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Applying Newton’s Laws: Equilibrium, Dynamics, Friction, and Circular Motion

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Applying Newton’s Laws

Overview

This chapter explores the application of Newton’s laws of motion to solve problems involving equilibrium, dynamics, friction, and circular motion. Mastery of these concepts is essential for understanding the behavior of physical systems in classical mechanics.

Equilibrium and Newton’s First Law

Definition of Equilibrium

A body is in equilibrium when it is at rest or moving with constant velocity in an inertial frame of reference. Newton’s first law states that the net force on a body in equilibrium must be zero.

  • Net force: The vector sum of all forces acting on a body.

  • Equilibrium conditions: The sum of the x-components and y-components of force must each be zero.

Equations:

Newton's first law and equilibrium conditions

Problem-Solving Strategy for Equilibrium

  1. Draw a sketch of the physical situation.

  2. Draw a free-body diagram for each body in equilibrium.

  3. Identify all forces acting on the body (e.g., weight ).

  4. Choose coordinate axes and include them in the diagram.

  5. Find force components along each axis and set their sums to zero.

  6. Solve the resulting equations for unknowns.

Dynamics and Newton’s Second Law

Definition of Dynamics

When the net force on a body is not zero, the body accelerates according to Newton’s second law. The acceleration is in the direction of the net force.

  • Newton’s second law:

  • Each component: ,

Newton's second law and dynamics conditions

Problem-Solving Strategy for Dynamics

  1. Draw a sketch and free-body diagram for each moving body.

  2. Label all forces, including weight .

  3. Choose coordinate axes and show them in the diagram.

  4. Identify relationships among bodies (e.g., connected by a rope).

  5. Determine force components and write Newton’s second law for each axis.

  6. List knowns and unknowns, solve for target variables.

Free-Body Diagrams: Correct and Incorrect Practices

  • Only forces should be included in a free-body diagram.

  • Acceleration vectors can be drawn to the side, but is not a force and should not be included as a force vector.

Only gravity acts on a falling fruit Correct free-body diagram with acceleration vector Incorrect free-body diagram with m a vector

Frictional Forces

Nature of Friction

Friction is a force that opposes the relative motion of two surfaces in contact. It is essential for locomotion and many everyday phenomena.

  • Frictional force: Acts parallel to the surface.

  • Normal force: Acts perpendicular to the surface.

  • Both are components of the contact force between surfaces.

Caterpillar on apple illustrating friction Contact force components: friction and normal force Molecular origin of friction and normal forces

Kinetic and Static Friction

  • Kinetic friction: Acts when a body slides over a surface.

  • Static friction: Acts when there is no relative motion.

  • Static friction increases up to a maximum value before motion begins.

Stages of Friction in Box Motion

  1. No applied force:

  2. Weak applied force:

  3. Stronger applied force:

  4. Box slides:

Box at rest, no friction Box with weak applied force, static friction Box with strong applied force, maximum static friction Box sliding, kinetic friction

Coefficients of Friction

The coefficient of friction depends on the materials in contact. Static friction is usually greater than kinetic friction.

Materials

Coefficient of Static Friction, \(\mu_s\)

Coefficient of Kinetic Friction, \(\mu_k\)

Steel on steel

0.74

0.57

Aluminum on steel

0.61

0.47

Copper on steel

0.53

0.36

Brass on steel

0.51

0.44

Zinc on cast iron

0.85

0.21

Copper on cast iron

1.05

0.29

Glass on glass

0.94

0.40

Copper on glass

0.68

0.53

Teflon on steel

0.04

0.04

Teflon on Teflon

0.04

0.04

Rubber on concrete (dry)

1.0

0.8

Rubber on concrete (wet)

0.30

0.25

Table of coefficients of friction for various materials

Stick-Slip Phenomenon

Stick-slip occurs when static friction alternates with kinetic friction, as seen in squeaky windshield wipers on dry glass. Wet surfaces reduce friction and eliminate stick-slip.

Windshield wiper stick-slip phenomenon

Fluid Resistance and Terminal Speed

Fluid Resistance

Fluid resistance (drag) opposes the motion of objects through fluids. The resisting force increases with speed and can be linear or quadratic in velocity.

  • At terminal speed, the drag force equals the weight of the body.

  • Before terminal speed: or

  • At terminal speed: or

Drag force and terminal speed conditions

Velocity vs. Time with Fluid Resistance

With fluid resistance, velocity approaches an upper limit (terminal speed) rather than increasing indefinitely.

Velocity versus time with and without fluid resistance

Dynamics of Circular Motion

Uniform Circular Motion

In uniform circular motion, both acceleration and net force are directed toward the center of the circle. The net force is called the centripetal force.

  • Velocity is tangent to the circle; acceleration and net force point toward the center.

Uniform circular motion: force and acceleration toward center

What Happens if the String Breaks?

If the string breaks, no net force acts on the ball, and it moves in a straight line at constant velocity, obeying Newton’s first law.

Ball moves in straight line after string breaks

Avoiding the 'Centrifugal Force' Misconception

In an inertial frame, there is no such thing as 'centrifugal force.' Only real forces should be included in free-body diagrams. The quantity is not a force but the result of the net force required for circular motion.

Correct and incorrect free-body diagrams for circular motion

The Fundamental Forces of Nature

Classification of Forces

All forces in nature are manifestations of four fundamental interactions:

  • Gravitational

  • Electromagnetic

  • Strong interaction

  • Weak interaction

Physicists aim to unify these interactions into a comprehensive theory of everything.

Summary Table: Types of Friction

Type

Formula

Condition

Static friction

No relative motion

Kinetic friction

Sliding motion

Key Equations

  • Equilibrium:

  • Newton’s second law:

  • Static friction:

  • Kinetic friction:

  • Circular motion:

Example Application

Example: A box is pulled across a floor. If the coefficient of kinetic friction is 0.4 and the normal force is 50 N, the frictional force is N.

Example: A ball of mass 0.5 kg moves in a circle of radius 2 m at 3 m/s. The net force required is N toward the center.

Additional info: Academic context and examples were added to ensure completeness and clarity for exam preparation.

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