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Motion in Two Dimensions: Vectors, Acceleration, and Projectile Motion

Study Guide - Smart Notes

Tailored notes based on your materials, expanded with key definitions, examples, and context.

Motion in Two Dimensions

Learning Goals

This chapter introduces the analysis of motion in two or three dimensions using vectors. The main objectives are:

  • Representing position and velocity of a particle using vectors in two or three dimensions.

  • Finding vector acceleration and interpreting its components parallel and perpendicular to a particle’s path.

  • Solving problems involving curved paths, such as projectile motion.

  • Analyzing circular motion with constant or varying speed.

  • Relating velocities as seen from different frames of reference.

Position and Displacement in 2D

Position Vectors

In two dimensions, the position of a particle is represented by a vector from the origin to the particle’s location.

  • The position vector r at time t has components (x, y).

  • Displacement is the change in position, given by the vector difference:

  • Components: ,

Velocity in Two Dimensions

Average and Instantaneous Velocity

Velocity is the rate of change of position. In two dimensions:

  • Average velocity:

  • Instantaneous velocity:

  • The velocity vector is always tangent to the path of the particle.

Example: If a comet moves from (2.0 m, 1.0 m) to (3.0 m, 5.0 m) in 4.0 s, its average velocity is:

Acceleration in Two Dimensions

Average and Instantaneous Acceleration

Acceleration describes how velocity changes with time.

  • Average acceleration:

  • Instantaneous acceleration:

  • The direction of average acceleration is the same as the change in velocity .

Components of Acceleration

  • Acceleration can be decomposed into components parallel () and perpendicular () to the velocity vector.

  • changes the speed; changes the direction.

  • For curved paths, points toward the center of curvature (concave side).

Motion in a Circular Path

Uniform Circular Motion

When a particle moves in a circle at constant speed:

  • The acceleration is always directed toward the center (centripetal acceleration).

  • Magnitude: , where is speed and is the radius.

  • The period (time for one revolution):

  • Velocity and acceleration vectors are always perpendicular.

Nonuniform Circular Motion

  • If speed varies, there is a tangential acceleration in addition to the radial (centripetal) acceleration .

  • (radial), (tangential)

  • The total acceleration is the vector sum of and .

Projectile Motion

Basic Principles

A projectile is any object given an initial velocity and then allowed to move under the influence of gravity alone (neglecting air resistance).

  • Projectile motion occurs in a vertical plane.

  • The horizontal motion has constant velocity; the vertical motion has constant acceleration .

  • At the peak of the trajectory, velocity and acceleration are perpendicular.

Equations of Projectile Motion

  • Let initial position be , initial speed , and launch angle .

  • Horizontal motion:

  • Vertical motion:

  • Horizontal velocity: (constant)

  • Vertical velocity:

  • The trajectory is a parabola:

Projectile Range

  • The range (horizontal distance traveled) is maximized for a launch angle of (on level ground).

  • Range formula:

  • On the Moon, where is smaller, the range increases (for the same and ).

Relative Motion

Frames of Reference

The velocity of an object depends on the observer’s frame of reference.

  • Relative velocity:

  • Example: A person walks at 1.0 m/s on a train moving at 10 m/s. Relative to the ground, their speed is 11 m/s (if walking in the same direction as the train).

Applications

  • River crossing problems: Swimmers or boats must account for both their own speed and the current’s speed.

  • To move directly across a river, a swimmer must aim upstream to compensate for the current.

Effects of Air Resistance

Air Drag in Projectile Motion

When air resistance is significant:

  • Acceleration is no longer constant.

  • The trajectory is not a perfect parabola; maximum height and range decrease.

  • Air drag acts opposite to the velocity vector.

Direction of Drag Force

  • The acceleration due to drag always points opposite to the direction of motion.

  • After the peak of a projectile’s flight, drag continues to oppose the velocity, affecting both horizontal and vertical components.

Summary Table: Key Equations for 2D Motion

Quantity

Equation

Description

Displacement

Change in position vector

Average velocity

Rate of change of position

Instantaneous velocity

Velocity at a specific instant

Average acceleration

Rate of change of velocity

Instantaneous acceleration

Acceleration at a specific instant

Centripetal acceleration

Uniform circular motion

Projectile horizontal position

Horizontal displacement

Projectile vertical position

Vertical displacement

Projectile range

Maximum horizontal distance

Relative velocity

Velocity addition between frames

Additional info: Some context and equations have been inferred and expanded for clarity and completeness, based on standard college physics curriculum.

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