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

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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.

ScenarioΔtF_avgOutcome
Head into windshield (no belt, no airbag)~1 ms938,000 N (~96,000 kg force)Lethal trauma
Head/torso into seatbelt only~100 ms9,380 N (~960 kg force)Bruising, possible chest injury
Head/torso into airbag + seatbelt~300 ms3,127 N (~320 kg force)Mild discomfort, survivable
Same crash with high-end safety + crumple~500+ ms~1,876 NOften 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

SituationWhy impulse matters
Pitcher's follow-throughExtends contact time → more impulse → faster pitch
Tennis serveRacquet drags through ball; longer contact = more energy transfer
Catching a ballPull hand back as ball arrives → extends Δt → reduces hand pain
Diver entering poolSplayed entry: short Δt, painful. Streamlined entry: long Δt through water resistance, painless
Karate chopHard board, short Δt — high peak F → board breaks. Soft pillow doesn't break: long Δt, low F
Golf club headStiff face for short contact (more transmitted F); soft face deforms (longer Δt, more energy)
Bicycle helmetFoam crumples on impact — extends Δt for the head, reduces peak force
Bungee jumpLong 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 typeIspv_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 sc (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.