Question:

A car is moving in a circular horizontal track of radius 10 m with a constant speed of 10 m/s-1. A bob is suspended from the roof of the car by a light wire of length 1.0 m. The angle made by the wire with the vertical is (in radian)

Updated On: Apr 1, 2025
  • 0
  • π/6
  • π/3
  • π/4
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The Correct Option is D

Approach Solution - 1

Forces on the bob:

  • The tension force \( T \) acts towards the center of the circle.
  • The gravitational force \( mg \) acts vertically downward.

Since the bob is moving with constant speed, the bob is in equilibrium, and the net force acting on it must be zero. Now, we consider the forces in both directions:

For the vertical direction:

\(T \cos(\theta) - mg = 0\)

For the horizontal direction:

\( T \sin(\theta) = \frac{mv^2}{r} \)

From the vertical direction equation:

\( T \cos(\theta) = mg \quad \Rightarrow \quad T = \frac{mg}{\cos(\theta)} \)

Substitute this value of \( T \) into the horizontal direction equation:

\[ \frac{mg}{\cos(\theta)} \cdot \sin(\theta) = \frac{mv^2}{r} \]

Simplifying:

\[ \tan(\theta) = \frac{v^2}{rg} \]

Given values:

  • Speed \( v = 10 \, \text{m/s} \)
  • Radius \( r = 10 \, \text{m} \)
  • Gravitational acceleration \( g = 10 \, \text{m/s}^2 \)

Substitute these values into the equation:

\[ \tan(\theta) = \frac{10^2}{10 \times 10} = 1 \]

Now, to find the angle \( \theta \), we take the inverse tangent (arctan) of both sides:

\[ \theta = \arctan(1) = \frac{\pi}{4} \]

Therefore, the angle made by the wire with the vertical is: \( \frac{\pi}{4} \) radians (option D).

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Approach Solution -2

Let \( \theta \) be the angle made by the wire with the vertical.

We know that: 

\( \tan \theta = \frac{v^2}{r g} \)

Given: \( v = 10 \, \text{m/s} \), \( r = 10 \, \text{m} \), and \( g = 10 \, \text{m/s}^2 \), we substitute these values into the equation:

\( \tan \theta = \frac{(10 \, \text{m/s})^2}{10 \, \text{m} \times 10 \, \text{m/s}^2} = 1 \)

Now, solving for \( \theta \):

\( \theta = \tan^{-1}(1) = \frac{\pi}{4} \)

Therefore, the angle \( \theta \) is: \( \frac{\pi}{4} \).

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Top Questions on Uniform Circular Motion

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Concepts Used:

Uniform Circular Motion

A circular motion is defined as the movement of a body that follows a circular route. The motion of a body going at a constant speed along a circular path is known as uniform circular motion. The velocity varies while the speed of the body in uniform circular motion remains constant.

Uniform Circular Motion Examples:

  • The motion of electrons around its nucleus.
  • The motion of blades of the windmills.

Uniform Circular Motion Formula:

When the radius of the circular path is R, and the magnitude of the velocity of the object is V. Then, the radial acceleration of the object is:

arad = v2/R

Similarly, this radial acceleration is always perpendicular to the velocity direction. Its SI unit is m2s−2.

The radial acceleration can be mathematically written using the period of the motion i.e. T. This period T is the volume of time taken to complete a revolution. Its unit is measurable in seconds.

When angular velocity changes in a unit of time, it is a radial acceleration.

Angular acceleration indicates the time rate of change of angular velocity and is usually denoted by α and is expressed in radians per second. Moreover, the angular acceleration is constant and does not depend on the time variable as it varies linearly with time. Angular Acceleration is also called Rotational Acceleration.

Angular acceleration is a vector quantity, meaning it has magnitude and direction. The direction of angular acceleration is perpendicular to the plane of rotation.

Formula Of Angular Acceleration

The formula of angular acceleration can be given in three different ways.

α = dωdt

Where,

ω → Angular speed

t → Time

α = d2θdt2

Where,

θ → Angle of rotation

t → Time

Average angular acceleration can be calculated by the formula below. This formula comes in handy when angular acceleration is not constant and changes with time.

αavg = ω2 - ω1t2 - t1

Where,

ω1 → Initial angular speed

ω2 → Final angular speed

t1 → Starting time

t2 → Ending time

Also Read: Angular Motion