Rotational and Circular Motion

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Vocabulary flashcards covering rotational and circular motion, including angular displacement, angular velocity, angular acceleration, kinematic relationships, tangential and radial components, and centripetal acceleration.

Last updated 6:31 PM on 10/12/26
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18 Terms

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Angular Displacement (Δθ\Delta\theta)

The angle swept out by a reference line fixed to a rigid object as a particle travels from position A to position B in a time interval tt, given by Δθ=θf−θi\Delta\theta = \theta_f - \theta_i.

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Radian (rad\text{rad})

The SI unit of angular displacement, defined as the angle subtended at the center of a circle by an arc with a length equal to the radius of the circle, where 1 rad=360∘2π≈57.3∘1\,\text{rad} = \frac{360^\circ}{2\pi} \approx 57.3^\circ.

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Right Hand Rule (for Angular Displacement)

The rule specifying direction by holding the axis of rotation in the right hand with fingers curling in the direction of rotation; the thumb points in the direction of angular displacement.

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Angular Velocity (ω\omega)

The time rate of change of angular displacement of a body, defined by ω=ΔθΔt\omega = \frac{\Delta\theta}{\Delta t}, with the SI unit of radian per second (rad s−1\text{rad s}^{-1}).

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Average Angular Velocity (ωav\omega_{av})

The total angular displacement θ\theta of a body divided by the total time tt, given by ωav=θt\omega_{av} = \frac{\theta}{t}.

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Instantaneous Angular Velocity (ωinst\omega_{inst})

The limiting value of the ratio between small angular displacement Δθ\Delta\theta and small time interval Δt\Delta t as the time approaches zero: ωinst=lim⁡Δt→0ΔθΔt\omega_{inst} = \lim_{\Delta t \to 0} \frac{\Delta\theta}{\Delta t}.

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Angular Acceleration (α\alpha)

The time rate of change of angular velocity, given by α=ΔωΔt\alpha = \frac{\Delta\omega}{\Delta t}, with the SI unit of rad/s2\text{rad/s}^2.

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Average Angular Acceleration (αav\alpha_{av})

The total angular velocity ω\omega of a body divided by the total time tt, given by αav=ωt\alpha_{av} = \frac{\omega}{t}.

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Instantaneous Angular Acceleration (αinst\alpha_{inst})

The limiting value of the ratio between small change in angular velocity Δω\Delta\omega and small time interval Δt\Delta t as time approaches zero: αinst=lim⁡Δt→0ΔωΔt\alpha_{inst} = \lim_{\Delta t \to 0} \frac{\Delta\omega}{\Delta t}.

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Positive Angular Acceleration

The condition where the angular velocity of a body increases, causing angular velocity and angular acceleration to point in the same direction.

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Negative Angular Acceleration

The condition where the angular velocity of a body decreases, causing angular velocity and angular acceleration to be anti-parallel.

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Linear and Angular Displacement Relation

The geometric relationship connecting arc length (linear displacement SS) to radius rr and angular displacement θ\theta (in radians): S=rθS = r\theta.

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Tangential Velocity (vv)

The linear velocity directed along the tangent to the circular path, related to angular velocity by v=rωv = r\omega, or in vector form by vtangent=ω×r\mathbf{v}_{\text{tangent}} = \boldsymbol{\omega} \times \mathbf{r}.

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Tangential Component of Acceleration (aTa_T)

The component of acceleration parallel to linear instantaneous velocity that occurs due to a change in the magnitude of linear velocity, given by aT=rαa_T = r\alpha.

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Radial Component of Acceleration (aRa_R)

The component of acceleration along the radius of the circular path that arises due to a change in the direction of linear instantaneous velocity; also referred to as centripetal acceleration.

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Resultant Linear Acceleration Magnitude

The total magnitude of linear acceleration combining both tangential and radial components: a=aT2+aR2a = \sqrt{a_T^2 + a_R^2}.

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Centripetal Acceleration

The acceleration produced by the continuous change in direction of velocity of a particle moving in a circular path of radius rr at constant speed, directed towards the center of the circle.

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Uniform Circular Motion

Circular motion in which a particle travels at constant speed, where velocities at initial and final times differ only in direction while their magnitudes are equal: ∣vi∣=∣vf∣=v|v_i| = |v_f| = v.