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Flashcards · 9702 · A Level Topic 12

Motion in a circle (A Level) flashcards

11 cards on A Level Topic 12, subtopics 12.1 to 12.2. Pick a subtopic or study them all.

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12.1 Kinematics of uniform circular motion

The radian
The angle subtended at the centre of a circle by an arc equal in length to the radius. Angle in radians = arc length ÷ radius.
Converting between degrees and radians
360° = 2π rad, so θ (rad) = θ (degrees) × π ÷ 180. 1 rad ≈ 57.3°.
Angular speed
The rate of change of angle swept out: ω = θ ÷ t = 2π ÷ T = 2πf. Unit rad s⁻¹.
Relationship between linear speed and angular speed
v = rω, with ω in rad s⁻¹.
A wheel of radius 0.30 m turns at 5.0 revolutions per second. Find ω and the rim speed.
ω = 2π × 5.0 = 31.4 rad s⁻¹. v = rω = 0.30 × 31.4 = 9.4 m s⁻¹.

12.2 Centripetal acceleration

Why is an object moving in a circle at constant speed accelerating?
Its direction keeps changing, so its velocity (a vector) changes even though its speed is constant.
Centripetal acceleration and force
a = v² ÷ r = rω². F = mv² ÷ r = mrω². Both are directed towards the centre of the circle.
Is centripetal force an extra force on a free-body diagram?
No. It is the resultant of the real forces acting, for example tension (ball on a string), friction (car on a flat bend) or gravity (planet in orbit).
Why does a centripetal force do no work?
It is perpendicular to the velocity at every instant, so there is no displacement along it. The kinetic energy stays constant.
Minimum speed at the top of a vertical circle (mass on a string)
At minimum speed the tension is zero and weight alone provides the centripetal force: mg = mv² ÷ r, so v = √(gr).
Tension at the top and bottom of a vertical circle
Top: T + mg = mv² ÷ r. Bottom: T − mg = mv² ÷ r. The tension is greatest at the bottom.