Problem 1.68 — Looping the loop — minimum speed

Problem Statement

A ball is threaded on a circular loop of radius $R$. What minimum speed must it have at the top to maintain contact?

Given Information

  • See problem statement for all given quantities.

Physical Concepts & Formulas

Circular motion requires a centripetal force directed toward the centre, providing the centripetal acceleration $a_c = v^2/r = \omega^2 r$. This force is not a new type of force — it is always the resultant of real forces (tension, normal force, friction, gravity) directed inward. At the minimum speed for maintaining contact, the normal force drops to zero.

  • $a_c = v^2/R = \omega^2 R$ — centripetal acceleration
  • $F_c = mv^2/R$ — net centripetal force needed
  • Banked curve: $\tan\theta = v^2/(Rg)$ — ideal banking angle
  • Loop minimum speed: $v_{\min} = \sqrt{gR}$ at top (N=0)

Step-by-Step Solution

Step 1 — Identify given quantities and set up the problem: At the top, both gravity and the normal force point downward (toward center).

Step 2 — Apply the relevant physical law or equation: For minimum contact, $N = 0$:

Step 3 — Solve algebraically for the unknown: $$mg = \frac{mv_{top}^2}{R} \implies v_{top,\min} = \sqrt{gR}$$

Step 4 — Substitute numerical values with units: Minimum speed at bottom (energy conservation from bottom to top):

Step 5 — Compute and check the result: $$\frac12 mv_{bot}^2 = \frac12 mv_{top}^2 + mg(2R)$$
$$v_{bot,\min} = \sqrt{v_{top,\min}^2 + 4gR} = \sqrt{gR+4gR} = \sqrt{5gR}$$

Step 6: Tension at bottom with minimum speed:

Worked Calculation

$$mg = \frac{mv_{top}^2}{R} \implies v_{top,\min} = \sqrt{gR}$$

$$\frac12 mv_{bot}^2 = \frac12 mv_{top}^2 + mg(2R)$$

$$v_{bot,\min} = \sqrt{v_{top,\min}^2 + 4gR} = \sqrt{gR+4gR} = \sqrt{5gR}$$

At the top, both gravity and the normal force point downward (toward center).

For minimum contact, $N = 0$:

$$mg = \frac{mv_{top}^2}{R} \implies v_{top,\min} = \sqrt{gR}$$

Minimum speed at bottom (energy conservation from bottom to top):

$$\frac12 mv_{bot}^2 = \frac12 mv_{top}^2 + mg(2R)$$
$$v_{bot,\min} = \sqrt{v_{top,\min}^2 + 4gR} = \sqrt{gR+4gR} = \sqrt{5gR}$$

Tension at bottom with minimum speed:

$$T_{bot} = m\left(g + \frac{v_{bot}^2}{R}\right) = m\left(g + 5g\right) = 6mg$$

Answer

$$\boxed{T_{bot} = m\left(g + \frac{v_{bot}^2}{R}\right) = m\left(g + 5g\right) = 6mg}$$

Physical Interpretation

The numerical answer is physically reasonable — matching expected orders of magnitude and dimensional analysis. The result confirms the theoretical prediction and provides quantitative insight into the system’s behaviour.


Comments

Leave a Reply

Your email address will not be published. Required fields are marked *