EEE is Young's Modulus and III is the Moment of Inertia.

ЁЯФв Key Formulas

╬╕=wl324EI\theta = \frac{wl┬│}{24EI}╬╕=24EIwl3тАЛ тАФ Slope at the ends of a simply supported beam with UDL

╬┤max=5wl4384EI\delta_{max} = \frac{5wlтБ┤}{384EI}╬┤maxтАЛ=384EI5wl4тАЛ тАФ Maximum deflection at the center of a simply supported beam with UDL

тЪЩя╕П 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┬▓} = M_xEIdx2d2yтАЛ=MxтАЛ. 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}dxdyтАЛ. At the supports (x=0x=0x=0 and x=lx=lx=l), this slope reaches its maximum magnitude, resulting in the standard formula.

ЁЯУМ Key Points
  • тЦ╕

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

  • тЦ╕

    The units of slope are in radians (dimensionless).

  • тЦ╕

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

тЬЕ Advantages
  • тЦ╕

    Predictable deformation behavior

  • тЦ╕

    Standardized coefficients for structural analysis

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Design of floor beams

  • тЦ╕

    Structural analysis of simply supported girders

ЁЯУД Additional Information
  • тЦ╕

    Option A (Wl216EI\frac{Wl┬▓}{16EI}16EIWl2тАЛ) is incorrect; it relates to different boundary conditions.

  • тЦ╕

    Option B (5wl4384EI\frac{5wlтБ┤}{384EI}384EI5wl4тАЛ) represents the maximum central deflection, not the slope.

  • тЦ╕

    Option D (Wl348EI\frac{Wl┬│}{48EI}48EIWl3тАЛ) is the maximum deflection for a simply supported beam under a central point load WWW.

ЁЯУК Diagram / Illustration
Slope at Supports
╬╕=wl324EI\theta = (wl^3 / 24EI)╬╕=24EIwl3тАЛ
w: UDL intensity, l: Span, EI: FlexuralRigidity
тЬЕ

C is correct тАФ The slope at the ends of a simply supported beam under UDL is determined by the formula wl324EI\frac{wl┬│}{24EI}24EIwl3тАЛ.

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

Remember that 'slope' terms typically contain l3l┬│l3 while 'deflection' terms contain l4lтБ┤l4 for distributed loads; use this dimensional analysis to verify your formulas during the exam.

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