Some Particular Forces — Question 4

Section 5-6 · Physics pages 718–719

Question 4 An angled pull can reduce floor support A 5 kg block stays on a frictionless horizontal floor. A force of 20 N acts 30◦above horizontal. Take g = 10 m/s2. N mg P The pull supplies some upward force, reducing the required floor support. (a) Find the normal force. (b) Find horizontal acceleration. (c) At what pull magnitude would contact become marginal if the angle stayed 30◦?
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Question 4 - Solution An angled pull can reduce floor support N mg P (a) Balance the constrained vertical component. N + P sin θ −mg = 0 ⇒ N = 50 −20 sin 30◦= 40 N N + 20 sin 30◦−50 = 0, so N = 40 N. (b) Use the unbalanced horizontal component. max = P cos θ ⇒ax = 20 cos 30◦ 5 = 2 √ 3 m/s2 ax = 20 cos 30◦/5 = 2 √ 3 ≈3.464 m/s2. (c) Set the limiting normal to zero. N = 0 ⇒Pcrit = mg sin θ = 50 0.5 = 100 N P sin 30◦= 50 gives P = 100 N. Above that value the assumed zero vertical acceleration with contact would require negative N; the block lifts and the constrained equations must change.

Question 4

An angled pull can reduce floor support

A 5 kg block stays on a frictionless horizontal floor. A force of 20 N acts 30∘30^\circ above horizontal. Take g=10g=10 m/s2^2.

Diagram shown in the original SVG worksheet.

  1. Find the normal force.

  2. Find horizontal acceleration.

  3. At what pull magnitude would contact become marginal if the angle stayed 30∘30^\circ?

Question 4 - Solution

An angled pull can reduce floor support

Diagram shown in the original SVG worksheet.

(a) Balance the constrained vertical component.

N+Psin⁡θ−mg=0⇒N=50−20sin⁡30∘=40NN+P\sin\theta-mg=0\ \Rightarrow\ \boxed{N=50-20\sin30^\circ=40\,\mathrm N} N+20sin⁡30∘−50=0N+20\sin30^\circ-50=0, so N=40N=40 N.

(b) Use the unbalanced horizontal component.

max=Pcos⁡θ⇒ax=20cos⁡30∘5=23m/s2ma_x=P\cos\theta\ \Rightarrow\ a_x=\frac{20\cos30^\circ}{5}=2\sqrt3\,\mathrm{m/s^2} ax=20cos⁡30∘/5=23≈3.464a_x=20\cos30^\circ/5=2\sqrt3\approx3.464 m/s2^2.

(c) Set the limiting normal to zero.

N=0⇒Pcrit=mgsin⁡θ=500.5=100NN=0\ \Rightarrow\ P_{\mathrm{crit}}=\frac{mg}{\sin\theta}=\frac{50}{0.5}=100\,\mathrm N Psin⁡30∘=50P\sin30^\circ=50 gives P=100P=100 N. Above that value the assumed zero vertical acceleration with contact would require negative N; the block lifts and the constrained equations must change.