Linear Momentum — Question 6

Section 9-3 · Physics pages 1202–1203

Question 6 A tangent to momentum is not a tangent to the path A particle of mass 2.0 kg has⃗p(t) = (2t, 4 −t2) kg m/s, with numerical t in seconds. x y⃗ p(1)⃗ F(1) Momentum and force have an obtuse angle at the stated time, indicating decreasing kinetic energy. (a) At t = 1.0 s, find the force and decide whether the speed is increasing. (b) Find the positive time at which the force is perpendicular to velocity.
Show solutionHide solution
Question 6 - Solution A tangent to momentum is not a tangent to the path x y⃗ p(1)⃗ F(1) (a) Derivation and calculation Differentiate the given vector history:⃗ F(t) = d⃗p dt = (2, −2t) N.⃗ F(1) = (2, −2) N ,⃗ v(1) = (2, 3) 2 = (1, 1.5) m/s.⃗ F ·⃗v = 2(1) −2(1.5) = −1 W < 0, so the speed decreases. (b) Result and interpretation Perpendicularity requires⃗F ·⃗p = 0: 2(2t) −2t(4 −t2) = 2t(t2 −2) = 0. t = √ 2 s for t > 0. The nonzero force then changes direction without an instantaneous first-order speed change. Physical check The zero power at this time agrees with an extremum of the squared momentum magnitude.

Question 6

A tangent to momentum is not a tangent to the path

A particle of mass 2.0kg2.0\,\mathrm{kg} has p→(t)=(2t,4−t2)kgm/s\vec p(t)=(2t,4-t^2)\,\mathrm{kg\,m/s}, with numerical tt in seconds.

Diagram shown in the original SVG worksheet.

  1. At t=1.0st=1.0\,\mathrm s, find the force and decide whether the speed is increasing.

  2. Find the positive time at which the force is perpendicular to velocity.

Question 6 - Solution

A tangent to momentum is not a tangent to the path

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Differentiate the given vector history: F→(t)=dp→dt=(2,−2t)N.\vec F(t)=\frac{d\vec p}{dt}=(2,-2t)\ \mathrm N. F→(1)=(2,−2)N,v→(1)=(2,3)2=(1,1.5)m/s.\boxed{\vec F(1)=(2,-2)\ \mathrm N},\qquad\vec v(1)=\frac{(2,3)}2=(1,1.5)\ \mathrm{m/s}. F→⋅v→=2(1)−2(1.5)=−1W<0,\vec F\cdot\vec v=2(1)-2(1.5)=-1\ \mathrm W<0, so the speed decreases.

(b) Result and interpretation

Perpendicularity requires F→⋅p→=0\vec F\cdot\vec p=0: 2(2t)−2t(4−t2)=2t(t2−2)=0.2(2t)-2t(4-t^2)=2t(t^2-2)=0. t=2sfor t>0.\boxed{t=\sqrt2\ \mathrm s}\quad\text{for }t>0. The nonzero force then changes direction without an instantaneous first-order speed change.

Physical check

The zero power at this time agrees with an extremum of the squared momentum magnitude.