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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Newton's Laws of Motion

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Newton's Laws of Motion

A car accelerates on a horizontal road with an acceleration a . Two...

A car accelerates on a horizontal road with an acceleration aa. Two situations are considered inside the car. First, a ball is suspended from the ceiling by a string and maintains a constant angle with the vertical. Second, a block is placed on a smooth incline and does not slip on the incline. Determine the angle of the string with the vertical, and the angle of the incline with the horizontal.

Options

  1. Atan⁡−1(ag)\tan^{-1} \left(\dfrac{a}{g}\right)and sin⁡−1(ag)\sin^{-1} \left(\dfrac{a}{g}\right)
  2. Btan⁡−1(ga)\tan^{-1} \left(\dfrac{g}{a}\right)and tan⁡−1(ga)\tan^{-1} \left(\dfrac{g}{a}\right)
  3. Ctan⁡−1(ag)\tan^{-1} \left(\dfrac{a}{g}\right)and tan⁡−1(ag)\tan^{-1} \left(\dfrac{a}{g}\right)
  4. Dsin⁡−1(ag)\sin^{-1} \left(\dfrac{a}{g}\right)and tan⁡−1(ag)\tan^{-1} \left(\dfrac{a}{g}\right)

Correct answer

C. tan⁡−1(ag)\tan^{-1} \left(\dfrac{a}{g}\right)and tan⁡−1(ag)\tan^{-1} \left(\dfrac{a}{g}\right)

Step-by-step solution

In the frame of the accelerating car, a pseudo force mama acts on the objects in the direction opposite to the acceleration.

For the suspended ball, the forces acting are tension TT, weight mgmg, and pseudo force mama.

Resolving forces along the horizontal and vertical directions for equilibrium:

Tsin⁡θ=maT \sin \theta = ma

Tcos⁡θ=mgT \cos \theta = mg

Dividing the two equations, we get tan⁡θ=ag⇒θ=tan⁡−1(ag).<br><br>Fortheblockonthesmoothincline,theforcesactingarenormalreaction\tan \theta = \dfrac{a}{g} \Rightarrow \theta = \tan^{-1} \left(\dfrac{a}{g}\right).<br><br>For the block on the smooth incline, the forces acting are normal reactionN,weight, weightmg,andpseudoforce, and pseudo forcema.<br><br>Fortheblocktonotslip,thenetforcealongtheinclinemustbezero.<br><br>Thecomponentofgravitydowntheinclineis.<br><br>For the block to not slip, the net force along the incline must be zero.<br><br>The component of gravity down the incline ismg \sin αandthecomponentofthepseudoforceuptheinclineis\alpha and the component of the pseudo force up the incline isma \cos α.<br><br>Equatingthesecomponents:<br><br>\alpha.<br><br>Equating these components:<br><br>mg \sin α=\alpha =ma \cos α<br><br>\alpha<br><br>\tan α=ag⇒α=tan⁡−1(ag).<br><br>Bothanglesare\alpha = \dfrac{a}{g} \Rightarrow \alpha = \tan^{-1} \left(\dfrac{a}{g}\right).<br><br>Both angles are\tan^{-1} \left(\dfrac{a}{g}\right).
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