Home / Equation sheets / Physics 1 equation sheet AP Physics 1: Algebra-Based
The Physics 1 equation sheet, annotated for 2026 Print this sheet Transcribed from the equations table of the official AP Physics 1: Algebra-Based Course and Exam Description (Effective Fall 2024). College Board provides this sheet on both sections of the exam, so nothing here needs memorizing; knowing when each equation applies is the skill the exam actually tests. The geometry and math reference tables printed alongside the equations are not reproduced here.
For the units these equations belong to, see the Physics 1 course hub .
Constants and Conversion Factors G = 6.67 × 10 − 11 m 3 / ( kg ⋅ s 2 ) = 6.67 × 10 − 11 N ⋅ m 2 / kg 2 G = 6.67 \times 10^{-11}\ \text{m}^3/(\text{kg} \cdot \text{s}^2) = 6.67 \times 10^{-11}\ \text{N} \cdot \text{m}^2/\text{kg}^2 G = 6.67 × 1 0 − 11 m 3 / ( kg ⋅ s 2 ) = 6.67 × 1 0 − 11 N ⋅ m 2 / kg 2 Universal gravitational constant
1 atm = 1.0 × 10 5 N/m 2 = 1.0 × 10 5 Pa 1\ \text{atm} = 1.0 \times 10^5\ \text{N/m}^2 = 1.0 \times 10^5\ \text{Pa} 1 atm = 1.0 × 1 0 5 N/m 2 = 1.0 × 1 0 5 Pa 1 atmosphere of pressure
g = 9.8 m/s 2 g = 9.8\ \text{m/s}^2 g = 9.8 m/s 2 Magnitude of the acceleration due to gravity at Earth's surface
g = 9.8 N/kg g = 9.8\ \text{N/kg} g = 9.8 N/kg Magnitude of the gravitational field strength at Earth's surface
Mechanics and Fluids (translational) v x = v x 0 + a x t v_x = v_{x0} + a_x t v x = v x 0 + a x t x = x 0 + v x 0 t + 1 2 a x t 2 x = x_0 + v_{x0} t + \frac{1}{2} a_x t^2 x = x 0 + v x 0 t + 2 1 a x t 2 v x 2 = v x 0 2 + 2 a x ( x − x 0 ) v_x^2 = v_{x0}^2 + 2 a_x (x - x_0) v x 2 = v x 0 2 + 2 a x ( x − x 0 ) x ⃗ cm = ∑ m i x ⃗ i ∑ m i \vec{x}_{\text{cm}} = \frac{\sum m_i \vec{x}_i}{\sum m_i} x cm = ∑ m i ∑ m i x i a ⃗ sys = ∑ F ⃗ m sys = F ⃗ net m sys \vec{a}_{\text{sys}} = \frac{\sum \vec{F}}{m_{\text{sys}}} = \frac{\vec{F}_{\text{net}}}{m_{\text{sys}}} a sys = m sys ∑ F = m sys F net ∣ F ⃗ g ∣ = G m 1 m 2 r 2 \left| \vec{F}_g \right| = \frac{G m_1 m_2}{r^2} F g = r 2 G m 1 m 2 ∣ F ⃗ f ∣ ≤ ∣ μ F ⃗ N ∣ \left| \vec{F}_f \right| \leq \left| \mu \vec{F}_N \right| F f ≤ μ F N F ⃗ s = − k Δ x ⃗ \vec{F}_s = -k \Delta \vec{x} F s = − k Δ x a c = v 2 r a_c = \frac{v^2}{r} a c = r v 2 K = 1 2 m v 2 K = \frac{1}{2} m v^2 K = 2 1 m v 2 W = F ∥ d = F d cos θ W = F_{\parallel} d = F d \cos\theta W = F ∥ d = F d cos θ Δ K = ∑ W i = ∑ F ∥ , i d i \Delta K = \sum W_i = \sum F_{\parallel, i}\, d_i Δ K = ∑ W i = ∑ F ∥ , i d i U s = 1 2 k ( Δ x ) 2 U_s = \frac{1}{2} k (\Delta x)^2 U s = 2 1 k ( Δ x ) 2 U G = − G m 1 m 2 r U_G = -\frac{G m_1 m_2}{r} U G = − r G m 1 m 2 Δ U g = m g Δ y \Delta U_g = m g \Delta y Δ U g = m g Δ y P avg = W Δ t = Δ E Δ t P_{\text{avg}} = \frac{W}{\Delta t} = \frac{\Delta E}{\Delta t} P avg = Δ t W = Δ t Δ E P inst = F ∥ v = F v cos θ P_{\text{inst}} = F_{\parallel} v = F v \cos\theta P inst = F ∥ v = F v cos θ p ⃗ = m v ⃗ \vec{p} = m \vec{v} p = m v F ⃗ net = Δ p ⃗ Δ t = m Δ v ⃗ Δ t = m a ⃗ \vec{F}_{\text{net}} = \frac{\Delta \vec{p}}{\Delta t} = m \frac{\Delta \vec{v}}{\Delta t} = m \vec{a} F net = Δ t Δ p = m Δ t Δ v = m a J ⃗ = F ⃗ avg Δ t = Δ p ⃗ \vec{J} = \vec{F}_{\text{avg}} \Delta t = \Delta \vec{p} J = F avg Δ t = Δ p v ⃗ cm = ∑ p ⃗ i ∑ m i = ∑ m i v ⃗ i ∑ m i \vec{v}_{\text{cm}} = \frac{\sum \vec{p}_i}{\sum m_i} = \frac{\sum m_i \vec{v}_i}{\sum m_i} v cm = ∑ m i ∑ p i = ∑ m i ∑ m i v i Mechanics and Fluids (rotational, oscillations, and fluids) ω = ω 0 + α t \omega = \omega_0 + \alpha t ω = ω 0 + α t θ = θ 0 + ω 0 t + 1 2 α t 2 \theta = \theta_0 + \omega_0 t + \frac{1}{2} \alpha t^2 θ = θ 0 + ω 0 t + 2 1 α t 2 ω 2 = ω 0 2 + 2 α ( θ − θ 0 ) \omega^2 = \omega_0^2 + 2 \alpha (\theta - \theta_0) ω 2 = ω 0 2 + 2 α ( θ − θ 0 ) a T = r α a_T = r \alpha a T = r α τ = r ⊥ F = r F sin θ \tau = r_{\perp} F = r F \sin\theta τ = r ⊥ F = r F sin θ I = ∑ m i r i 2 I = \sum m_i r_i^2 I = ∑ m i r i 2 I ′ = I cm + M d 2 I' = I_{\text{cm}} + M d^2 I ′ = I cm + M d 2 α sys = ∑ τ I sys = τ net I sys \alpha_{\text{sys}} = \frac{\sum \tau}{I_{\text{sys}}} = \frac{\tau_{\text{net}}}{I_{\text{sys}}} α sys = I sys ∑ τ = I sys τ net K = 1 2 I ω 2 K = \frac{1}{2} I \omega^2 K = 2 1 I ω 2 W = τ Δ θ W = \tau \Delta\theta W = τ Δ θ L = r m v sin θ L = r m v \sin\theta L = r m v sin θ Δ L = τ Δ t \Delta L = \tau \Delta t Δ L = τ Δ t Δ x cm = r Δ θ \Delta x_{\text{cm}} = r \Delta\theta Δ x cm = r Δ θ T s = 2 π m k T_s = 2\pi \sqrt{\frac{m}{k}} T s = 2 π k m T p = 2 π ℓ g T_p = 2\pi \sqrt{\frac{\ell}{g}} T p = 2 π g ℓ x = A cos ( 2 π f t ) x = A \cos(2\pi f t) x = A cos ( 2 π f t ) x = A sin ( 2 π f t ) x = A \sin(2\pi f t) x = A sin ( 2 π f t ) ρ = m V \rho = \frac{m}{V} ρ = V m P = F ⊥ A P = \frac{F_{\perp}}{A} P = A F ⊥ P = P 0 + ρ g h P = P_0 + \rho g h P = P 0 + ρ g h P gauge = ρ g h P_{\text{gauge}} = \rho g h P gauge = ρ g h F b = ρ V g F_b = \rho V g F b = ρ V g A 1 v 1 = A 2 v 2 A_1 v_1 = A_2 v_2 A 1 v 1 = A 2 v 2 P 1 + ρ g y 1 + 1 2 ρ v 1 2 = P 2 + ρ g y 2 + 1 2 ρ v 2 2 P_1 + \rho g y_1 + \frac{1}{2} \rho v_1^2 = P_2 + \rho g y_2 + \frac{1}{2} \rho v_2^2 P 1 + ρ g y 1 + 2 1 ρ v 1 2 = P 2 + ρ g y 2 + 2 1 ρ v 2 2 The other sheets