Some Particular Forces — Question 8

Section 5-6 · Physics pages 726–727

Question 8 A prescribed tangential contact force is distinct from the normal A 2 kg block slides right on a horizontal surface. A 9 N horizontal pull acts right. The surface exerts a measured 3 N resistance left. Take g = 10 m/s2; vertical acceleration is zero. N 3 N 9 N mg Normal and tangential surface forces have perpendicular directions. (a) Find normal force and horizontal acceleration. (b) Find the magnitude and direction of the total surface-contact force. (c) Why must the 3 N not be automatically replaced by the normal force?
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Question 8 - Solution A prescribed tangential contact force is distinct from the normal N 3 N 9 N mg (a) Separate perpendicular equations. N −20 = 0, 9 −3 = 2ax ⇒ N = 20 N, ax = 3 m/s2 N = 20 N. Horizontal resultant is 9 −3 = 6 N, so ax = 3 m/s2. (b) Combine the two contact components.⃗ Fsurface = (−3, 20) N, Fsurface = √ 409 = 20.224 N, ϕ = tan−1(3/20) = 8.531◦ The surface force is (−3, 20) N, magnitude √ 409 ≈20.224 N. Its direction is tan−1(3/20) ≈8.531◦ left of upward vertical. (c) Keep normal and tangential information distinct.⃗ Fsurface = N ˆy −f ˆx, ˆx · ˆy = 0, f = 3 N̸ = N The normal is perpendicular to the surface; resistance is tangential. Their magnitudes need not agree. No coefficient law is supplied here; the tangential force is measured, with detailed friction models reserved for later sections.

Question 8

A prescribed tangential contact force is distinct from the normal

A 2 kg block slides right on a horizontal surface. A 9 N horizontal pull acts right. The surface exerts a measured 3 N resistance left. Take g=10g=10 m/s2^2; vertical acceleration is zero.

Diagram shown in the original SVG worksheet.

  1. Find normal force and horizontal acceleration.

  2. Find the magnitude and direction of the total surface-contact force.

  3. Why must the 3 N not be automatically replaced by the normal force?

Question 8 - Solution

A prescribed tangential contact force is distinct from the normal

Diagram shown in the original SVG worksheet.

(a) Separate perpendicular equations.

N−20=0,9−3=2ax⇒N=20N,ax=3m/s2N-20=0,\quad9-3=2a_x\ \Rightarrow\ \boxed{N=20\,\mathrm N,\quad a_x=3\,\mathrm{m/s^2}} N=20N=20 N. Horizontal resultant is 9−3=69-3=6 N, so ax=3a_x=3 m/s2^2.

(b) Combine the two contact components.

F→surface=(−3,20)N,Fsurface=409=20.224N,ϕ=tan⁡−1(3/20)=8.531∘\vec F_{\mathrm{surface}}=(-3,20)\,\mathrm N,\quad F_{\mathrm{surface}}=\sqrt{409}=20.224\,\mathrm N,\quad\phi=\tan^{-1}(3/20)=8.531^\circ The surface force is (−3,20)(-3,20) N, magnitude 409≈20.224\sqrt{409}\approx20.224 N. Its direction is tan⁡−1(3/20)≈8.531∘\tan^{-1}(3/20)\approx8.531^\circ left of upward vertical.

(c) Keep normal and tangential information distinct.

F→surface=Nŷ−fx̂,x̂⋅ŷ=0,f=3N≠N\vec F_{\mathrm{surface}}=N\hat y-f\hat x,\quad\hat x\cdot\hat y=0,\quad f=3\,\mathrm N\ne N The normal is perpendicular to the surface; resistance is tangential. Their magnitudes need not agree. No coefficient law is supplied here; the tangential force is measured, with detailed friction models reserved for later sections.