Applying Newton's Laws — Question 3

Section 5-8 · Physics pages 756–757

Question 3 An incline changes the gravitational driving component Take g = 10 m/s2. A 4 kg block on a frictionless 30◦incline connects over an ideal fixed pulley at the top to a hanging 3 kg mass. The light cord is taut. 4 kg 3 kg 30◦ Frictionless incline and ideal fixed pulley; the cord constrains both motions. (a) Choose and verify the direction of acceleration. (b) Find acceleration, tension and incline normal force. (c) What hanging mass would instead produce zero acceleration?
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Question 3 - Solution An incline changes the gravitational driving component 4 kg 3 kg 30◦ (a) Compare driving components. Fdrive = mhg −mig sin 30◦= 30 −20 = 10 N > 0 The block’s downslope gravity component is 4(10) sin 30◦= 20 N. The hanging weight is 30 N, so the 3 kg mass descends and the block ascends. (b) Write both equations with consistent senses. 30 −T = 3a, T −20 = 4a : a = 10/7, T = 180/7, N = 20 √ 3 (SI) 30 −T = 3a and T −20 = 4a give a = 10/7 ≈1.429 m/s2 and T = 180/7 ≈25.714 N. Perpendicular balance gives N = 20 √ 3 ≈34.641 N. (c) Match the driving weights. a = 0 ⇒mhg = mig sin 30◦⇒mh = 2 kg Zero acceleration requires mhg = 4g sin 30◦, hence mh = 2 kg. This permits either rest or compatible constant motion, depending on initial conditions.

Question 3

An incline changes the gravitational driving component

Take g=10g=10 m/s2^2. A 4 kg block on a frictionless 30∘30^\circ incline connects over an ideal fixed pulley at the top to a hanging 3 kg mass. The light cord is taut.

Diagram shown in the original SVG worksheet.

  1. Choose and verify the direction of acceleration.

  2. Find acceleration, tension and incline normal force.

  3. What hanging mass would instead produce zero acceleration?

Question 3 - Solution

An incline changes the gravitational driving component

Diagram shown in the original SVG worksheet.

(a) Compare driving components.

Fdrive=mhg−migsin⁡30∘=30−20=10N>0F_{\mathrm{drive}}=m_hg-m_ig\sin30^\circ=30-20=10\,\mathrm N>0 The block’s downslope gravity component is 4(10)sin⁡30∘=204(10)\sin30^\circ=20 N. The hanging weight is 30 N, so the 3 kg mass descends and the block ascends.

(b) Write both equations with consistent senses.

30−T=3a,T−20=4a:a=10/7,T=180/7,N=203(SI)30-T=3a,\quad T-20=4a:\quad\boxed{a=10/7,\ T=180/7,\ N=20\sqrt3}\quad\text{(SI)} 30−T=3a30-T=3a and T−20=4aT-20=4a give a=10/7≈1.429a=10/7\approx1.429 m/s2^2 and T=180/7≈25.714T=180/7\approx25.714 N. Perpendicular balance gives N=203≈34.641N=20\sqrt3\approx34.641 N.

(c) Match the driving weights.

a=0⇒mhg=migsin⁡30∘⇒mh=2kga=0\ \Rightarrow\ m_hg=m_ig\sin30^\circ\ \Rightarrow\ m_h=2\,\mathrm{kg} Zero acceleration requires mhg=4gsin⁡30∘m_hg=4g\sin30^\circ, hence mh=2m_h=2 kg. This permits either rest or compatible constant motion, depending on initial conditions.