Rotational Motion, Equilibrium, and Dynamics Flashcards

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Vocabulary flashcards covering key definitions, equations, and principles of rotational motion, rotational equilibrium, and dynamics.

Last updated 2:26 PM on 10/5/26
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23 Terms

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Center of Gravity

The single point in a rigid body where the single equivalent force of all individual gravitational forces acting on its particles is located, calculated using coordinates xcg=∑mixi∑mix_{cg} = \frac{\sum m_i x_i}{\sum m_i} and ycg=∑miyi∑miy_{cg} = \frac{\sum m_i y_i}{\sum m_i}.

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Plumb Line Method

An experimental method used to determine the center of gravity of an object, where the center of gravity always coincides with a vertical line extended from a suspended string.

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Torque (τ\tau)

A quantitative measure of the tendency of a force to cause or change a body's rotational motion (SI unit:N⋅mSI\,unit: N \cdot m), calculated as τ=rF⊥\tau = r F_{\perp}, where positive torque causes counterclockwise rotation and negative torque causes clockwise rotation.

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Lever Arm (r⊥r_{\perp})

The perpendicular distance from the rotational axis to the line of action of an applied force, used to calculate torque via τ=r⊥F\tau = r_{\perp} F.

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Static Equilibrium of a Rigid Body

The state of a rigid body in which both the net external force is zero (∑F=0\sum F = 0) and the net external torque about any axis is zero (∑τ=0\sum \tau = 0).

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Moment of Inertia (II)

A measure of an object's resistance against changes in its rotational motion (SI unit:kg⋅m2SI\,unit: kg \cdot m^2), defined as I=mr2I = m r^2 for a point mass or I=∑miri2I = \sum m_i r_i^2 for a system of particles.

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Newton's Second Law for Rotational Motion

The law stating that when a net external torque ∑τ\sum \tau acts on a rigid body with moment of inertia II, it produces an angular acceleration α\alpha given by ∑τ=Iα\sum \tau = I \alpha.

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Rotational Kinetic Energy (KErKE_r)

The kinetic energy possessed by an object rotating with angular speed ω\omega, expressed as KEr=12Iω2KE_r = \frac{1}{2} I \omega^2.

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Total Kinetic Energy of Rolling Motion

The total kinetic energy acquired by a rolling object without slipping, given by the sum of its rotational kinetic energy and translational kinetic energy: KE=KEr+KEt=12Iω2+12mv2KE = KE_r + KE_t = \frac{1}{2} I \omega^2 + \frac{1}{2} m v^2.

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Rotational Work (WW)

The work done on a rigid body when it undergoes an angular displacement Δθ\Delta \theta due to an applied torque τ\tau, given by W=τΔθW = \tau \Delta \theta.

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Angular Momentum (LL)

The rotational analog of linear momentum (SI unit:kg⋅m2/sSI\,unit: kg \cdot m^2/s), calculated as the product of an object's moment of inertia II and its angular velocity ω\omega (L=IωL = I \omega).

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Law of Conservation of Angular Momentum

The principle stating that when a rigid body experiences no net external torque, its total angular momentum remains constant over time (Li=LfL_i = L_f).

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<p>Radian ($$rad$$)</p>

Radian (radrad)

The SI unit of angular measurement defined as the angle subtended at the center of a circle by an arc whose length ss equals the radius rr (s=rs = r), where 1 rev=2π rad=360∘1\,rev = 2\pi\,rad = 360^\circ.

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Angular Displacement (Δθ\Delta \theta)

The angle through which a body rotates from an initial angular position θo\theta_o to a final position θ\theta, defined as Δθ=θ−θo\Delta \theta = \theta - \theta_o and related to arc length by Δs=rΔθ\Delta s = r \Delta \theta.

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Angular Velocity (ω\omega)

The rate of change of angular displacement with respect to time (SI unit:rad/sSI\,unit: rad/s), with average angular velocity expressed as ωav=ΔθΔt\omega_{av} = \frac{\Delta \theta}{\Delta t}.

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Angular Acceleration (α\alpha)

The rate of change of angular velocity with respect to time (SI unit:rad/s2SI\,unit: rad/s^2), with average angular acceleration expressed as αav=ΔωΔt\alpha_{av} = \frac{\Delta \omega}{\Delta t}.

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Tangential Velocity (vtv_t)

The linear velocity of a point on a rotating body directed tangent to the circular path (SI unit:m/sSI\,unit: m/s), related to angular velocity by vt=rωv_t = r \omega.

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Tangential Acceleration (ata_t)

The linear acceleration of a point on a rotating body directed tangent to its circular path (SI unit:m/s2SI\,unit: m/s^2), caused by a change in tangential speed and calculated as at=rαa_t = r \alpha.

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Centripetal Acceleration (aca_c)

The acceleration directed toward the center of a circular path (SI unit:m/s2SI\,unit: m/s^2) caused by a continuous change in the direction of velocity, given by ac=v2r=ω2ra_c = \frac{v^2}{r} = \omega^2 r.

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<p>Uniform Circular Motion</p>

Uniform Circular Motion

A special case of circular motion in which an object moves in a circle at constant tangential speed, experiencing zero tangential acceleration (at=0a_t = 0) and non-zero centripetal acceleration (ac≠0a_c \neq 0).

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Centrifugal Force

An apparent outward fictitious force felt by an object moving in a circular path, arising from Newton's first law of motion as the body tends to maintain straight-line motion.

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Conical Pendulum

A pendulum consisting of a bob revolving in a horizontal circular path of radius rr at a string length LL, with a period given by Period=2πLcos⁡(θ)gPeriod = 2\pi \sqrt{\frac{L \cos(\theta)}{g}}.

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Banked Curve

A curve on a track or road tilted at an angle θ\theta so that a component of the normal force provides the centripetal force required to turn safely without relying entirely on friction, with optimal speed v=grtan⁡(θ)v = \sqrt{g r \tan(\theta)}.