Skip to main content
Back

Kinematics: Describing Motion in One and Two Dimensions

Study Guide - Smart Notes

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

Motion and Mechanics

Introduction to Motion

Motion is a fundamental concept in physics, describing the change in position of objects over time. The study of motion is called mechanics, which is divided into two main branches: kinematics (how objects move) and dynamics (why objects move).

  • Kinematics: Focuses on the description of motion without considering its causes.

  • Dynamics: Explains the reasons behind motion, such as forces.

Frames of Reference and Coordinate Systems

Understanding Frames of Reference

To describe motion accurately, it is essential to specify a frame of reference. A frame of reference is a coordinate system within which the position, velocity, and acceleration of objects are measured. The same event can appear different in different frames of reference.

  • Inertial Frame: A non-accelerating frame where Newton's laws hold.

  • Accelerated Frame: A frame that is accelerating relative to an inertial frame.

Position and Displacement

Position Vectors

The position of an object is described by a vector \( \vec{r} \) in a coordinate system, typically given as \( \vec{r} = x \hat{i} + y \hat{j} \) in two dimensions.

  • Polar Coordinates: \( x = r \cos \theta \), \( y = r \sin \theta \)

  • Magnitude: \( r = \sqrt{x^2 + y^2} \)

  • Direction: \( \theta = \tan^{-1}(y/x) \)

Displacement

Displacement is the change in position of an object, defined as the vector difference between the final and initial positions:

  • \( \Delta \vec{r} = \vec{r}_f - \vec{r}_i = (x_f - x_i) \hat{i} + (y_f - y_i) \hat{j} \)

  • Magnitude: \( \Delta r = \sqrt{(\Delta x)^2 + (\Delta y)^2} \)

  • Direction: \( \theta_{\Delta r} = \tan^{-1}(\Delta y / \Delta x) \)

Distance is the total length of the path traveled, while displacement is the straight-line vector from start to finish.

Velocity and Speed

Average and Instantaneous Velocity

Velocity is the rate of change of displacement with respect to time. It is a vector quantity, having both magnitude and direction.

  • Average velocity: \( \vec{v}_{avg} = \frac{\Delta \vec{r}}{\Delta t} \)

  • Instantaneous velocity: \( \vec{v} = \lim_{\Delta t \to 0} \frac{\Delta \vec{r}}{\Delta t} = \frac{d\vec{r}}{dt} \)

  • Components: \( \vec{v} = v_x \hat{i} + v_y \hat{j} \)

  • Magnitude: \( v = \sqrt{v_x^2 + v_y^2} \)

  • Direction: \( \theta_v = \tan^{-1}(v_y / v_x) \)

Speed is the magnitude of velocity and is always positive. Average speed is defined as total distance divided by total time: \( v_{avg} = \frac{d}{\Delta t} \).

Graphical Interpretation

  • On a position-time (r-t) graph, the slope at any point gives the instantaneous velocity.

  • On a velocity-time (v-t) graph, the area under the curve represents displacement.

Acceleration

Definition and Interpretation

Acceleration is the rate of change of velocity with respect to time. It is a vector quantity.

  • Average acceleration: \( \vec{a}_{avg} = \frac{\Delta \vec{v}}{\Delta t} \)

  • Instantaneous acceleration: \( \vec{a} = \lim_{\Delta t \to 0} \frac{\Delta \vec{v}}{\Delta t} = \frac{d\vec{v}}{dt} \)

  • Positive acceleration: Increasing speed in the direction of velocity.

  • Negative acceleration (deceleration): Decreasing speed, acceleration opposite to velocity.

On a velocity-time (v-t) graph, the slope gives acceleration. On an acceleration-time (a-t) graph, the area under the curve gives the change in velocity.

Relative Motion and Galilean Relativity

Relative Velocity in One and Two Dimensions

Relative motion describes how the velocity of an object appears different depending on the observer's frame of reference. The Galilean transformation is used for adding velocities in classical mechanics:

  • \( \vec{v}_{A/B} = \vec{v}_{A/C} + \vec{v}_{C/B} \)

  • For example, the velocity of a ball inside a moving bus as seen from the ground is the sum of the ball's velocity relative to the bus and the bus's velocity relative to the ground.

Example: If a boat moves north at 10 m/s relative to the water, and the river flows east at 3 m/s, the boat's velocity relative to the ground is found by vector addition:

  • \( \vec{v}_{BG} = \vec{v}_{BW} + \vec{v}_{WG} \)

  • \( \vec{v}_{BG} = 10 \hat{j} + 3 \hat{i} \) m/s

  • Magnitude: \( v = \sqrt{10^2 + 3^2} = \sqrt{109} \approx 10.44 \) m/s

  • Direction: \( \theta = \tan^{-1}(3/10) \approx 16.7^\circ \) east of north

Frame of Reference

Velocity Observed

Ground

Sum of all relative velocities

Moving Vehicle

Object's velocity relative to vehicle

Summary Table: Key Kinematic Quantities

Quantity

Symbol

Definition

Equation

Position

\( \vec{r} \)

Location in space

\( \vec{r} = x \hat{i} + y \hat{j} \)

Displacement

\( \Delta \vec{r} \)

Change in position

\( \Delta \vec{r} = \vec{r}_f - \vec{r}_i \)

Velocity

\( \vec{v} \)

Rate of change of displacement

\( \vec{v} = \frac{d\vec{r}}{dt} \)

Speed

\( v \)

Magnitude of velocity

\( v = |\vec{v}| \)

Acceleration

\( \vec{a} \)

Rate of change of velocity

\( \vec{a} = \frac{d\vec{v}}{dt} \)

Additional info: In real-world applications, understanding frames of reference is crucial for navigation, engineering, and interpreting experimental results in physics.

Pearson Logo

Study Prep