Calculate linear momentum (p = m·v), relativistic momentum, impulse (J = F·Δt), kinetic energy (Ek = p²/2m), and 1D elastic/inelastic collisions with the free Momentum Calculator.
37,500 N·s • 27,651 lb·ft/s • Ek: 468,750 J • Force @ 0.1s: 375.0 kN • λ: 1.178 × 10⁻³⁸ m
345,732 ft·lbf
84,303 lbf
859.4 slug·ft/s
Relativistic scale
Quantum wavelength
90.0 km/h (55.9 mph)
In classical physics, engineering mechanics, and Newtonian kinematics, linear momentum (symbolized as \(\vec{p}\), derived from the Latin petere, meaning "to go towards") is a fundamental vector quantity that quantifies the total quantity of motion possessed by a mass in motion:
Linear momentum scales proportionally with both inertia and speed: \(\vec{p} = m \vec{v}\). A massive freight train moving slowly possesses equal momentum to a lightweight bullet moving at supersonic speed.
Momentum is intrinsically directional, possessing both magnitude and spatial orientation along the object's velocity vector, enabling vector summation in multi-dimensional collision analysis.
According to Noether's theorem, the law of conservation of linear momentum is a direct mathematical consequence of the continuous translational symmetry of space.
Summary of the foundational equations used in mechanics, automotive safety, and physics:
| Physical Metric | Mathematical Formula | Standard SI Units |
|---|---|---|
| Linear Momentum (\(p\)) | $$p = m \cdot v$$ | \(\text{kg}\cdot\text{m/s} \equiv \text{N}\cdot\text{s}\) |
| Kinetic Energy from Momentum (\(E_k\)) | $$E_k = \frac{p^2}{2m} = \frac{1}{2} m v^2$$ | \(\text{Joules (J)} \equiv \text{N}\cdot\text{m}\) |
| Impulse-Momentum Theorem (\(J\)) | $$J = \Delta p = F_{\text{avg}} \cdot \Delta t$$ | \(\text{N}\cdot\text{s}\) |
| Average Impact Force (\(F_{\text{avg}}\)) | $$F_{\text{avg}} = \frac{\Delta p}{\Delta t} = \frac{m(v_f - v_i)}{\Delta t}$$ | \(\text{Newtons (N)}\) |
| Relativistic Momentum (\(p_{\text{rel}}\)) | $$p_{\text{rel}} = \gamma m v = \frac{m v}{\sqrt{1 - v^2/c^2}}$$ | \(\text{kg}\cdot\text{m/s}\) |
| De Broglie Matter Wavelength (\(\lambda\)) | $$\lambda = \frac{h}{p} = \frac{h}{m v}$$ | \(\text{meters (m)}\) |
Choose between Standard Momentum (\(p = mv\)), Velocity Solver (\(v = p/m\)), Mass Solver (\(m = p/v\)), or 1D Collision Simulator.
Input mass in \(\text{kg}\), \(\text{g}\), \(\text{lbs}\), or \(\text{tonnes}\) and velocity in \(\text{m/s}\), \(\text{km/h}\), \(\text{ft/s}\), \(\text{mph}\), or \(c\).
Specify crash or stopping duration to evaluate peak deceleration and average impact force in \(\text{kN}\) and \(\text{lbf}\).
Inspect linear momentum, kinetic energy, de Broglie matter wavelength, relativistic factor, and live KaTeX derivations.
Why momentum and kinetic energy govern fundamentally different physical phenomena:
A vector quantity that measures resistance to stopping. Strictly conserved in all collisions (elastic and inelastic) regardless of internal friction or thermal energy conversion.
A scalar quantity that measures the mechanical work capacity. Scaled quadratically with velocity (\(v^2\)) and only conserved in perfectly elastic collisions.
Applying Newton's second law in its original momentum-rate formulation (\(F = \frac{dp}{dt}\)):
When bringing an object of momentum \(p\) to a complete stop (\(\Delta p = p\)), the required impulse is constant. Rearranging the impulse formula demonstrates that average impact force is inversely proportional to collision time:
Automotive safety engineers design front crumple zones and deploying airbags to lengthen impact duration from \(0.01\text{ s}\) (rigid barrier) to \(0.10\text{ s}\), slashing peak deceleration forces on passengers by \(90\%\).
Solve for momentum (\(p\)), mass (\(m\)), or velocity (\(v\)) with automatic unit conversions.
Simulate two-body elastic, inelastic, and partially inelastic collisions with coefficient of restitution (\(e\)).
Evaluates stopping time (\(\Delta t\)) to calculate average impact force in kiloNewtons and pounds-force.
Applies Einstein's Lorentz factor (\(\gamma\)) for near-light-speed particle physics calculations.
Computes quantum matter wavelength (\(\lambda = h/p\)) across macro and atomic scales.
Executes instantly on your device with zero server latency and total calculation privacy.
Prevents dimensional errors when converting between metric (\(\text{kg}\cdot\text{m/s}\), \(\text{N}\cdot\text{s}\)) and imperial (\(\text{lb}\cdot\text{ft/s}\), \(\text{slug}\cdot\text{ft/s}\)) momentum units.
Solves coupled simultaneous momentum and kinetic energy conservation equations for two colliding vehicles or billiard balls without tedious manual algebra.
How energy conservation dictates post-collision rebound velocities:
The general post-collision velocities for two bodies (\(m_1, m_2\)) with coefficient of restitution \(e = \frac{v_2' - v_1'}{v_1 - v_2}\) are:
Why classical momentum fails as velocity approaches the speed of light (\(c \approx 3 \times 10^8\text{ m/s}\)):
In special relativity, as \(v \to c\), the Lorentz factor \(\gamma = \frac{1}{\sqrt{1 - v^2/c^2}} \to \infty\). An infinite force would be required to accelerate any massive body to the speed of light, establishing \(c\) as the absolute cosmic speed limit.
Comparing translational motion with rotational orbital dynamics:
Translational quantity of motion along a straight-line vector. Changes only when an external net force applies an impulse (\(\vec{F} = \frac{d\vec{p}}{dt}\)).
Rotational quantity of motion about an axis. Governs gyroscopic stabilization, spinning figure skaters, and Keplerian orbital velocity variations (\(r_1 v_1 = r_2 v_2\)).
Wave-particle duality in quantum physics and solar radiation pressure:
Louis de Broglie postulated that every moving particle possesses an associated quantum wave packet with wavelength inversely proportional to its momentum:
Because macro objects have immense mass, their de Broglie wavelengths are imperceptibly small (\(\sim 10^{-38}\text{ m}\)), whereas high-speed electrons possess wavelengths comparable to atomic lattice spacings, powering transmission electron microscopes (TEM).
How continuous mass ejection drives aerospace propulsion in a vacuum:
In deep space with no external air to push against, a rocket accelerates by ejecting high-velocity combustion gases rearward. Conservation of momentum across differential mass elements (\(m \, dv = -v_e \, dm\)) yields the ideal rocket equation:
Why total system momentum equals the motion of its center of mass:
For any multi-particle system or complex vehicle collision, the total momentum equals total system mass multiplied by the velocity of the center of mass (\(\vec{v}_{\text{cm}}\)):
Because internal collision forces cancel out in pairs (Newton's third law), \(\vec{v}_{\text{cm}}\) remains completely unchanged before, during, and after any impact or explosive separation.
Classic experimental apparatus linking momentum conservation with potential energy:
When a high-speed bullet of mass \(m\) embeds into a suspended wooden block of mass \(M\), momentum is conserved during impact (\(m v_0 = (m + M) V\)), after which mechanical energy conserves as the pendulum swings up to vertical height \(h\):
Glancing impacts in subatomic physics and billiard mechanics:
In two-dimensional glancing collisions, vector momentum is conserved independently along orthogonal \(x\) and \(y\) axes:
In an elastic collision between two identical masses (\(m_1 = m_2\)) where one is initially stationary, the outgoing trajectory angles always form a right angle (\(\theta_1 + \theta_2 = 90^\circ\)), a property exploited by competitive pool players and particle physicists alike.
Comprehensive answers to common questions about momentum formulas, impulse calculations, kinetic energy relationships, and collision mechanics.