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CivilStructural Mechanics-II
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A cantilever beam of span l, carrying udl of w on entire span, slope at free end will be

A

Wl33EI\frac{Wl┬│}{3EI}3EIWl3тАЛ

B

Wl22EI\frac{Wl┬▓}{2EI}2EIWl2тАЛ

C

wl36EI\frac{wl┬│}{6EI}6EIwl3тАЛ

D

wl48EI\frac{wlтБ┤}{8EI}8EIwl4тАЛ

Correct Answer

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

wl36EI\frac{wl┬│}{6EI}6EIwl3тАЛ

Quick Summary:

For a cantilever beam of span lll subjected to a uniformly distributed load (UDL) of intensity www per unit length, the slope at the free end is determined by integrating the bending moment equation Mx=тИТw(lтИТx)22M_x = -\frac{w(l-x)^2}{2}MxтАЛ=тИТ2w(lтИТx)2тАЛ. The resulting expression for the slope ╬╕\theta╬╕ at the free end (x=0x=0x=0) is ╬╕=wl36EI\theta = \frac{wl┬│}{6EI}╬╕=6EIwl3тАЛ.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

For a cantilever beam of span lll subjected to a uniformly distributed load (UDL) of intensity www per unit length, the slope at the free end is determined by integrating the bending moment equation Mx=тИТw(lтИТx)22M_x = -\frac{w(l-x)^2}{2}MxтАЛ=тИТ2w(lтИТx)2тАЛ. The resulting expression for the slope ╬╕\theta╬╕ at the free end (x=0x=0x=0) is ╬╕=wl36EI\theta = \frac{wl┬│}{6EI}╬╕=6EIwl3тАЛ.

ЁЯФв Key Formulas

╬╕=wl36EI\theta = \frac{wl┬│}{6EI}╬╕=6EIwl3тАЛ тАФ Slope at the free end of a cantilever with UDL

╬┤=wl48EI\delta = \frac{wlтБ┤}{8EI}╬┤=8EIwl4тАЛ тАФ Deflection at the free end of a cantilever with UDL

тЪЩя╕П Working Principle

The slope is found by integrating the MEI\frac{M}{EI}EIMтАЛ diagram over the length of the beam. Since M(x)=тИТw(lтИТx)22M(x) = -\frac{w(l-x)^2}{2}M(x)=тИТ2w(lтИТx)2тАЛ, the rotation ╬╕\theta╬╕ at the free end is тИл0lMEIdx=тИл0lw(lтИТx)22EIdx\int_{0}^{l} \frac{M}{EI} dx = \int_{0}^{l} \frac{w(l-x)^2}{2EI} dxтИл0lтАЛEIMтАЛdx=тИл0lтАЛ2EIw(lтИТx)2тАЛdx. Performing this definite integral yields w2EI[(lтИТx)3тИТ3]0l=w2EI[0тИТ(тИТl33)]=wl36EI\frac{w}{2EI} [\frac{(l-x)^3}{-3}]_0^l = \frac{w}{2EI} [0 - (-\frac{l┬│}{3})] = \frac{wl┬│}{6EI}2EIwтАЛ[тИТ3(lтИТx)3тАЛ]0lтАЛ=2EIwтАЛ[0тИТ(тИТ3l3тАЛ)]=6EIwl3тАЛ.

ЁЯУМ Key Points
  • тЦ╕

    The slope at the fixed end of a cantilever beam is always zero.

  • тЦ╕

    The maximum slope and maximum deflection for a cantilever with UDL occur at the free end.

  • тЦ╕

    Flexural rigidity (EIEIEI) represents the beam's resistance to bending; higher values result in lower slopes and deflections.

тЬЕ Advantages
  • тЦ╕

    Simple analytical calculation for standard loading cases

  • тЦ╕

    Applicable to structural design of overhangs and cantilevers

тЭМ Disadvantages / Limitations
  • тЦ╕

    Does not account for shear deformation (usually neglected in Euler-Bernoulli beam theory)

  • тЦ╕

    Assumes linear elastic material behavior

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Structural analysis of balcony projections

  • тЦ╕

    Design of cantilever retaining walls and canopy structures

ЁЯУД Additional Information
  • тЦ╕

    Option A (Wl33EI\frac{Wl┬│}{3EI}3EIWl3тАЛ) is the deflection at the free end for a point load WWW at the free end.

  • тЦ╕

    Option B (Wl22EI\frac{Wl┬▓}{2EI}2EIWl2тАЛ) is the slope at the free end for a point load WWW at the free end.

  • тЦ╕

    Option D (wl48EI\frac{wlтБ┤}{8EI}8EIwl4тАЛ) is the deflection at the free end for a cantilever with UDL www.

ЁЯУК Diagram / Illustration
Cantilever Beam: Slope (╬╕\theta╬╕)
╬╕=wl36EI\theta = (wl^3 / 6EI)╬╕=6EIwl3тАЛ
www : UDL intensity (N/m)
lll : Span length
EIEIEI : Flexural Rigidity
тЬЕ

C is correct тАФ The slope at the free end of a cantilever beam carrying a UDL of www over its entire length is wl36EI\frac{wl┬│}{6EI}6EIwl3тАЛ.

Core Concepts Used
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Euler-Bernoulli Beam Theory Slope and Deflection Integration of Bending Moment Equation
ЁЯТб EXAM TIP

Remember the mnemonic 'Slope is 1 degree less than deflection' (╬╕тИЭl3\theta \propto l┬│╬╕тИЭl3 and ╬┤тИЭl4\delta \propto lтБ┤╬┤тИЭl4) for standard cantilever cases.

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