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๐Ÿ”‹College Physics I โ€“ Introduction

Types of Forces

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Why This Matters

Forces are the foundation of everything in mechanicsโ€”they're what make objects speed up, slow down, change direction, or stay perfectly still. In Intro to College Physics, you're being tested on your ability to identify forces, draw free-body diagrams, and apply Newton's laws to predict motion. Every problem you encounter, from blocks on inclined planes to satellites in orbit, requires you to recognize which forces are acting and how they combine.

But here's the key insight: forces aren't random. They fall into predictable categories based on what causes themโ€”contact between surfaces, gravitational attraction, electromagnetic interactions, or restoring mechanisms. When you understand the underlying principle behind each force, you can tackle any scenario the exam throws at you. Don't just memorize names and formulasโ€”know what physical mechanism each force represents and when it shows up in problems.


Contact Forces: When Objects Touch

These forces arise from direct physical contact between objects. They result from electromagnetic interactions at the atomic level, but in introductory physics, we treat them as separate, measurable pushes and pulls at surfaces.

Normal Force

  • Always perpendicular to the contact surfaceโ€”this is the defining characteristic that distinguishes it from friction
  • Adjusts automatically to prevent objects from passing through surfaces; it's a response force, not a fixed value
  • Critical for inclined plane problemsโ€”on a slope at angle ฮธ\theta, the normal force equals mgcosโกฮธmg\cos\theta, not simply mgmg

Friction Force

  • Opposes relative motion or attempted motion between surfaces in contact; described by f=ฮผNf = \mu N
  • Static friction (ฮผs\mu_s) prevents motion and can vary up to a maximum; kinetic friction (ฮผk\mu_k) acts during sliding and is typically smaller
  • Depends on normal force, not surface areaโ€”doubling the weight doubles the friction

Applied Force

  • Any external push or pull delivered by a person, machine, or another object
  • Direction and magnitude are given in problems; this is usually your "known" force in calculations
  • Appears in Newton's second law as part of the net force determining acceleration

Compare: Normal force vs. Friction forceโ€”both arise from surface contact, but normal force acts perpendicular to the surface while friction acts parallel. On free-body diagrams, always draw these at right angles to each other.


Forces Transmitted Through Objects

Some forces travel through connecting materials like ropes, cables, or springs. These forces transfer energy and momentum from one point to another without the objects being in direct contact.

Tension Force

  • Pulls equally at both ends of an ideal rope or string; tension is transmitted, not created
  • Acts along the length of the connector and always pulls (never pushes)
  • In pulley systems, tension redirects force; for ideal pulleys, tension remains constant throughout the rope

Spring Force (Elastic Force)

  • Described by Hooke's Law: F=โˆ’kxF = -kx, where kk is the spring constant and xx is displacement from equilibrium
  • Always a restoring forceโ€”the negative sign indicates it opposes the displacement direction
  • Proportional to displacement, making springs ideal for studying simple harmonic motion

Compare: Tension vs. Spring forceโ€”both transmit force through a connector, but tension is constant along an ideal rope while spring force varies with stretch. If a problem involves changing force with position, think springs; if force is constant throughout, think tension.


Field Forces: Action at a Distance

These forces act without physical contact, operating through invisible fields that permeate space. They follow inverse-square laws, meaning their strength decreases with the square of the distance.

Gravitational Force

  • Attracts any two masses according to Newton's law: F=Gm1m2r2F = G\frac{m_1 m_2}{r^2}
  • Near Earth's surface, simplifies to Fg=mgF_g = mg where g=9.8ย m/s2g = 9.8 \text{ m/s}^2
  • Always attractive and responsible for weight, orbital motion, and tides

Electrostatic Force

  • Acts between charged objects following Coulomb's law: F=kq1q2r2F = k\frac{q_1 q_2}{r^2}
  • Can attract or repelโ€”opposite charges attract, like charges repel
  • Much stronger than gravity at atomic scales; holds atoms and molecules together

Magnetic Force

  • Acts on moving charges or magnetic materials, described by the Lorentz force: F=qvร—BF = qv \times B
  • Perpendicular to both velocity and fieldโ€”use the right-hand rule to find direction
  • Does no work on charged particles because force is always perpendicular to motion

Compare: Gravitational vs. Electrostatic forceโ€”both follow inverse-square laws (1/r21/r^2), but gravity only attracts while electrostatic force can attract or repel. FRQs often ask you to compare their relative strengths or explain why gravity dominates at large scales despite being weaker.


Resistive Forces: Opposition to Motion

These forces arise when objects move through a medium and always act opposite to the direction of motion. They convert kinetic energy into thermal energy, slowing objects down.

Air Resistance (Drag Force)

  • Opposes motion through air and increases with velocity; often modeled as Fdโˆv2F_d \propto v^2
  • Depends on shape and cross-sectional areaโ€”streamlined objects experience less drag
  • Creates terminal velocity when drag equals gravitational force, resulting in zero net force

Compare: Friction vs. Air resistanceโ€”both oppose motion, but friction depends on normal force while air resistance depends on speed and shape. At low speeds, friction dominates; at high speeds, drag becomes the limiting factor.


Forces That Maintain Circular Motion

Centripetal Force

  • Not a new type of forceโ€”it's the net force directed toward the center of a circular path
  • Provided by other forces: gravity (orbits), tension (swinging objects), friction (cars turning), or normal force (roller coasters)
  • Calculated as Fc=mv2r=mฯ‰2rF_c = \frac{mv^2}{r} = m\omega^2 r, where vv is speed and rr is radius

Compare: Centripetal force vs. individual forcesโ€”centripetal force is a role, not a force type. On free-body diagrams, never label a force as "centripetal"; instead, identify which real force (gravity, tension, friction) provides the centripetal acceleration.


Quick Reference Table

ConceptBest Examples
Contact forcesNormal force, Friction, Applied force
Transmitted forcesTension, Spring force
Inverse-square field forcesGravitational force, Electrostatic force
Forces on moving chargesMagnetic force, Electrostatic force
Resistive forcesFriction, Air resistance
Restoring forcesSpring force
Forces providing circular motionGravity, Tension, Friction, Normal force
Forces that can attract or repelElectrostatic force, Magnetic force

Self-Check Questions

  1. Which two forces both follow an inverse-square law, and what key difference determines whether they attract or repel?

  2. On an inclined plane, how do normal force and friction force differ in direction, and what determines the magnitude of each?

  3. A block hangs from a spring attached to the ceiling. Identify all forces acting on the block and explain which force is responsible for the spring stretching.

  4. Compare and contrast static friction and kinetic friction: under what conditions does each apply, and which has the larger coefficient?

  5. A car rounds a flat curve at constant speed. What type of force provides the centripetal acceleration, and what would happen if this force were suddenly removed?