Kinetic Energy — Question 2

Section 7-2 · Physics pages 874–875

Question 2 A right-angle turn can leave kinetic energy unchanged Use classical translational kinetic energy K = 1 2m|⃗v|2. A 2 kg particle changes velocity from (3, 4) m/s to (−4, 3) m/s in a fixed perpendicular x-y frame. x y⃗ vi⃗ vf The velocity arrows have equal length and perpendicular directions. (a) Find initial and final kinetic energies. (b) Find the velocity-change vector and its magnitude. (c) Is 1 2m|∆⃗v|2 the kinetic-energy change? Explain numerically.
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Question 2 - Solution A right-angle turn can leave kinetic energy unchanged x y⃗ vi⃗ vf (a) Compute the squared norms. The governing relation is K = 1 2m(v2 x + v2 y), ∆K = 1 2m(|⃗vf|2 −|⃗vi|2) Both velocity norms squared are 32 + 42 = 25 m2/s2, giving Ki = Kf = 25 J, ∆K = 0. (b) Subtract vectors first. ∆⃗v = (−7, −1) m/s, so |∆⃗v| = √ 50 = 5 √ 2 m/s. The velocity changes despite unchanged speed. (c) Distinguish two quadratic expressions. 1 2m|∆⃗v|2 = 50 J, not zero. In general ∆K = 1 2m(|⃗vf|2 −|⃗vi|2); squaring a vector difference adds different cross terms.

Question 2

A right-angle turn can leave kinetic energy unchanged

Use classical translational kinetic energy K=12m|v→|2K=\tfrac12 m|\vec v|^2. A 2 kg particle changes velocity from (3,4)(3,4) m/s to (−4,3)(-4,3) m/s in a fixed perpendicular x-y frame.

Diagram shown in the original SVG worksheet.

  1. Find initial and final kinetic energies.

  2. Find the velocity-change vector and its magnitude.

  3. Is 12m|Δv→|2\tfrac12m|\Delta\vec v|^2 the kinetic-energy change? Explain numerically.

Question 2 - Solution

A right-angle turn can leave kinetic energy unchanged

Diagram shown in the original SVG worksheet.

(a) Compute the squared norms.

The governing relation is K=12m(vx2+vy2),ΔK=12m(|v→f|2−|v→i|2)\boxed{K=\tfrac12m(v_x^2+v_y^2),\qquad\Delta K=\tfrac12m(|\vec v_f|^2-|\vec v_i|^2)} Both velocity norms squared are 32+42=25m2/s2,3^2+4^2=25\ \mathrm{m^2/s^2}, giving Ki=Kf=25J,ΔK=0.K_i=K_f=25\ \mathrm J,\qquad \Delta K=0.

(b) Subtract vectors first.

Δv→=(−7,−1)m/s,\Delta\vec v=(-7,-1)\ \mathrm{m/s}, so |Δv→|=50=52m/s.|\Delta\vec v|=\sqrt{50}=5\sqrt2\ \mathrm{m/s}. The velocity changes despite unchanged speed.

(c) Distinguish two quadratic expressions.

12m|Δv→|2=50J,\tfrac12m|\Delta\vec v|^2=50\ \mathrm J, not zero. In general ΔK=12m(|v→f|2−|v→i|2);\Delta K=\tfrac12m(|\vec v_f|^2-|\vec v_i|^2); squaring a vector difference adds different cross terms.