Rotational Motion and Equilibrium Practice Flashcards

0.0(0)
Studied by 0 people
call kaiCall Kai
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/15

flashcard set

Earn XP

Description and Tags

A set of vocabulary flashcards covering key concepts of rotational motion, torque, moment of inertia, and static equilibrium based on physics exam problems.

Last updated 3:58 PM on 4/29/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai

No analytics yet

Send a link to your students to track their progress

16 Terms

1
New cards

Torque (τ\tau)

The product of the force and the lever arm, calculated as τ=F×r×sin(θ)\tau = F \times r \times \sin(\theta), measured in units of NmN \cdot m.

2
New cards

Lever arm

The perpendicular distance from the axis of rotation to the line of action of the force, given by the expression rsin(θ)r \sin(\theta).

3
New cards

Angular displacement (θ\theta)

The change in the angle as an object rotates, often measured in radians (radrad). One complete revolution is equal to 2πrad2\pi\,rad.

4
New cards

Angular velocity (ω\omega)

The rate of change of angular displacement over time, often expressed in rad/srad/s or rad/minrad/min. For example, one counterclockwise rotation in 1 minute equals a velocity of 6.28rad/min6.28\,rad/min.

5
New cards

Angular acceleration (α\alpha)

The rate of change of angular velocity over time. It is positive for counterclockwise acceleration and negative for deceleration in the counterclockwise direction.

6
New cards

Linear acceleration (aa)

The rate of change of linear velocity, linked to angular acceleration by the formula a=rαa = r\alpha, where rr is the radius of the rotating object.

7
New cards

Rotational equilibrium

A state in which the sum of the torques acting on an object is zero (τ=0\sum \tau = 0), meaning clockwise torques are balanced by counterclockwise torques.

8
New cards

Moment of inertia (II)

A measure of an object's resistance to change in its rotation, which depends on the object's mass and how that mass is distributed relative to the axis of rotation.

9
New cards

Moment of inertia: Thin hoop

The rotational inertia for an object with all its mass concentrated at the rim, calculated as I=mr2I = mr^2.

10
New cards

Moment of inertia: Solid, uniform cylinder

The rotational inertia for a solid cylinder rotating about its central axis, calculated as I=12mr2I = \frac{1}{2}mr^2.

11
New cards

Moment of inertia: Solid, uniform sphere

The rotational inertia for a solid sphere rotating about its center, calculated as I=25mr2I = \frac{2}{5}mr^2.

12
New cards

Moment of inertia: Hollow sphere (Thin shell)

The rotational inertia for a sphere with all mass distributed at its surface, calculated as I=23mr2I = \frac{2}{3}mr^2. This value is greater than that of a solid sphere of equal mass and radius.

13
New cards

Newton's second law for rotational motion

The relationship stating that torque is equal to the moment of inertia multiplied by the angular acceleration, expressed as τ=Iα\tau = I\alpha.

14
New cards

Center of mass

The point on an object through which the force of gravity (weight) is considered to act, used as a reference point for calculating torques and balancing supports.

15
New cards

Static equilibrium

A state where an object remains at rest because both the net force and the net torque acting on it are zero.

16
New cards

Angular frequency

The number of revolutions per unit of time, which can be converted to angular velocity by multiplying by 2π2\pi.