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Defining Linear Momentum

Momentum is "quantity of motion."

p=mv\vec{p} = m\vec{v}

Units: kg - m/s

Properties:

  • Vector quantity (direction = velocity direction)
  • Mass × velocity
  • Frame-dependent

Defining Impulse

Impulse is change in momentum.

J=Δp=pfpi\vec{J} = \Delta \vec{p} = \vec{p}_f - \vec{p}_i

p=mvp = mv

Momentum formula.

p=mv\vec{p} = m\vec{v}

J=Fdt=ΔpJ = \int F dt = \Delta p

J = ∫ F dt = Deltap:

Impulse-momentum theorem (integral form).

J=titfF(t)dt=Δp=mvfmvi\vec{J} = \int_{t_i}^{t_f} \vec{F}(t) \, dt = \Delta \vec{p} = m\vec{v}_f - m\vec{v}_i

Physical meaning:

  • Force applied over time changes momentum
  • Impulse equals area under force-time graph

J=FavgΔtJ = F_{avg} \Delta t

J = F_avg Deltat:

Average force form.

J=FavgΔt\vec{J} = \vec{F}_{avg} \Delta t

Where Favg=1ΔtFdt\vec{F}_{avg} = \frac{1}{\Delta t}\int \vec{F} \, dt

Σpinitial=Σpfinal\Sigma p_{initial} = \Sigma p_{final} (For Isolated System)

Sigmap_initial = Sigmap_final (for isolated system):

Total momentum conserved in isolated system.

ptotal,i=ptotal,f\vec{p}_{total,i} = \vec{p}_{total,f}

imivi,i=imivi,f\sum_{i} m_i \vec{v}_{i,i} = \sum_{i} m_i \vec{v}_{i,f}

When applicable:

  • Net external force = 0
  • Or collision time very short (internal >> external forces)

Analyzing Elastic, Inelastic, And Perfectly Inelastic Collisions

Elastic: Both momentum and kinetic energy conserved pi=pf,Ki=Kf\vec{p}_i = \vec{p}_f, \quad K_i = K_f

Inelastic: Momentum conserved, kinetic energy NOT conserved pi=pf,Kf<Ki\vec{p}_i = \vec{p}_f, \quad K_f < K_i

Perfectly inelastic: Objects stick together, maximum KE loss pi=pf,vf=pim1+m2\vec{p}_i = \vec{p}_f, \quad \vec{v}_f = \frac{\vec{p}_i}{m_1 + m_2}

Coefficient Of Restitution

Measure of "bounciness" of collision.

e=vseparationvapproach=v2fv1fv1iv2ie = \frac{v_{separation}}{v_{approach}} = \frac{v_{2f} - v_{1f}}{v_{1i} - v_{2i}}

Values:

  • e = 1: perfectly elastic
  • 0 < e < 1: inelastic
  • e = 0: perfectly inelastic (objects stick)

Conservation Of Kinetic Energy (Elastic Only)

Only elastic collisions conserve kinetic energy.

Ki=KfK_i = K_f

12m1v1i2+12m2v2i2=12m1v1f2+12m2v2f2\frac{1}{2}m_1v_{1i}^2 + \frac{1}{2}m_2v_{2i}^2 = \frac{1}{2}m_1v_{1f}^2 + \frac{1}{2}m_2v_{2f}^2

Inelastic: Kf<KiK_f < K_i (energy converted to heat, deformation, sound, etc.)

Velocity And Acceleration Of Center Of Mass

Center of mass moves as if total mass concentrated there.

vcm=ptotalM=mivimi\vec{v}_{cm} = \frac{\vec{p}_{total}}{M} = \frac{\sum m_i \vec{v}_i}{\sum m_i}

acm=Fnet,extM\vec{a}_{cm} = \frac{\vec{F}_{net,ext}}{M}

ΣFext=Macm\Sigma F_{ext} = Ma_{cm}

SigmaF_ext = Ma_cm:

Newton's Second Law for system.

Fnet,ext=Macm=dptotaldt\vec{F}_{net,ext} = M\vec{a}_{cm} = \frac{d\vec{p}_{total}}{dt}

Physical meaning:

  • Only external forces affect COM motion
  • Internal forces cancel by Newton's Third Law
  • COM follows "particle" trajectory even for complex systems

Rocket Equation

For systems losing/gaining mass (rockets, leaking containers).

Tsiolkovsky rocket equation: Δv=vexln(minitialmfinal)\Delta v = v_{ex} \ln\left(\frac{m_{initial}}{m_{final}}\right)

Where vexv_{ex} = exhaust velocity relative to rocket.

Thrust Force

Propulsive force from mass ejection.

Fthrust=dmdtvexF_{thrust} = \frac{dm}{dt} v_{ex}

Where dm/dt = rate of mass change, vexv_{ex} = exhaust velocity

Sign convention: dm/dt negative for losing mass