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Motion in a Plane - Uniform Circular Motion

Grade 11CBSEPhysics

Review the key concepts, formulae, and examples before starting your quiz.

🔑Concepts

Uniform Circular Motion (UCM) is defined as the motion of an object traveling along a circular path at a constant speed. Although the speed is constant, the velocity is not, because the direction of motion changes continuously.

The angular displacement θ\theta is the angle subtended by the radius vector at the center of the circular path. It is measured in radians (radrad).

Angular velocity ω\omega is the rate of change of angular displacement. It is a vector quantity with the unit rad/srad/s.

The linear velocity vv of the particle is always tangential to the circular path at any given point.

In UCM, there is a constant acceleration acting towards the center of the circle called Centripetal Acceleration (aca_c). It is responsible for changing the direction of the velocity vector.

The time period TT is the time taken by the object to complete one revolution, while frequency ν\nu is the number of revolutions completed per unit time: ν=1T\nu = \frac{1}{T}.

📐Formulae

ω=dθdt=2πT=2πν\omega = \frac{d\theta}{dt} = \frac{2\pi}{T} = 2\pi\nu

v=rωv = r\omega

ac=v2r=ω2ra_c = \frac{v^2}{r} = \omega^2 r

ac=4π2ν2r=4π2rT2a_c = 4\pi^2 \nu^2 r = \frac{4\pi^2 r}{T^2}

ac=ω2r\vec{a}_c = -\omega^2 \vec{r}

💡Examples

Problem 1:

A stone tied to the end of a string 1.5 m1.5 \text{ m} long is whirled in a horizontal circle with a constant speed. If the stone makes 1010 revolutions in 20 s20 \text{ s}, calculate the magnitude of the centripetal acceleration.

Solution:

Given: Radius r=1.5 mr = 1.5 \text{ m}, Number of revolutions n=10n = 10, Time t=20 st = 20 \text{ s}. \n1. Calculate frequency: ν=nt=1020=0.5 Hz\nu = \frac{n}{t} = \frac{10}{20} = 0.5 \text{ Hz}. \n2. Calculate angular velocity: ω=2πν=2×π×0.5=π rad/s\omega = 2\pi\nu = 2 \times \pi \times 0.5 = \pi \text{ rad/s}. \n3. Calculate centripetal acceleration: ac=ω2r=(π)2×1.514.8 m/s2a_c = \omega^2 r = (\pi)^2 \times 1.5 \approx 14.8 \text{ m/s}^2.

Explanation:

The frequency is first determined to find the angular velocity. Since the speed is constant, we use the formula for centripetal acceleration involving ω\omega and rr.

Problem 2:

An aircraft executes a horizontal loop of radius 1 km1 \text{ km} with a steady speed of 900 km/h900 \text{ km/h}. Compare its centripetal acceleration with the acceleration due to gravity g=9.8 m/s2g = 9.8 \text{ m/s}^2.

Solution:

Given: r=1000 mr = 1000 \text{ m}, v=900 km/h=900×518=250 m/sv = 900 \text{ km/h} = 900 \times \frac{5}{18} = 250 \text{ m/s}. \n1. Centripetal acceleration: ac=v2r=25021000=625001000=62.5 m/s2a_c = \frac{v^2}{r} = \frac{250^2}{1000} = \frac{62500}{1000} = 62.5 \text{ m/s}^2. \n2. Ratio: acg=62.59.86.38\frac{a_c}{g} = \frac{62.5}{9.8} \approx 6.38.

Explanation:

The acceleration of the aircraft is approximately 6.386.38 times the acceleration due to gravity, highlighting the high 'g-force' experienced during such maneuvers.

Uniform Circular Motion - Revision Notes & Key Formulas | CBSE Class 11 Physics