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Physics · Ch 4 — Laws of Motion

Importance of Newton's Second Law of Motion

4.3.2

Importance of Newton's Second Law of Motion

The second law's real contribution is turning force into a precise, MEASURABLE, mathematical quantity: the rate of change of linear momentum, F⃗=dp⃗dt\vec{F}=\frac{d\vec{p}}{dt}.

It is essential to remember this momentum form as the fundamental statement, and NOT simply F⃗=ma⃗\vec{F}=m\vec{a}, because momentum p⃗=mv⃗\vec{p}=m\vec{v} can change either because the velocity changes or because the mass itself changes (or both). Expanding the derivative using the product rule, F⃗=d(mv⃗)dt=mdv⃗dt+v⃗dmdt=ma⃗+v⃗dmdt\vec{F}=\frac{d(m\vec{v})}{dt}=m\frac{d\vec{v}}{dt}+\vec{v}\frac{dm}{dt}=m\vec{a}+\vec{v}\frac{dm}{dt}. Only when the mass is constant, i.e. dmdt=0\frac{dm}{dt}=0, does this collapse to the familiar F⃗=ma⃗\vec{F}=m\vec{a}. For a system like a rocket, where the body continuously loses mass (burnt fuel is ejected) while its velocity also changes, BOTH terms on the right must be kept -- F⃗=ma⃗\vec{F}=m\vec{a} alone would be wrong.

This correction changes what counts as the 'fundamental' kinematic quantity of dynamics: it is MOMENTUM, not velocity, that a force directly changes. This matters because the effect of a force can show up as a change in a variable-mass system's mass distribution and not merely as a change in speed or direction. …

Misc Ex.1Force exerted on a hose pipe by ejected water

Worked out. A gardener's hose ejects water horizontally at 0.5 m/s through a bore of area 10 cm^2; using the variable-mass form of Newton's second law, F = v(dm/dt), the example finds the recoil force the gardener must apply to hold the pipe stationary, since density and ejection speed give the mass flow rate dm/dt = (rho)(A)( …