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๐Ÿ”งIntro to Mechanics

Fundamental Forces in Nature

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Why This Matters

In AP Physics 1, you're building the foundation for understanding why objects move and interact the way they do. While the full picture of fundamental forces spans all of physics, your exam focuses specifically on gravitational force and how it connects to the broader framework of Newton's laws, free-body diagrams, and conservation principles. Understanding gravity isn't just about memorizing an equationโ€”it's about recognizing how this single force explains everything from why you stay on the ground to how satellites orbit Earth.

The key insight here is that gravitational force follows predictable mathematical rules that let you solve real problems. You'll need to connect Newton's law of universal gravitation to concepts like weight, apparent weight, free fall, and orbital motion. Don't just memorize that Fg=Gm1m2r2F_g = \frac{Gm_1m_2}{r^2}โ€”know how this inverse-square relationship affects gravitational field strength at different distances, and how gravity interacts with other forces in systems you'll analyze on the exam.


The Gravitational Force: Your AP Physics 1 Focus

Gravity is the force that acts between any two objects with mass, always attractive, and responsible for the large-scale structure of the universe. On the AP exam, you'll apply gravitational concepts to analyze motion, weight, and orbital scenarios.

Newton's Law of Universal Gravitation

  • Every mass attracts every other massโ€”the force is always attractive and acts along the line connecting the objects' centers of mass
  • Inverse-square law means the force decreases with the square of the distance: โˆฃFgโˆฃ=Gm1m2r2|F_g| = \frac{Gm_1m_2}{r^2}, where G=6.67ร—10โˆ’11ย N\cdotpm2/kg2G = 6.67 \times 10^{-11} \text{ Nยทm}^2/\text{kg}^2
  • Gravitational field strength g=GMr2g = \frac{GM}{r^2} gives the force per unit mass at any distance from a massive objectโ€”this is why gโ‰ˆ10ย m/s2g \approx 10 \text{ m/s}^2 near Earth's surface

Gravitational Field Strength

  • Field strength varies with distanceโ€”as you move farther from a planet's center, gg decreases following the inverse-square relationship
  • Near Earth's surface, we approximate gg as constant (โ‰ˆ9.8ย m/s2\approx 9.8 \text{ m/s}^2 or 10ย N/kg10 \text{ N/kg}) because changes in altitude are negligible compared to Earth's radius
  • Units of N/kg and m/sยฒ are equivalentโ€”this connects gravitational field to acceleration, which is why objects in free fall accelerate at gg

Compare: Gravitational force vs. gravitational field strengthโ€”force (FgF_g) depends on both masses and requires you to know the object's mass, while field strength (gg) depends only on the source mass and distance. If an FRQ asks about conditions at a location in space, calculate gg first, then find force for any object placed there.


Weight and Apparent Weight

Understanding the difference between actual gravitational force and what you feel is crucial for analyzing systems where objects accelerate. This distinction appears frequently in elevator problems and free-fall scenarios.

Weight as Gravitational Force

  • Weight equals mass times gravitational field strengthโ€”mathematically W=mgW = mg, representing the actual gravitational pull on an object
  • Weight is a force, measured in newtons, and always points toward the center of the attracting mass
  • Weight changes with locationโ€”an astronaut weighs less on the Moon because gMoon<gEarthg_{\text{Moon}} < g_{\text{Earth}}, not because their mass changed

Apparent Weight and Normal Force

  • Apparent weight is what you feelโ€”it equals the normal force exerted on you by a surface (like a scale reading)
  • In accelerating systems, use Nโˆ’mg=maN - mg = ma to find apparent weight: accelerating upward increases it, accelerating downward decreases it
  • Weightlessness occurs in free fallโ€”when gravity is the only force acting, there's no normal force, so apparent weight is zero (this is why astronauts float in orbit)

The Equivalence Principle

  • You cannot distinguish between gravity and accelerationโ€”an observer in a closed box can't tell if they're in a gravitational field or accelerating through space
  • Inertial mass equals gravitational massโ€”this fundamental principle means the mm in F=maF = ma is the same as the mm in Fg=mgF_g = mg
  • This explains why all objects fall at the same rateโ€”the mm cancels when you set mg=mamg = ma, giving a=ga = g regardless of mass

Compare: True weight vs. apparent weightโ€”both equal mgmg when you're at rest on the ground, but they diverge in accelerating systems. In an elevator accelerating upward at 2ย m/s22 \text{ m/s}^2, your apparent weight is m(g+2)m(g + 2) while your true weight remains mgmg. Exam tip: always draw a free-body diagram showing gravity down and normal force up before solving.


Forces and Conservation Laws

The gravitational force connects directly to the conservation principles you'll use throughout AP Physics 1. Newton's third law and momentum conservation are essential tools for analyzing gravitational interactions.

Newton's Third Law in Gravitational Systems

  • Forces come in pairsโ€”Earth pulls on you with force FF, and you pull on Earth with equal force FF in the opposite direction
  • Both objects experience the same magnitude of forceโ€”but because a=F/ma = F/m, Earth's acceleration is negligible due to its enormous mass
  • This applies to all gravitational interactionsโ€”the Moon pulls on Earth just as hard as Earth pulls on the Moon

Conservation of Momentum in Gravitational Systems

  • Total momentum is conserved when no external forces actโ€”internal gravitational forces between objects in a system don't change total system momentum
  • Center-of-mass velocity remains constant for isolated systems: vcm=ฮฃmiviฮฃmiv_{cm} = \frac{\Sigma m_i v_i}{\Sigma m_i}
  • Recoil problems use this principleโ€”when a rocket expels fuel, momentum conservation explains the rocket's acceleration even though gravity acts on both

Impulse and Gravitational Force

  • Impulse equals change in momentumโ€”J=ฮ”p=Fโ‹…ฮ”tJ = \Delta p = F \cdot \Delta t, connecting force, time, and momentum change
  • Gravitational force delivers continuous impulseโ€”a falling object gains momentum at rate mgmg per second
  • Conservation applies to collisions and explosionsโ€”even when gravity acts, if the collision time is short enough, we can ignore gravity's impulse during the interaction

Compare: Internal vs. external forces in momentum conservationโ€”gravitational forces between objects in your system are internal and don't change total momentum, but gravitational forces from outside your system (like Earth pulling on a ball you're analyzing) are external and do change momentum. Define your system boundaries carefully on FRQs.


Beyond AP Physics 1: The Four Fundamental Forces

While AP Physics 1 focuses on gravity, understanding where it fits among nature's forces gives you perspective. You won't be tested on nuclear forces, but this context helps you appreciate why gravity matters.

Overview of All Four Forces

  • Gravitational force is the weakest but has infinite rangeโ€”it dominates at large scales because it's always attractive and mass accumulates
  • Electromagnetic force is much stronger than gravity with infinite rangeโ€”it governs charged particle interactions but cancels out in neutral matter
  • Strong nuclear force is the strongest but only acts at femtometer scalesโ€”it holds atomic nuclei together against electromagnetic repulsion

Why Gravity Dominates Your World

  • Large objects are electrically neutralโ€”positive and negative charges cancel, so electromagnetic forces between planets are negligible
  • Gravity never cancelsโ€”there's no "negative mass," so gravitational effects always add up
  • At human and astronomical scales, gravity is the dominant force shaping motion, orbits, and structure

Compare: Gravitational vs. electromagnetic forceโ€”both follow inverse-square laws (1/r21/r^2), but electromagnetic force is about 103610^{36} times stronger. The reason gravity dominates planetary motion is that large objects have enormous mass but nearly zero net charge. This is a great example of how context determines which force matters.


Quick Reference Table

ConceptKey Equations & Examples
Universal GravitationFg=Gm1m2r2F_g = \frac{Gm_1m_2}{r^2}, attraction between any two masses
Gravitational Field Strengthg=GMr2g = \frac{GM}{r^2}, varies with distance from source
WeightW=mgW = mg, gravitational force on an object
Apparent WeightNormal force felt by object, N=m(gยฑa)N = m(g \pm a) in accelerating systems
Free Fall / WeightlessnessApparent weight = 0 when gravity is the only force
Equivalence PrincipleCannot distinguish gravity from acceleration in closed system
Momentum Conservationฮฃpbefore=ฮฃpafter\Sigma p_{\text{before}} = \Sigma p_{\text{after}} for isolated systems
Impulse-MomentumJ=ฮ”p=Fโ‹…ฮ”tJ = \Delta p = F \cdot \Delta t

Self-Check Questions

  1. An astronaut orbiting Earth feels weightless. Is the gravitational force on them zero? Explain using the concepts of weight and apparent weight.

  2. Compare how gravitational force and gravitational field strength change as you move from Earth's surface to twice Earth's radius from the center. Which quantity requires knowing the object's mass?

  3. A 60 kg person stands on a scale in an elevator. The scale reads 720 N. Is the elevator accelerating upward, downward, or not at all? Calculate the acceleration.

  4. Two ice skaters push off each other on frictionless ice. Explain why total momentum is conserved even though gravitational force acts on both skaters.

  5. Earth exerts a gravitational force of 800 N on an astronaut. What force does the astronaut exert on Earth, and why don't we notice Earth accelerating toward the astronaut?