Physics · Units 1–10 · Quick reference
Physics 1
Units, vectors and significant figures; motion and projectiles; Newton’s laws, friction and pulleys; circular motion and gravity; energy, momentum and rotation; oscillations, waves and sound; fluids; heat; electricity, magnetism and optics.
1Measurement, Units & Vectors
| Quantity | Unit | Symbol |
|---|---|---|
| length | meter | m |
| mass | kilogram | kg |
| time | second | s |
| electric current | ampere | A |
| temperature | kelvin | K |
| amount | mole | mol |
| brightness | candela | cd |
Metric prefixes
- G, M, k
- 10⁹, 10⁶, 10³ (giga, mega, kilo)
- c, m
- 10⁻², 10⁻³ (centi, milli)
- μ, n
- 10⁻⁶, 10⁻⁹ (micro, nano)
Gentle Mice Keep Cheese Mostly Under Nightstands
Prefixes from big to small: G, M, k, c, m, μ, n.
| Unit | Equals | Unit | Equals |
|---|---|---|---|
| N | kg·m/s² | Pa | N/m² |
| J | N·m | Hz | 1/s |
| W | J/s | C | A·s |
| V | J/C | Ω | V/A |
Convert with unit fractions Worked
Significant figures
- Nonzero digits and zeros between them count; leading zeros never do (0.00340 has 3).
- Trailing zeros count only with a decimal point (2.50 has 3).
- × and ÷: fewest significant figures. + and −: fewest decimal places.
- Counted and defined numbers are exact.
Rounding the answer Worked
Components and resultant
Scalar: size only (12 s). Vector: size and direction (5 m north). Add x parts and y parts separately.
Aₓ = A cos θ, Ay = A sin θ
R = √(Rₓ² + Ry²)
θ = tan⁻¹(Ry ÷ Rₓ)
Walk east, then north Worked
Cos is close
The cosine goes with the side close to the angle, so with θ measured from the x-axis, A cos θ is the x part.
Honest measure
- Accurate: near the true value. Precise: repeats agree.
- Percent error = |measured − accepted| ÷ accepted × 100 %.
- “A false balance is abomination to the LORD: but a just weight is his delight” (Proverbs 11:1, KJV).
2Constants & Key Equations
| Constant | Value |
|---|---|
| g (Earth’s surface) | 9.8 m/s² |
| G (gravitation) | 6.674 × 10⁻¹¹ N·m²/kg² |
| k (Coulomb) | 8.99 × 10⁹ N·m²/C² |
| e (elementary charge) | 1.602 × 10⁻¹⁹ C |
| c (light in vacuum) | 3.00 × 10⁸ m/s |
| μ₀ (magnetic) | 4π × 10⁻⁷ T·m/A |
| Earth: mass, radius | 5.97 × 10²⁴ kg, 6371 km |
Solving any problem
- Sketch; list knowns with units; name the unknown.
- Pick an equation where only the unknown is missing; solve with symbols, then numbers.
- Check units, size and sig figs.
| Quantity | Value |
|---|---|
| water density | 1000 kg/m³ |
| water specific heat | 4186 J/(kg·°C) |
| ice melts (Lf) | 334 kJ/kg |
| water boils (Lv) | 2260 kJ/kg |
| 1 atm | 101.3 kPa = 760 mm Hg |
| sound in air, 20 °C | 343 m/s |
| n: air, water, glass | 1.00, 1.33, ≈ 1.50 |
| absolute zero | 0 K = −273.15 °C |
| 1 cal; 1 hp | 4.186 J; 746 W |
| 1 kWh | 3.6 × 10⁶ J |
Units ride along
Carry units through every line; wrong units in the answer mean an algebra slip.
| Topic | Equations |
|---|---|
| Motion | v = v₀ + at; Δx = v₀t + ½at²; v² = v₀² + 2aΔx |
| Forces | Fnet = ma; W = mg; f = μN; F = kx |
| Gravity | ac = v²/r; F = Gm₁m₂/r² |
| Energy | W = Fd cos θ; KE = ½mv²; PE = mgh; P = W/t |
| Momentum | p = mv; FΔt = Δp |
| Rotation | τ = rF sin θ; τ = Iα; L = Iω |
| Waves | v = fλ; T = 2π√(L/g); T = 2π√(m/k) |
| Fluids | P = F/A; P = P₀ + ρgh; Fb = ρVg |
| Heat | Q = mcΔT; Q = mL; ΔU = Q − W |
| Electricity | F = kq₁q₂/r²; V = IR; P = IV |
| Magnetism | F = BIL sin θ; F = qvB sin θ |
| Optics | n₁ sin θ₁ = n₂ sin θ₂; 1/f = 1/do + 1/di |
3Motion in One Dimension
- Displacement Δx
- change in position, with direction (vector)
- Distance
- total path length (scalar)
- Velocity v
- Δx ÷ Δt, with direction
- Speed
- size of velocity
- Acceleration a
- Δv ÷ Δt (m/s²): speeding up, slowing down or turning
| Equation (constant a) | Leaves out |
|---|---|
| v = v₀ + at | Δx |
| Δx = v₀t + ½at² | v |
| v² = v₀² + 2aΔx | t |
| Δx = ½(v₀ + v)t | a |
Skip the stranger
List the five letters v₀, v, a, t, Δx. Choose the equation that leaves out the one you neither know nor want.
Speeding up Worked
Braking distance Worked
Free fall
- Take up as +: a = −g = −9.8 m/s², going up or coming down.
- Without air, all objects fall alike (Apollo 15 hammer and feather, 1971).
- At the top v = 0 but a is still −g.
Thrown straight up at 19.6 m/s Worked
Dropped from 45 m Worked
Reading a v–t graph Worked
| Graph | Slope gives | Area gives |
|---|---|---|
| x–t | velocity | — |
| v–t | acceleration | displacement |
| a–t | — | change in v |
Round trip Worked
Watch out
- Negative a does not always mean slowing; it means a points in the − direction.
- A flat x–t line means at rest; a flat v–t line means steady velocity.
4Projectiles
The key idea
- Horizontal and vertical motions are independent; time links them.
- Horizontal: no force (ignoring air), so vₓ stays constant.
- Vertical: free fall, a = −g.
Galileo showed the path is a parabola (Two New Sciences, 1638).
Off a cliff Worked
Projectile equations
R and H formulas: level ground, no air.
vₓ = v₀ cos θ, v0y = v₀ sin θ
x = vₓt, y = v0yt − ½gt²
R = v₀² sin 2θg, H = (v₀ sin θ)²2g
Launched at an angle Worked
Watch out
- At the top the velocity is vₓ, not zero.
- The acceleration is g downward at every point of the flight.
Facts worth knowing
- On level ground 45° gives the longest range (no air).
- Angles that add to 90° (30° and 60°) give the same range.
- A ball dropped and one thrown sideways from the same height land together.
Crossing a river Worked
Ruler across, stone down
Sideways the motion is steady as a ruler; up and down it falls like a dropped stone. Solve each, then join them by t.
5Newton’s Laws & Free-Body Diagrams
| Law | In words | Example |
|---|---|---|
| 1st (inertia) | An object keeps its velocity (or rest) unless a net force acts. | riders lurch forward when a car stops |
| 2nd | Fnet = ma: acceleration follows the net force. | twice the force, twice the acceleration |
| 3rd | Forces come in equal, opposite pairs on two different objects. | a rocket pushes gas down; gas pushes it up |
- Force
- a push or pull, in newtons (N)
- Mass m
- amount of matter; measures inertia (kg)
- Weight W
- gravity’s pull: W = mg (N)
- Equilibrium
- ΣF = 0: at rest or at constant velocity
Drawing a free-body diagram
- Draw the object alone as a box or dot.
- Draw every force on it as an arrow from it; label each.
- Choose axes, one along the acceleration.
- Write ΣFₓ = maₓ and ΣFy = may; solve.
| Force | Direction |
|---|---|
| Weight W = mg | straight down |
| Normal N | perpendicular out of a surface |
| Tension T | along a rope, pulling |
| Friction f | along a surface, against sliding |
| Spring F = kx | back toward rest length (Hooke, 1678) |
| Air drag | against the motion |
F = ma Worked
Riding an elevator Worked
Weight on the Moon Worked
Hanging sign Worked
Terminal velocity
- Air drag grows with speed until it equals the weight; then ΣF = 0 and the speed stays constant.
Two objects, two forces
A third-law pair acts on two different objects, so the pair never cancels. Forces that cancel act on the same object.
6Friction, Inclines & Pulleys
Friction
Static friction grows to match the push, up to its limit; usually μs > μk. Slipping angle: μs = tan θ.
fs ≤ μsN, fk = μkN
Incline (angle θ)
F∥ = mg sin θ, N = mg cos θ
a = g sin θ (no friction)
a = g(sin θ − μk cos θ) (sliding down)
| Surfaces | μs | μk |
|---|---|---|
| rubber on dry concrete | 1.0 | 0.8 |
| wood on wood | 0.25–0.5 | 0.2 |
| steel on steel (dry) | 0.74 | 0.57 |
| ice on ice | 0.1 | 0.03 |
Pushing a crate Worked
Sliding down a ramp Worked
Atwood machine
a = (m₂ − m₁)gm₁ + m₂, T = 2m₁m₂gm₁ + m₂
3.0 kg and 5.0 kg Worked
Two blocks pulled together Worked
Friction lies down, normal stands up
Friction runs along the surface against sliding; the normal force stands perpendicular to it. On a slope, N is less than mg.
7Circular Motion & Gravitation
Uniform circular motion
ac = v²r = 4π²rT²
Fc = mv²r, v = 2πrT
What supplies the force?
- Centripetal force is not a new force: it is the net inward force from tension, gravity, friction or the normal force.
- The outward “pull” riders feel is their own inertia.
Earth’s g from G Worked
Car on a flat curve Worked
Universal gravitation
r is center to center. Cavendish measured G with a torsion balance (1798).
F = Gm₁m₂r², g = GMr²
Twice as far, a quarter the pull
Gravity and the electric force fall off as 1/r²: double r and the force drops to ¼; triple it, to 1/9.
| Kepler’s law | Says |
|---|---|
| 1st (1609) | Planets move in ellipses with the Sun at one focus. |
| 2nd (1609) | A line to the Sun sweeps equal areas in equal times: faster when closer. |
| 3rd (1619) | T² ∝ a³; around the Sun, T² = a³ (T in years, a in AU). |
Circular orbits
GME = 3.986 × 10¹⁴ m³/s².
v = √(GMr), T = 2π√(r³GM)
Space station orbit Worked
Loop-the-loop Worked
Kepler’s third law Worked
Held in place
- “He stretcheth out the north over the empty place, and hangeth the earth upon nothing” (Job 26:7, KJV).
8Work, Energy & Power
Work
In joules. θ is between the force and the motion. A force at 90° to the motion does no work.
W = Fd cos θ
Pulling a wagon Worked
Work–energy theorem
Wnet = ΔKE = ½mvf² − ½mvi²
Roller coaster drop Worked
| Energy | Formula |
|---|---|
| Kinetic | KE = ½mv² |
| Gravitational potential | PE = mgh |
| Spring (elastic) | PE = ½kx² |
| Thermal, chemical, electrical | stored or moving in particles and fields |
Conservation of energy
- Without friction: KEi + PEi = KEf + PEf.
- With friction, the lost mechanical energy becomes thermal energy; the total stays the same.
Joule’s falling-weight paddle wheel (1845) showed heat is a form of energy.
Spring launcher Worked
Power
In watts (J/s). James Watt’s unit: 1 hp = 746 W. Energy bills use 1 kWh = 3.6 × 10⁶ J.
P = Wt = Fv
Climbing stairs Worked
- Efficiency
- useful energy outenergy in × 100 %; always under 100 %
- Kilowatt-hour
- a 100 W bulb lit for 10 h uses 1 kWh
Push along the path
Work needs force along the motion. Carrying a tray across a level room, or gravity on a circular orbit, does zero work.
9Momentum & Collisions
Momentum and impulse
In kg·m/s (= N·s). Momentum is a vector: pick a + direction.
p = mv
J = FavgΔt = Δp
Batting a ball Worked
Stretch the time
- The same Δp over a longer time means a smaller force: air bags, seat belts, crumple zones, bent knees on landing.
Conservation of momentum
Holds whenever no outside net force acts on the system.
m₁v₁ + m₂v₂ = m₁v₁′ + m₂v₂′
Truck meets car; they stick Worked
| Collision | Momentum | Kinetic energy |
|---|---|---|
| Elastic | conserved | conserved (equal billiard balls swap speeds) |
| Inelastic | conserved | some lost to heat, sound, bending |
| Perfectly inelastic | conserved | most lost: objects stick |
Add up before, add up after
Total momentum before equals total after. Choose + once, give each velocity its sign, then solve.
10Rotation, Torque & Balance
- Angle θ
- in radians: 1 rev = 2π rad = 360°
- Angular velocity ω
- Δθ ÷ Δt (rad/s); v = ωr
- Angular acceleration α
- Δω ÷ Δt (rad/s²)
Equilibrium
An object tips once its center of mass passes outside its base.
ΣF = 0 and Στ = 0
F₁d₁ = F₂d₂ (lever)
Torque
Lever arm: the perpendicular distance from the pivot to the force’s line.
τ = rF sin θ = F × lever arm
Wrench Worked
| Linear | Rotational |
|---|---|
| x, v, a | θ, ω, α |
| mass m | rotational inertia I |
| F = ma | τ = Iα |
| KE = ½mv² | KE = ½Iω² |
| p = mv | L = Iω |
| Shape (mass M, radius R) | I |
|---|---|
| hoop or ring | MR² |
| solid disk | ½MR² |
| solid sphere | ⅖MR² |
| rod (length L) about center | 112ML² |
| rod about one end | ⅓ML² |
Spinning skater Worked
Leverage is length
The same push gives more torque farther from the pivot: grab a door at the handle, not near the hinge, and push at right angles.
11Oscillations & Pendulums
- Period T
- time for one full cycle (s)
- Frequency f
- cycles per second, f = 1/T (Hz)
- Amplitude A
- largest distance from rest; restoring force F = −kx
Periods
Pendulum: small swings; mass and amplitude do not matter.
pendulum: T = 2π√(Lg)
spring: T = 2π√(mk)
Four times the string, twice the swing
T grows with √L: make a pendulum 4× longer and its period doubles.
Two periods Worked
Energy in SHM
- Ends: speed 0; PE and acceleration greatest. Center: speed and KE greatest.
- Huygens built the first pendulum clock (1656).
12Waves & Sound
- Mechanical wave
- needs a medium (sound, water, string)
- Electromagnetic wave
- needs none (light, radio)
- Wavelength λ
- crest to crest (m)
Wave speed
The medium sets v; the source sets f.
v = fλ
What waves do
- Reflect (echo), refract (bend entering a new medium), diffract (spread around edges).
- Interfere: in step add (constructive); out of step cancel (destructive).
- Two waves crossing back and forth make standing waves with nodes (still) and antinodes.
Concert A Worked
Standing waves
String fixed at both ends, n = 1, 2, 3, … Tube closed at one end: λ₁ = 4L.
λₙ = 2Ln, fₙ = nv2L
| Sound | Fact |
|---|---|
| speed | ≈ (331 + 0.6T) m/s; 343 m/s at 20 °C |
| pitch | set by frequency |
| loudness | set by amplitude; +10 dB = 10× the intensity |
| human range | about 20 to 20,000 Hz |
Light is a wave too
Young’s two-slit experiment (early 1800s): bright fringes where waves from the slits arrive in step.
d sin θ = mλ, Δy = λLd
Guitar string Worked
Red laser, two slits Worked
Doppler effect
Upper signs when moving toward each other. Doppler (1842); Buys Ballot tested it with horn players on a train (1845).
f′ = f v ± vov ∓ vs
Passing horn Worked
Coming close, pitch goes up
Waves bunch up ahead of a moving source (higher f) and spread out behind it (lower f).
13Fluids
Density and pressure
Pressure in pascals (N/m²) acts in every direction and grows with depth.
ρ = mV, P = FA
P = P₀ + ρgh
Ten meters down Worked
Pascal’s principle
- Pressure on a confined fluid passes undiminished to every part: F₁A₁ = F₂A₂.
At Pascal’s request, Périer carried a barometer up the Puy de Dôme (1648); the mercury fell with height.
Ten meters, one atmosphere
Each 10 m of water adds about one atmosphere of pressure.
Hydraulic lift Worked
Archimedes’ principle
Buoyant force = weight of the fluid pushed aside. Floats if ρobject < ρfluid; fraction under = ρobject ÷ ρfluid.
Fb = ρfluidVsubg
Rock under water Worked
Iceberg Worked
Moving fluids
Continuity, and Bernoulli’s equation (Hydrodynamica, 1738): along a flow, faster fluid has lower pressure.
A₁v₁ = A₂v₂
P + ½ρv² + ρgh = constant
Leaking tank Worked
Thumb on the hose Worked
14Heat & Thermodynamics
- Temperature
- average kinetic energy of the particles
- Heat Q
- energy that flows because of a temperature difference
- Specific heat c
- J to warm 1 kg by 1 °C
- Latent heat L
- J per kg to melt or boil, with no temperature change
| Law | Says |
|---|---|
| Zeroth | Two objects in balance with a third are in balance with each other. |
| First | ΔU = Q − W: energy is conserved (500 J in, 200 J of work out: ΔU = +300 J). |
| Second | Heat flows hot → cold on its own; no engine turns all heat into work; entropy grows. |
| Third | Absolute zero cannot be reached. |
Scales
TK = TC + 273.15
TF = 95TC + 32
EX25 °C = 298 K = 77 °F. Kelvin set the absolute scale in 1848.
Heat equations
Q = mcΔT, Q = mL
Boiling water for pasta Worked
Melting ice Worked
Mixing water Worked
| Transfer | How | Example |
|---|---|---|
| Conduction | contact, particle to particle | hot pan handle |
| Convection | warm fluid rises and circulates | boiling pot, sea breeze |
| Radiation | electromagnetic waves; no medium | sunlight, campfire |
Heat engines
The best possible engine: Carnot (1824).
e = WQH = 1 − QCQH
emax = 1 − TCTH (kelvins)
Best possible engine Worked
Ratios need kelvins
Use kelvins whenever temperatures are multiplied or divided (efficiency, gas laws). A change of 1 °C equals a change of 1 K.
15Electricity: Charge & Circuits
Electric charge
- Two kinds: + and −. Like charges repel; opposites attract.
- Charge is conserved and comes in whole multiples of e = 1.602 × 10⁻¹⁹ C.
- Objects charge by friction, contact or induction; conductors let charge move, insulators do not.
Coulomb’s law
k = 8.99 × 10⁹ N·m²/C². Coulomb measured it with a torsion balance (1785).
F = kq₁q₂r²
- Current I
- charge per second, q ÷ t (amperes)
- Voltage V
- energy per charge (J/C = volts)
- Resistance R
- opposition to current (ohms)
- Conventional current
- flows + to −; electrons drift the other way
Two charged spheres Worked
Ohm’s law and power
Ohm (1827). Resistance of a wire: R = ρL ÷ A.
V = IR
P = IV = I²R = V²R
Series circuit Worked
Series shares volts, parallel shares amps
In series the voltage divides and current is the same; in parallel the current divides and voltage is the same.
| Series | Parallel | |
|---|---|---|
| Current | same everywhere | splits among branches |
| Voltage | shared (drops add up) | same across each branch |
| Total R | R₁ + R₂ + … | 1R = 1R₁ + 1R₂ + … |
| One bulb out | all go out | others stay lit (house wiring) |
Parallel circuit Worked
16Magnetism
Right-hand grip
Thumb along the current, fingers curl the way B circles the wire. (Traditional.)
Magnetic force
On a current-carrying wire, and on a moving charge. B in tesla (T); the force is perpendicular to both B and the motion.
F = BIL sin θ
F = qvB sin θ
Magnets
- Every magnet has a north and a south pole; like poles repel, unlike attract. Cutting a magnet makes two smaller magnets.
- Earth is a giant magnet (Gilbert, De Magnete, 1600); a compass’s north end points toward geographic north.
Currents make magnetism
- Oersted saw a current turn a compass needle (1820).
- Straight wire: B = μ₀I2πr; coil (solenoid): B = μ₀nI.
Induction
- A changing magnetic field through a coil makes a voltage (Faraday, 1831): generators turn motion into electricity.
- Transformer: VsVp = NsNp.
Force on a wire Worked
Field near a wire Worked
Step-down transformer Worked
Go deeper
- Loops and solenoids, electromagnets, the motor effect, DC motors, and Faraday’s and Lenz’s laws: see the School Launch Magnetism and Induction sheet (Physics, Unit 10).
17Light & Optics
- Light
- an electromagnetic wave; c = 3.00 × 10⁸ m/s in vacuum
- Spectrum
- radio, microwave, infrared, visible (700–400 nm), ultraviolet, X-ray, gamma: rising frequency
- Index n
- n = c ÷ v: how much a material slows light
ROY G BIV
Red, orange, yellow, green, blue, indigo, violet: longest to shortest visible wavelength. (Traditional.)
Reflection
- Angle of reflection = angle of incidence, both from the normal.
- A flat mirror makes an upright, same-size, virtual image as far behind as the object is in front.
Refraction (Snell’s law)
Snell (1621); Ibn Sahl found it about 984. Past the critical angle θc, light reflects totally (optical fibers).
n₁ sin θ₁ = n₂ sin θ₂
sin θc = n₂n₁
Air into water Worked
Critical angle Worked
| Object (converging lens) | Image |
|---|---|
| beyond 2F | real, inverted, smaller (camera) |
| between F and 2F | real, inverted, larger (projector) |
| inside F | virtual, upright, larger (magnifier) |
| any (diverging lens) | virtual, upright, smaller |
Thin lens and mirror
f + for converging lenses and concave mirrors; di + real, − virtual; m − inverted.
1f = 1do + 1di
m = −dido = hiho
Camera-style image Worked
Real images flip
A real image is inverted and can fall on a screen; a virtual image is upright and only seen by looking through the lens or into the mirror.