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CivilStructural Mechanics-II
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A cantilever beam of span l, carrying point load W at free end, deflection 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 A

Wl33EI\frac{Wl┬│}{3EI}3EIWl3тАЛ

Quick Summary:

For a cantilever beam of length lll subjected to a point load WWW at its free end, the maximum deflection occurs at the free end. This deflection is derived using the double integration method or the moment-area method as ╬┤max=Wl33EI\delta_{max} = \frac{Wl┬│}{3EI}╬┤maxтАЛ=3EIWl3тАЛ.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

For a cantilever beam of length lll subjected to a point load WWW at its free end, the maximum deflection occurs at the free end. This deflection is derived using the double integration method or the moment-area method as ╬┤max=Wl33EI\delta_{max} = \frac{Wl┬│}{3EI}╬┤maxтАЛ=3EIWl3тАЛ.

ЁЯФв Key Formulas

╬┤=Wl33EI\delta = \frac{Wl┬│}{3EI}╬┤=3EIWl3тАЛ тАФ Deflection at free end of a cantilever with point load

╬╕=Wl22EI\theta = \frac{Wl┬▓}{2EI}╬╕=2EIWl2тАЛ тАФ Slope at free end of a cantilever with point load

тЪЩя╕П Working Principle

The deflection is caused by the bending moment induced throughout the beam length. Since the bending moment MxM_xMxтАЛ at a distance xxx from the free end is WxWxWx, integrating the differential equation of the elastic curve EId2ydx2=MxEI \frac{d^2y}{dx┬▓} = M_xEIdx2d2yтАЛ=MxтАЛ with boundary conditions of zero slope and zero deflection at the fixed support yields the cubic variation of deflection.

ЁЯУМ Key Points
  • тЦ╕

    Maximum deflection always occurs at the free end of a cantilever beam.

  • тЦ╕

    The deflection is directly proportional to the load WWW and the cube of the length lll.

  • тЦ╕

    The product EIEIEI is known as the flexural rigidity of the beam.

  • тЦ╕

    The slope at the free end is ╬╕=Wl22EI\theta = \frac{Wl┬▓}{2EI}╬╕=2EIWl2тАЛ.

тЬЕ Advantages
  • тЦ╕

    Simple linear relationship with load

  • тЦ╕

    Easy to compute for standard load cases

тЭМ Disadvantages / Limitations
  • тЦ╕

    Limited to small deflection theory

  • тЦ╕

    Assumes linear elastic material behavior

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Design of cantilever balconies

  • тЦ╕

    Structural analysis of aircraft wings

  • тЦ╕

    Mechanical spring and cantilever sensor design

ЁЯУД Additional Information
  • тЦ╕

    Option B represents the slope at the free end, not the deflection.

  • тЦ╕

    Option C (wl3/6EIwl┬│/6EIwl3/6EI) is incorrect as it does not match standard cantilever deflection formulas.

  • тЦ╕

    Option D (wl4/8EIwlтБ┤/8EIwl4/8EI) represents the maximum deflection of a cantilever under a Uniformly Distributed Load (UDL).

ЁЯУК Diagram / Illustration
Cantilever Deflection Formula
Wl3W l^3Wl3
3EI3 E I3EI
╬┤max=Deflection┬аat┬аfree┬аend\delta_{max} = \text{Deflection at free end}╬┤maxтАЛ=Deflection┬аat┬аfree┬аend
тЬЕ

A is correct тАФ The deflection at the free end of a cantilever beam with a point load WWW is Wl33EI\frac{Wl┬│}{3EI}3EIWl3тАЛ.

Core Concepts Used
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Flexural Rigidity ($EI$) Elastic Curve Equation Cantilever Boundary Conditions
ЁЯТб EXAM TIP

Always verify if the question asks for deflection (unit of length) or slope (dimensionless/radians) to avoid choosing the wrong formula.

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