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CivilStructural Mechanics-II
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A cantilever beam with point load at free end and udl on entire span, slope will be

A

Wl216EI+wl324EI\frac{Wl┬▓}{16EI} + \frac{wl┬│}{24EI}16EIWl2тАЛ+24EIwl3тАЛ

B

Wl33EI+wl48EI\frac{Wl┬│}{3EI} + \frac{wlтБ┤}{8EI}3EIWl3тАЛ+8EIwl4тАЛ

C

Wl22EI+wl36EI\frac{Wl┬▓}{2EI} + \frac{wl┬│}{6EI}2EIWl2тАЛ+6EIwl3тАЛ

D

Wl348EI+5wl4384EI\frac{Wl┬│}{48EI} + \frac{5wlтБ┤}{384EI}48EIWl3тАЛ+384EI5wl4тАЛ

Correct Answer

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

Wl22EI+wl36EI\frac{Wl┬▓}{2EI} + \frac{wl┬│}{6EI}2EIWl2тАЛ+6EIwl3тАЛ

Quick Summary:

The slope of a cantilever beam at the free end is determined by the principle of superposition, where the total slope is the sum of the slope due to a point load at the free end and the slope due to a uniformly distributed load (UDL) on the entire span. For a point load W, the slope at the free end is Wl22EI\frac{Wl┬▓}{2EI}2EIWl2тАЛ, and for a UDL of intensity w, it is wl36EI\frac{wl┬│}{6EI}6EIwl3тАЛ.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The slope of a cantilever beam at the free end is determined by the principle of superposition, where the total slope is the sum of the slope due to a point load at the free end and the slope due to a uniformly distributed load (UDL) on the entire span. For a point load W, the slope at the free end is Wl22EI\frac{Wl┬▓}{2EI}2EIWl2тАЛ, and for a UDL of intensity w, it is wl36EI\frac{wl┬│}{6EI}6EIwl3тАЛ.

ЁЯФв Key Formulas

╬╕P=Wl22EI\theta_P = \frac{Wl┬▓}{2EI}╬╕PтАЛ=2EIWl2тАЛ тАФ Slope due to point load

╬╕u=wl36EI\theta_u = \frac{wl┬│}{6EI}╬╕uтАЛ=6EIwl3тАЛ тАФ Slope due to UDL

тЪЩя╕П Working Principle

According to the Euler-Bernoulli beam theory, the slope ╬╕\theta╬╕ is the integral of the curvature M(x)EI\frac{M(x)}{EI}EIM(x)тАЛ. By evaluating the moment equations for a point load MP=W(lтИТx)M_P = W(l-x)MPтАЛ=W(lтИТx) and a UDL Mu=w(lтИТx)22M_u = \frac{w(l-x)^2}{2}MuтАЛ=2w(lтИТx)2тАЛ, and integrating over the beam length, the superposition of these individual slopes results in the total rotation at the free end.

ЁЯУМ Key Points
  • тЦ╕

    Superposition applies because the structure behaves linearly elastically.

  • тЦ╕

    The slope is measured relative to the fixed end (where slope is zero).

  • тЦ╕

    Both loadings produce maximum slope at the free end of the cantilever.

тЬЕ Advantages
  • тЦ╕

    Simplifies complex problems into solvable elementary components.

  • тЦ╕

    Provides a direct analytical result for standard load cases.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Applicable only within the linear elastic limit of the material.

  • тЦ╕

    Assumes small deflection theory.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Design of cantilever brackets and overhang beams.

  • тЦ╕

    Verification of structural software simulations.

ЁЯУД Additional Information
  • тЦ╕

    Option B represents the deflection (not slope) at the free end.

  • тЦ╕

    Option D relates to a simply supported beam with UDL, where the coefficient 5/384 is used for deflection.

  • тЦ╕

    Ensure consistent units for load (N or kN), length (m or mm), and flexural rigidity (EI).

ЁЯУК Diagram / Illustration
Total Slope (╬╕) at Free End
Wl22EI+wl36EI(Wl^2 / 2EI) + (wl^3 / 6EI)2EIWl2тАЛ+6EIwl3тАЛ
= ╬╕тВЪ + ╬╕с╡д
тЬЕ

C is correct тАФ The total slope at the free end is the summation of the individual slopes caused by the point load and the UDL, defined as Wl22EI+wl36EI\frac{Wl┬▓}{2EI} + \frac{wl┬│}{6EI}2EIWl2тАЛ+6EIwl3тАЛ.

Core Concepts Used
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Euler-Bernoulli Beam Theory Principle of Superposition Slope and Deflection of Cantilever Beams
ЁЯТб EXAM TIP

Always distinguish between slope (╬╕)\theta)╬╕)and deflection (╬┤).\delta).╬┤).Slopes involve l2l┬▓l2 and l3l┬│l3, whereas deflections involve l3l┬│l3 and l4lтБ┤l4 for point and UDL respectively.

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