AP Physics Formula Sheet — Physics 1, Physics 2 and C Key Equations
Every key equation for AP Physics 1 and AP Physics 2 in one place, organised by topic, with a plain-English note on when to reach for each one. A few extra equations needed for AP Physics C are included and clearly marked [C]. Good news: the College Board hands you an equation sheet inside the exam itself — so you do not need to memorise these by rote. What scores marks is recognising which equation fits a situation and what each symbol means, and that is exactly what this page trains.
Key Constants
Speed of light in a vacuum c = 3.00 × 108 m/s
Universal gravitational constant G = 6.67 × 10−11 N m2/kg2
Coulomb’s law constant k = 8.99 × 109 N m2/C2
Elementary charge e = 1.60 × 10−19 C
Planck’s constant h = 6.63 × 10−34 J s
Electron mass me = 9.11 × 10−31 kg
Proton mass mp = 1.67 × 10−27 kg
Permittivity of free space ε0 = 8.85 × 10−12 C2/(N m2)
Boltzmann constant kB = 1.38 × 10−23 J/K
Gas constant R = 8.31 J/(mol K)
Kinematics & Dynamics (Physics 1)
| Equation | What it is / When to use it |
|---|---|
| v = v0 + at | Final velocity after time t under constant acceleration. The first of the three big kinematics equations. |
| x = x0 + v0t + ½at2 | Position after time t under constant acceleration. Use when time is known or asked for and final velocity is not. |
| v2 = v02 + 2aΔx | Links velocities and displacement with no time involved. The go-to equation when a problem never mentions time. |
| Fnet = ma | Newton’s second law: add all force vectors first, then divide by mass. Almost every dynamics problem starts here. |
| f ≤ μN | Friction: kinetic friction equals μkN; static friction adjusts up to a maximum of μsN. It is an inequality, not always an equality. |
| ac = v2/r, Fc = mv2/r | Centripetal acceleration and the net inward force needed for circular motion. Centripetal force is a role played by tension, gravity or friction — never an extra force to add. |
| τ = rF sin θ | Torque: the turning effect of a force. Maximum when the force is perpendicular to the lever arm (sin θ = 1), zero when it points along it. |
| Δθ = ω0t + ½αt2, ω = ω0 + αt, τnet = Iα | Rotational analogues of the linear equations: θ (angle) → x, ω (angular velocity) → v, α (angular acceleration) → a, and torque plays the role of force. If you know the linear version, you know the rotational one. |
| I = Σ miri2 (e.g. hoop I = MR2, solid disk I = ½MR2, rod about centre I = (1/12)ML2) | Moment of inertia: rotational inertia. Mass far from the axis counts much more than mass near it, because r is squared. |
| L = Iω = r p sin θ | Angular momentum, for a spinning object (Iω) or a moving particle (r p sin θ). Conserved whenever the net external torque is zero. |
| KErot = ½Iω2 | Rotational kinetic energy. Rolling objects carry both this and ½mv2 — forgetting one of them is a classic lost mark. |
Energy, Work & Momentum (Physics 1)
| Equation | What it is / When to use it |
|---|---|
| W = Fd cos θ | Work done by a constant force: only the component of force along the displacement does work. Work is the area under a force–position graph. |
| KE = ½mv2 | Translational kinetic energy. Doubling speed quadruples it. |
| ΔKE = Wnet | Work–energy theorem: the net work done on an object equals its change in kinetic energy. Often faster than Newton’s laws when only speeds matter. |
| GPE = mgh (near Earth’s surface) | Gravitational potential energy. Only the change in height matters; you may set h = 0 wherever is convenient. |
| Fs = −kx, PEs = ½kx2 | Hooke’s law and spring potential energy. The minus sign means the force always points back towards equilibrium. |
| P = W/t = Fv | Power: the rate of doing work or transferring energy, in watts. P = Fv applies when a force acts at constant velocity. |
| p = mv | Linear momentum, a vector. It depends on velocity, not speed alone. |
| J = Δp = FΔt | Impulse equals change in momentum, and equals the area under a force–time graph. Explains why airbags help: same Δp, longer Δt, smaller F. |
| m1v1 + m2v2 = constant (no external impulse) | Conservation of momentum: holds in every collision and explosion, elastic or not, as long as external impulses are negligible. |
| Elastic collision: KE is also conserved, and v1 − v2 = −(v1′ − v2′) | In an elastic collision both momentum and kinetic energy survive, and the relative speed of approach equals the relative speed of separation. |
| Perfectly inelastic collision: objects stick, only momentum is conserved | Maximum kinetic energy is lost when the objects move off together with a single shared velocity. Never apply KE conservation here. |
| Tspring = 2π√(m/k) | Period of a mass on a spring. Depends on mass and stiffness only — not on amplitude or gravity. |
| Tpendulum = 2π√(L/g) | Period of a simple pendulum for small swings. Depends on length and g only — not on the bob’s mass. |
| x(t) = A cos(2πft), f = 1/T | Position in simple harmonic motion. Velocity is greatest at equilibrium, acceleration is greatest (and directed back to equilibrium) at the extremes. |
Fluids & Thermodynamics (Physics 2)
| Equation | What it is / When to use it |
|---|---|
| ρ = m/V | Density: mass per unit volume. The property that decides floating, sinking and buoyant force. |
| P = F/A | Pressure: force per unit area, in pascals. A fluid pushes equally in all directions at a given depth. |
| P = P0 + ρgh | Pressure at depth h in a static fluid: surface pressure plus the weight of the fluid column above. |
| Fb = ρfluidVdisplacedg | Buoyant force (Archimedes’ principle): it equals the weight of displaced fluid. Use the submerged volume, not the object’s total volume. |
| A1v1 = A2v2 | Continuity equation: for an incompressible fluid, where the pipe narrows the flow speeds up. |
| P + ρgy + ½ρv2 = constant | Bernoulli’s equation along a streamline: where a fluid moves faster, its pressure is lower (for steady, incompressible, low-viscosity flow). |
| PV = nRT | Ideal gas law, with T in kelvin. Links pressure, volume, amount of gas and absolute temperature. |
| Average KE per molecule = (3/2)kBT | Kinetic theory: absolute temperature is a direct measure of the average kinetic energy of the molecules. |
| ΔU = Q + W | First law of thermodynamics. AP sign convention: W is the work done ON the gas, so compressing a gas makes W positive; Q is positive when heat flows into the gas. (Many textbooks write ΔU = Q − W with W done BY the gas — same physics, opposite sign for W.) |
| Efficiency = Wout/Qh = 1 − Qc/Qh | Heat engine efficiency: useful work out divided by heat taken from the hot reservoir. |
| Carnot efficiency = 1 − Tc/Th | The maximum possible efficiency between two temperatures (kelvin). No real engine between the same reservoirs can beat it. |
Electricity & Magnetism (Physics 2, plus Physics 1 circuits)
| Equation | What it is / When to use it |
|---|---|
| F = kq1q2/r2 | Coulomb’s law: the force between two point charges. Like charges repel, unlike charges attract, and the force falls with the square of the separation. |
| E = F/q, and for a point charge E = kq/r2 | Electric field strength: force per unit positive test charge. Field lines point away from positive charges and towards negative ones. |
| V = kq/r | Electric potential of a point charge: a scalar, so potentials from several charges simply add (no directions to resolve). |
| U = qV, ΔU = qΔV | Electric potential energy of a charge in a potential. A charge released in a field trades this energy for kinetic energy. |
| C = Q/V | Capacitance: charge stored per volt. It depends on the capacitor’s geometry, not on Q or V themselves. |
| C = ε0A/d | Parallel-plate capacitance: bigger plates or a smaller gap store more. Inserting a dielectric multiplies C by the dielectric constant κ. |
| UC = ½QV = ½CV2 = Q2/2C | Energy stored in a capacitor. The factor ½ appears because the voltage grows as the capacitor charges. |
| I = ΔQ/Δt | Electric current: rate of flow of charge, in amperes. Conventional current flows from + to − outside the battery. |
| R = ρL/A | Resistance of a uniform wire: longer and thinner means more resistance; ρ is the resistivity of the material. |
| V = IR | Ohm’s law. Applies to each component and to whole circuits; combine with the power forms below. |
| P = IV = I2R = V2/R | Electrical power dissipated. Pick the form using the quantities that stay constant in the question. |
| Series: Req = R1 + R2 + …; Parallel: 1/Req = 1/R1 + 1/R2 + … | Series resistors share the same current and resistances add (equivalent is bigger than the biggest). Parallel resistors share the same voltage and the equivalent is smaller than the smallest. |
| Capacitors: series 1/Ceq = 1/C1 + 1/C2 + …; parallel Ceq = C1 + C2 + … | Capacitor rules are the reverse of the resistor rules: parallel capacitors add, series capacitors combine reciprocally. |
| F = qvB sin θ | Magnetic force on a moving charge. Zero if the charge moves parallel to the field; direction from the right-hand rule (reverse it for electrons). |
| F = BIL sin θ | Magnetic force on a current-carrying wire of length L in a field. Maximum when the wire is perpendicular to the field. |
| B = μ0I/(2πr) | Magnetic field around a long straight wire (μ0 = 4π × 10−7 T m/A). Circles the wire; use the right-hand grip rule for direction. |
| Φ = BA cos θ | Magnetic flux through a loop: field × area × the cosine of the angle between the field and the loop’s normal (perpendicular) direction. |
| EMF = −N ΔΦ/Δt | Faraday’s law: a changing magnetic flux induces an EMF. The minus sign is Lenz’s law — the induced effect opposes the change that caused it. |
Waves, Sound & Optics (Physics 1 + 2)
| Equation | What it is / When to use it |
|---|---|
| v = fλ | Wave speed = frequency × wavelength. True for every wave; the medium sets the speed, the source sets the frequency. |
| String fixed at both ends: λn = 2L/n, fn = nv/2L | Standing waves on a string: all harmonics (n = 1, 2, 3, …) are present. A node sits at each fixed end. |
| Open pipe (both ends open): λn = 2L/n | All harmonics again, with an antinode at each open end — same maths as the string. |
| Closed pipe (one end closed): λn = 4L/n for odd n only | Only odd harmonics (n = 1, 3, 5, …) fit, because the closed end must be a node and the open end an antinode. |
| n1 sin θ1 = n2 sin θ2 | Snell’s law: how light bends at a boundary. Entering a denser medium (bigger n) bends it towards the normal, and its speed becomes v = c/n. |
| 1/f = 1/do + 1/di | Lens/mirror equation: links focal length, object distance and image distance. Real images form on the same side light reaches (positive di). |
| m = −di/do = hi/ho | Magnification: image size over object size. A negative m means the image is inverted; |m| > 1 means enlarged. |
| d sin θ = mλ | Double-slit interference maxima: the path difference for a bright fringe is a whole number of wavelengths (m = 0, 1, 2, …). |
| x = mλL/d | Small-angle form: position of the m-th bright fringe on a screen a distance L away, where d is the slit separation. Fringe spacing Δx = λL/d. |
| Diffraction grating: d sin θ = mλ, with d = 1/(lines per metre) | Same form as the double slit, but with many slits the maxima are much sharper and brighter. Single-slit dark fringes instead sit at a sin θ = mλ (a = slit width, m ≠ 0). |
Modern Physics (Physics 2)
| Equation | What it is / When to use it |
|---|---|
| E = hf | Photon energy: light comes in packets whose energy depends only on frequency. Also E = hc/λ when you are given wavelength. |
| KEmax = hf − φ | Photoelectric equation: photon energy minus the work function φ (energy needed to escape the metal) leaves the fastest electrons’ kinetic energy. Below the threshold frequency f0 = φ/h, nothing is emitted at all. |
| λ = h/p | de Broglie wavelength: every moving particle has wave behaviour. It only becomes noticeable for very small masses and momenta. |
| En = −13.6/n2 eV | Bohr model energy levels for hydrogen. A transition’s photon energy is the difference between levels: ΔE = Einitial − Efinal (emitted) or the reverse (absorbed). |
| rn = n2a0, with a0 = 5.29 × 10−11 m | Bohr orbit radii grow with n2: the electron’s allowed orbits spread out quickly as the energy level rises. |
| E = mc2 | Mass–energy equivalence. The binding energy of a nucleus equals its mass defect (mass of separate nucleons minus mass of the nucleus) multiplied by c2; that loss of mass is why fused/fissioned nuclei release energy. |
AP Physics C Additions [C]
| Equation | What it is / When to use it |
|---|---|
| [C] W = ∫ F dx | Work by a variable force is the integral of force over displacement — this is why spring work comes out as ½kx2. Rotational version: W = ∫ τ dθ, and P = τω. |
| [C] τ = dL/dt, I = ∫ r2 dm | Rotational dynamics with calculus: net torque is the rate of change of angular momentum, and moment of inertia for a continuous body is built up by integration. |
| [C] Gauss’s law: ΦE = Qenclosed/ε0 | The electric flux through any closed surface depends only on the charge inside it. Use symmetry (spheres, cylinders, planes) to pull E out of the flux integral and find fields efficiently. |
| [C] Ampère’s law: ∫ B · dl = μ0Ienclosed | The magnetic equivalent of Gauss’s law: the circulation of B around a closed loop equals μ0 times the current passing through the loop. Best for wires, solenoids and toroids. |
| [C] RC circuits: charging q = Q(1 − e−t/RC), discharging q = Qe−t/RC, time constant τ = RC | Capacitor charge and current change exponentially, never linearly. After one time constant the quantity has moved about 63% of the way (charging) or fallen to about 37% (discharging). |
| [C] LC oscillation: ω = 1/√(LC), T = 2π√(LC) | An inductor–capacitor circuit oscillates as energy swaps between the capacitor’s electric field and the inductor’s magnetic field — the electrical analogue of a mass on a spring. |
| [C] Maxwell’s equations (idea) | Changing electric fields create magnetic fields just as changing magnetic fields create electric fields; together the four equations predict self-propagating electromagnetic waves travelling at c = 1/√(ε0μ0). |
Keep Going with Physics on QuaidianPoint
Work through free practice questions on the Physics hub, and keep the matching formula sheet for your course open beside it:
This page is an original revision aid written for QuaidianPoint. It is not affiliated with, endorsed by, or produced by the College Board, which owns the AP name and publishes the official AP Physics course and exam descriptions.
