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Impulse and Momentum question

2021 · Shift 2 · Q39
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Impulse and Momentum question

2021 · Shift 2 · Q39

JEE AdvancedPhysicsImpulse and MomentumMultiple correct+4 / −2
One end of a horizontal uniform beam of weight W and length L is hinged on a vertical wall at point O and its other end is supported by a light inextensible rope. The other end of the rope is fixed at point Q, at a height L above the hinge at point O. A block of weight α\alphaα W is attached at the point P of the beam, as shown in the figure (not to scale). The rope can sustain a maximum tension of (2 2\sqrt 22​)W. Which of the following statement(s) is(are) correct? JEE Advanced 2021 Paper 2 Online Physics - Impulse & Momentum Question 11 English
  1. A
    The vertical component of reaction force at O does not depend on α\alphaα
  2. B
    The horizontal component of reaction force at O is equal to W for α\alphaα = 0.5
  3. C
    The tension in the rope is 2W for α\alphaα = 0.5
  4. D
    The rope breaks if α\alphaα > 1.5
View written solutionFree

Correct answer: A, B, D

  1. Set up the geometry

The beam is horizontal, hinged at OOO, and has length LLL.

The rope joins the free end of the beam to point QQQ, which is at height LLL above OOO. So the rope makes a 45∘45^\circ45∘ angle with the horizontal.

Hence, if the rope tension is TTT, then its components at the beam end are: Tx=−T2,Ty=T2T_x = -\frac{T}{\sqrt{2}}, \qquad T_y = \frac{T}{\sqrt{2}}Tx​=−2​T​,Ty​=2​T​ (leftward and upward respectively).

The beam has weight WWW acting at its center, i.e. at distance L/2L/2L/2 from OOO. A block of weight αW\alpha WαW is attached at the end point PPP of the beam (as implied by the figure/text), i.e. at distance LLL from OOO.

Let hinge reaction at OOO have components Rx,RyR_x, R_yRx​,Ry​.


  1. Torque equilibrium about hinge OOO

Taking anticlockwise torque as positive:

  • Upward component of tension at beam end gives torque: T2⋅L\frac{T}{\sqrt{2}}\cdot L2​T​⋅L
  • Weight of beam gives clockwise torque: W⋅L2W\cdot \frac{L}{2}W⋅2L​
  • Weight of block gives clockwise torque: αW⋅L\alpha W\cdot LαW⋅L

Equilibrium gives T2L−WL2−αWL=0\frac{T}{\sqrt{2}}L - W\frac{L}{2} - \alpha WL = 02​T​L−W2L​−αWL=0

Cancel LLL: T2=(α+12)W\frac{T}{\sqrt{2}} = \left(\alpha + \frac12\right)W2​T​=(α+21​)W

So T=2(α+12)WT = \sqrt{2}\left(\alpha + \frac12\right)WT=2​(α+21​)W


  1. Force equilibrium in vertical direction

Ry+T2−W−αW=0R_y + \frac{T}{\sqrt{2}} - W - \alpha W = 0Ry​+2​T​−W−αW=0

Substitute T2=(α+12)W\frac{T}{\sqrt{2}} = \left(\alpha + \frac12\right)W2​T​=(α+21​)W

Then Ry+(α+12)W−(1+α)W=0R_y + \left(\alpha + \frac12\right)W - (1+\alpha)W = 0Ry​+(α+21​)W−(1+α)W=0 Ry−W2=0R_y - \frac{W}{2} = 0Ry​−2W​=0 Ry=W2R_y = \frac{W}{2}Ry​=2W​

So the vertical reaction is independent of α\alphaα.

Hence A is correct.


  1. Force equilibrium in horizontal direction

Only two horizontal forces act:

  • hinge reaction RxR_xRx​ to the right,
  • rope component T/2T/\sqrt{2}T/2​ to the left.

Thus Rx=T2=(α+12)WR_x = \frac{T}{\sqrt{2}} = \left(\alpha + \frac12\right)WRx​=2​T​=(α+21​)W

For α=0.5\alpha = 0.5α=0.5, Rx=(0.5+0.5)W=WR_x = \left(0.5 + 0.5\right)W = WRx​=(0.5+0.5)W=W

Hence B is correct.


  1. Check tension for α=0.5\alpha = 0.5α=0.5

Using T=2(α+12)WT = \sqrt{2}\left(\alpha + \frac12\right)WT=2​(α+21​)W

For α=0.5\alpha=0.5α=0.5, T=2(1)W=2WT = \sqrt{2}(1)W = \sqrt{2}WT=2​(1)W=2​W

This is not equal to 2W2W2W.

Hence C is incorrect.


  1. Condition for rope to break

Maximum sustainable tension: Tmax⁡=22 WT_{\max} = 2\sqrt{2}\,WTmax​=22​W

The rope breaks when T>22WT > 2\sqrt{2}WT>22​W

Using T=2(α+12)WT = \sqrt{2}\left(\alpha + \frac12\right)WT=2​(α+21​)W

So 2(α+12)W>22W\sqrt{2}\left(\alpha + \frac12\right)W > 2\sqrt{2}W2​(α+21​)W>22​W

Cancel 2W\sqrt{2}W2​W: α+12>2\alpha + \frac12 > 2α+21​>2 α>32\alpha > \frac32α>23​

Thus the rope breaks if α>1.5\alpha > 1.5α>1.5

Hence D is correct.


  1. Final answer

Correct statements are: A, B, D\boxed{A,\ B,\ D}A, B, D​

This matches the stored correct answer.

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