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Zorluk: OrtaNewton's Laws of Motion and Linear Momentum

When a constant horizontal stream of water of fixed cross-sectional area strikes a flat vertical wall normally and comes to rest without rebounding, the magnitude of the force exerted on the wall is directly proportional to the square of the speed of the water stream.

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True. The force exerted on the wall is directly proportional to the square of the speed of the water stream (Fv2F \propto v^2).
According to Newton's second law, force is the rate of change of linear momentum (F=ΔpΔtF = \frac{\Delta p}{\Delta t}). For a continuous fluid stream, ΔmΔt=ρAv\frac{\Delta m}{\Delta t} = \rho A v. Since each unit mass loses speed vv upon impact, F=(ΔmΔt)v=ρAv2F = \left(\frac{\Delta m}{\Delta t}\right) v = \rho A v^2. Thus, force is directly proportional to the square of the speed.

Adım Adım Çözüm

1
Determine the mass of water striking the wall in time interval Δt\Delta t.
Δm=ρAvΔt\Delta m = \rho A v \Delta t, where ρ\rho is fluid density, AA is cross-sectional area, and vv is speed.
The volume of water reaching the wall per unit time is given by AvA v.
2
Apply Newton's Second Law in terms of rate of change of linear momentum.
F=ΔpΔt=ΔmvΔt=(ρAvΔt)vΔt=ρAv2F = \frac{\Delta p}{\Delta t} = \frac{\Delta m \cdot v}{\Delta t} = \frac{(\rho A v \Delta t) v}{\Delta t} = \rho A v^2.
Since the water comes to rest, its change in velocity per unit mass is vv.
3
Analyze the dependence of force FF on speed vv.
Since density ρ\rho and cross-sectional area AA are constant, F=(constant)×v2    Fv2F = (\text{constant}) \times v^2 \implies F \propto v^2.
Both mass flow rate and momentum change per unit mass are proportional to vv.

Anahtar Kavram

Newton's Second Law and continuous mass flow momentum change
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