Mechanics
Impulse
Force times time — change in momentum, the secret behind airbags and follow-through
Impulse is the change in momentum of an object — equal to the force applied times the duration of application — J = F·Δt = Δp. It explains why airbags, crumple zones, and parkour rolls reduce injury (extending Δt reduces peak force for the same Δp). Why pitchers follow through on throws (longer contact time = more impulse = more momentum). And why bullets penetrate (very short contact time = very large peak force).
- DefinitionJ = F·Δt = Δp
- UnitsN·s = kg·m/s (same as momentum)
- From Newton's 2ndF = dp/dt → ∫F dt = Δp
- Average forceF_avg = Δp/Δt
- Vector quantityDirection matters
- Key insightSame Δp can come from many F-vs-time profiles
Interactive visualization
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Watch the 60-second explainer
A condensed visual walkthrough — narrated, captioned, under a minute.
Definition
Impulse is the change in momentum of an object:
J = Δp = m·Δv
From Newton's second law (F = dp/dt), integrating over time gives:
J = ∫F dt = Δp
For constant force:
J = F·Δt
Units: N·s, equivalent to kg·m/s (the same as momentum). Impulse is a vector — direction matters.
The key insight — Δp = F·Δt
Two ways to give an object the same momentum change:
- Big force, short time. Hammer driving a nail. Bullet penetrating wood. Rear-ender at 30 mph into a brick wall.
- Small force, long time. Pushing a stalled car. Slow steady cooking with low heat. Decelerating a moving vehicle gradually with brakes.
Both have the same impulse. But the first hurts a lot; the second doesn't. Why? Peak FORCE matters for damage, not impulse.
Why airbags work — extending Δt
In a 30 mph head-on collision (Δv ≈ 13.4 m/s), your 70 kg body needs Δp = 70 × 13.4 = 938 kg·m/s of decelerating impulse.
| Scenario | Δt | F_avg | Outcome |
|---|---|---|---|
| Head into windshield (no belt, no airbag) | ~1 ms | 938,000 N (~96,000 kg force) | Lethal trauma |
| Head/torso into seatbelt only | ~100 ms | 9,380 N (~960 kg force) | Bruising, possible chest injury |
| Head/torso into airbag + seatbelt | ~300 ms | 3,127 N (~320 kg force) | Mild discomfort, survivable |
| Same crash with high-end safety + crumple | ~500+ ms | ~1,876 N | Often walk away |
By extending Δt by 300×, peak force drops by 300×. Your body can absorb ~6,000 N of localized force; ~1,000,000 N rips it apart. This factor of 300 is the difference between life and death.
Other impulse applications
| Situation | Why impulse matters |
|---|---|
| Pitcher's follow-through | Extends contact time → more impulse → faster pitch |
| Tennis serve | Racquet drags through ball; longer contact = more energy transfer |
| Catching a ball | Pull hand back as ball arrives → extends Δt → reduces hand pain |
| Diver entering pool | Splayed entry: short Δt, painful. Streamlined entry: long Δt through water resistance, painless |
| Karate chop | Hard board, short Δt — high peak F → board breaks. Soft pillow doesn't break: long Δt, low F |
| Golf club head | Stiff face for short contact (more transmitted F); soft face deforms (longer Δt, more energy) |
| Bicycle helmet | Foam crumples on impact — extends Δt for the head, reduces peak force |
| Bungee jump | Long elastic cord stretches → long Δt of deceleration → comfortable landing |
Rocket impulse and "specific impulse"
Rocket engines are characterized by specific impulse (Isp) — impulse per unit mass of propellant:
Isp = J / (m_propellant · g) = v_exhaust / g
Higher Isp means more momentum per kilogram of fuel — fewer trips to refuel.
| Engine type | Isp | v_exhaust |
|---|---|---|
| Solid rocket boosters | ~250 s | ~2,500 m/s |
| Liquid hydrogen/oxygen | ~450 s | ~4,400 m/s |
| Ion thruster (Xenon) | ~3,000 s | ~30,000 m/s |
| VASIMR (concept) | ~5,000-30,000 s | ~50-300 km/s |
| Photonic (theoretical) | ~30 million s | c (3 × 10⁸ m/s) |
JavaScript — impulse and force-time
// Average force from impulse and time
function avgForce(deltaP, deltaT) {
return deltaP / deltaT;
}
// Crash analysis
function crashForce(mass, vBefore, vAfter, contactTime) {
const deltaP = mass * (vBefore - vAfter); // momentum change
return avgForce(deltaP, contactTime);
}
// 70 kg passenger, 30 mph (13.4 m/s) → 0
console.log(`No airbag (1 ms): ${crashForce(70, 13.4, 0, 0.001).toFixed(0)} N`);
console.log(`With airbag (100 ms): ${crashForce(70, 13.4, 0, 0.1).toFixed(0)} N`);
console.log(`With airbag + crumple (300 ms): ${crashForce(70, 13.4, 0, 0.3).toFixed(0)} N`);
// Numerical integration of force over time → impulse
function impulse(forceArray, dt) {
// Trapezoidal rule on F(t)
let total = 0;
for (let i = 1; i < forceArray.length; i++) {
total += 0.5 * (forceArray[i-1] + forceArray[i]) * dt;
}
return total;
}
// Example: rectangular force profile (constant force F over time T)
function rectangularImpulse(F, T, dt = 0.001) {
const N = Math.floor(T / dt);
return impulse(Array(N).fill(F), dt);
}
console.log(rectangularImpulse(100, 0.5)); // 50 N·s
// Specific impulse from exhaust velocity
function specificImpulse(vExhaust, g = 9.81) {
return vExhaust / g;
}
console.log(`Solid rocket Isp: ${specificImpulse(2500).toFixed(0)} s`);
console.log(`Hydrolox Isp: ${specificImpulse(4400).toFixed(0)} s`);
Where impulse shows up
- Auto safety. Airbags, crumple zones, seatbelts — all extend Δt to reduce peak force. Federal Motor Vehicle Safety Standards specify maximum allowable forces.
- Sports. Follow-through in throwing/hitting; cushion landing in catching; soft landing in jumps; bat/racquet design.
- Helmets and protective gear. Foam padding extends impact time. Football helmets have multi-layer foam for various impact severities.
- Rocket science. Specific impulse (Isp) is the figure of merit — high Isp means efficient propellant use.
- Particle physics. Detector design uses controlled impulse-energy relationships to identify particles.
- Construction safety. Catch nets, harnesses, bungee cords for fall protection — all designed to extend Δt.
- Hammer/hammer-anvil. Brittle materials snap from short, sharp impulses; ductile materials deform from longer, gentler impulses.
Common mistakes
- Confusing impulse with force. Impulse is total momentum change (a vector quantity). Force is rate of momentum change (also a vector). They have different units (N·s vs N).
- Ignoring Δt's role in safety. Big airbags work not by being soft but by extending Δt by orders of magnitude.
- Using F·Δt when force varies. If force changes over time, J = ∫F dt (the integral). Average force F_avg = Δp/Δt is correct, but using peak force times duration overstates impulse.
- Treating impulse and energy as interchangeable. They're different. A 1 kg ball at 10 m/s has p = 10 kg·m/s and KE = 50 J. Doubling speed: p = 20, KE = 200 (4×). Different scaling.
- Forgetting impulse is a vector. Impulse from a force has the SAME direction as the force. Tackling at an angle gives angular impulse — affects spin, not just translation.
- Confusing specific impulse with regular impulse. Specific impulse is a measure of rocket fuel efficiency (s). Regular impulse is total momentum change (N·s). Different quantities.
Frequently asked questions
Why does extending impact time reduce force?
Impulse J = F·Δt = Δp (momentum change). For a given Δp (the velocity change you need to absorb), increasing Δt reduces the AVERAGE force F_avg = Δp/Δt. Airbags, crumple zones, and parkour rolls all extend the deceleration time, dropping peak force on the body. This is why a 30 mph car crash with airbag is survivable, but a 30 mph crash into a brick wall (instantaneous Δt) is fatal — same Δp, very different F_avg.
How is impulse the integral of force over time?
From Newton's second law F = dp/dt, integrating both sides over time — ∫F dt = Δp. The integral of force vs time is the impulse. For constant force, J = F·Δt. For variable force (real impacts), J equals the area under the force-time curve. Engineers measure this in crash tests with high-speed cameras and force sensors.
Why do pitchers follow through?
To extend the contact time between hand and ball, increasing impulse. F·Δt = Δp — for a given hand force, more time of contact = more momentum imparted = faster pitch. Same idea in tennis (racquet meeting ball), golf (club face), and boxing (punch follow-through to add momentum).
How does this differ from work-energy theorem?
Work-energy gives change in KINETIC ENERGY (W = ΔKE = ½mv² − ½mv₀²). Impulse gives change in MOMENTUM (J = Δp = mΔv). Both are integrals of force, but over different things — work over distance, impulse over time. Impulse is a vector; energy is a scalar. They give complementary info — impulse tells you final velocity vector; energy tells you final speed.
How do we measure impulse in real impacts?
With force sensors and high-speed cameras. Auto crash tests use accelerometers in dummies and force sensors in walls/airbags to measure F(t). The integral over the impact time is impulse. Sports science measures bat-ball or club-ball contact via force plates (~1 ms contact time) and high-speed video (~10,000 fps). Deformation, sound, and heat are byproducts.
What about explosions and jet thrust?
Explosions deliver large impulse over very short time — high peak force. Jet engines deliver smaller impulse continuously. Same total momentum change can come from either. Rockets have continuous F (dp/dt = thrust); explosions have brief intense F. The Saturn V rocket gave a 2300 ton spacecraft a Δv of ~3.5 km/s in ~150 s of burn time = enormous total impulse spread over a long burn.
How do safety devices use impulse?
Airbags inflate in ~30 ms, providing a soft cushion. Without airbag — head impacts dashboard in ~1 ms with peak force ~10,000 N. With airbag — head decelerates over ~50 ms with peak force ~500 N. Same total impulse (same momentum change), but 20× lower force. Helmets, padded floors, climbing harnesses all use the same principle — extend Δt to reduce peak F.