Block on a Smooth Circular Loop Track

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Work and Energy Beginner mechanical energy and conservation

Source: High school physics (Chinese)

Problem Sets:

work/energy basic

Problem

As shown in Figure below, a small block of mass m is released from rest at height H on a smooth track. The track becomes a vertical circular loop of radius R at the bottom. Neglect any resistance.

  1. What is the minimum height H required for the block to just pass through the highest point C of the circular loop?
  2. If the block is released from this minimum height H, what is the normal force it exerts on the track at the lowest point B?
P0470-problem-1

P0470-problem-1

[Q1] $H = \frac{5}{2}R$ [Q2] $F_{pressure} = 6mg$

[Q1] For the block to just pass the highest point C, the normal force from the track is zero. Gravity provides the required centripetal force. Let the speed at C be $v_C$.

$$mg = m\frac{v_C^2}{R} \implies v_C^2 = gR$$

Apply the conservation of mechanical energy between the starting point (height H) and point C (height 2R).

$$E_{initial} = E_C$$ $$mgH = \frac{1}{2}mv_C^2 + mg(2R)$$

Substitute $v_C^2 = gR$ into the energy equation:

$$mgH = \frac{1}{2}m(gR) + 2mgR$$ $$H = \frac{1}{2}R + 2R = \frac{5}{2}R$$

[Q2] The block is released from $H = \frac{5}{2}R$. Apply conservation of energy between the start and the lowest point B (height 0). Let the speed at B be $v_B$.

$$E_{initial} = E_B$$ $$mgH = \frac{1}{2}mv_B^2$$ $$mg\left(\frac{5}{2}R\right) = \frac{1}{2}mv_B^2 \implies v_B^2 = 5gR$$

At point B, the net force provides the centripetal force. The normal force $N_B$ points up and gravity $mg$ points down.

$$N_B - mg = m\frac{v_B^2}{R}$$ $$N_B = mg + m\frac{5gR}{R} = mg + 5mg = 6mg$$

By Newton's third law, the pressure exerted by the block on the track equals $N_B$.