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Vocabulary flashcards covering key concepts in two-dimensional motion, projectile motion, and circular motion from the notes.
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Position Vector (r)
A vector from the origin to the particle’s location in the plane; in components r = x i + y j.
Displacement (Δr)
The change in position; the difference between final and initial position vectors: Δr = rf − ri.
Trajectory
The path that a particle follows in the plane (xy-plane).
Average Velocity (v_avg)
Displacement divided by the time interval: v_avg = Δr/Δt; points in the direction of the displacement.
Instantaneous Velocity
The limit of average velocity as Δt → 0; the velocity at a specific instant; tangent to the trajectory.
Speed
Magnitude of velocity; the rate of motion without regard to direction.
Velocity Components (vx, vy)
Projections of velocity along the x and y axes; vx = dx/dt, vy = dy/dt.
Average Acceleration (a_avg)
Change in velocity over a time interval: a_avg = Δv/Δt.
Instantaneous Acceleration
The limit of average acceleration as Δt → 0; the acceleration at a specific time.
Acceleration Components (ax, ay)
Decomposition of acceleration along the x and y axes; ax = dvx/dt, ay = dvy/dt.
Projectile Motion
Two-dimensional motion under gravity with negligible air resistance; x-acceleration = 0, y-acceleration = −g.
Launch Angle (θ)
Angle of the initial velocity relative to the +x axis.
Initial Velocity (v0)
Velocity at launch; magnitude v0 with components v0x = v0 cosθ and v0y = v0 sinθ.
Independence of Motions
Motion along x and y are independent; x-equations involve x quantities and y-equations involve y quantities.
Uniform Circular Motion (UCM)
Motion around a circle at constant speed; velocity direction changes, producing centripetal acceleration toward the center.
Centripetal Acceleration (ac or ar)
Acceleration toward the circle’s center; magnitude a_r = v^2/r = ω^2 r.
Radius (R)
Distance from the center of the circle to a point on the circular path.
Period (T)
Time for one complete revolution; T = 2πR/v = 2π/ω.
Frequency (f)
Revolutions per unit time; f = 1/T; related to angular velocity by ω = 2π f.
Angular Position (θ)
Angle from the +x axis to the position on the circle; measured in radians, positive for counterclockwise.
Arc Length (s)
Distance traveled along the circular path; s = R θ.
Angular Displacement (Δθ)
Change in angular position; Δθ = θf − θi.
Angular Velocity (ω)
Rate of change of angular position; ω = dθ/dt; units rad/s; constant in uniform circular motion.
Tangential Acceleration (a_t)
Component of acceleration parallel to velocity; changes speed; a_t = α R where α = dω/dt.
Angular Acceleration (α)
Rate of change of angular velocity; α = dω/dt; units rad/s^2; describes speeding up or slowing down of rotation.
Radian (rad)
Unit of angular measure; 1 radian is the angle subtended by an arc length equal to the radius.
Relation v = ω r
Linear speed equals angular speed times radius: v = ω r.
Parabolic Trajectory
The projectile’s path is a parabola obtained by eliminating time between x(t) and y(t) equations.
Gravity (g)
Acceleration due to gravity; downward acceleration g ≈ 9.8 m/s^2 (downward).
Horizontal Motion in Projectile
No horizontal acceleration; x = v0x t.
Vertical Motion in Projectile
Constant downward acceleration −g; y = v0y t − 1/2 g t^2.
Independent Motion Example
Horizontal motion is independent of vertical motion, as seen when a ball is projected horizontally.
Trajectory Equation (y(x))
The relation between y and x for a projectile, typically a parabola described by y(x) = x tanθ − (g x^2)/(2 v0^2 cos^2 θ).
Center-Seeking Acceleration
Another name for centripetal (radial) acceleration toward the circle’s center.
Tangential vs Radial Components
Tangential acceleration changes speed (along v); radial (centripetal) acceleration changes direction (toward center).
Constant Acceleration Kinematics (2D)
When acceleration is constant, x and y motions can be treated independently with Δt the same for both.