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Animated Solution for Physics - Kinematics: Which of the following statements is false for a particle moving in a circle with a constant angular speed?

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Visualized Solution

\text{Uniform Circular Motion}

  • \text{Particle moving in a circle with constant angular speed } \omega.

\text{Velocity Vector}

  • \text{Velocity } \mathbf{v} \text{ is always tangential to the path.}

\text{Acceleration in UCM}

  • \text{Since } \omega \text{ is constant, tangential acceleration } a_t = 0.

\text{Centripetal Acceleration}

  • \text{Only centripetal acceleration } \mathbf{a}_c \text{ exists, pointing towards the center.}

\text{Relationship between } \mathbf{v} \text{ and } \mathbf{a}

  • \mathbf{v} \perp \mathbf{a}_c \text{ at all times.}

\text{Evaluating Options}

  • \text{Option (b) says acceleration is tangent, which is FALSE.}

\text{Non-Uniform Circular Motion}

  • \text{If } \omega \text{ varies, } \mathbf{a} = \mathbf{a}_c + \mathbf{a}_t \text{ (not purely radial).}

The Sigma Insight: Kinematics of Circular Motion

Solution Diagram

The Anatomy of Uniform Circular Motion

Imagine a particle whizzing around a circular track. The problem gives us a crucial piece of information: the particle is moving with a constant angular speed (). This specific scenario is known as Uniform Circular Motion (UCM). Let's break down the physical vectors involved in this motion to find which statement is false.

The Velocity Vector

Always on the Edge
By the fundamental definition of kinematics, the instantaneous velocity vector of any moving particle is always directed along the tangent to its path at that specific point.
Whether the particle is speeding up, slowing down, or maintaining a constant speed, its velocity vector will always graze the edge of the circle. Therefore, the statement "The velocity vector is tangent to the circle" is absolutely true.

The Acceleration Vector

The Center-Seeking Force
Now, let's analyze the acceleration. Acceleration is the rate of change of velocity. Since velocity is a vector, it can change in two ways: a change in magnitude (speed) or a change in direction.
Because our particle has a constant angular speed, its linear speed is also constant. This means there is zero tangential acceleration (). There is no force pulling the particle forward or pushing it backward along the track.
However, the direction of the velocity is continuously changing as the particle navigates the curve. This continuous change in direction requires an acceleration. This is the centripetal acceleration (), and it is always directed radially inward, pointing straight towards the center of the circle.
Therefore, the statement "The acceleration vector points to the centre of the circle" is true.

The Geometric Relationship

Let's look at the geometry of our two vectors. At any given point on the circle, the velocity vector lies along the tangent line, and the acceleration vector lies along the radial line.
From basic geometry, we know that a tangent to a circle is always perpendicular to the radius at the point of tangency. Consequently, the velocity vector and the centripetal acceleration vector must be perpendicular to each other.
This makes the statement "The velocity and acceleration vectors are perpendicular to each other" true.

The False Claim

We are left with option (b): "The acceleration vector is tangent to the circle." As we just established, in uniform circular motion, the only acceleration present is the centripetal acceleration, which is purely radial. There is no tangential component.
Thus, claiming the acceleration vector is tangent to the circle is a fundamental misunderstanding of uniform circular motion. This is our false statement.

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