Concept:
In vertical circular motion:
- Maximum tension occurs at lowest point
- Minimum tension occurs at highest point
\[
T_{\text{bottom}} = \frac{mv_b^2}{L} + mg
\]
\[
T_{\text{top}} = \frac{mv_t^2}{L} - mg
\]
Step 1: Given ratio.
\[
\frac{T_{\text{max}}}{T_{\text{min}}} = 3
\Rightarrow \frac{T_{\text{bottom}}}{T_{\text{top}}} = 3
\]
Step 2: Apply energy conservation.
Between top and bottom:
\[
\frac{1}{2}mv_b^2 = \frac{1}{2}mv_t^2 + 2mgL
\]
\[
v_b^2 = v_t^2 + 4gL
\]
Step 3: Substitute in tension ratio.
\[
\frac{\frac{m(v_t^2 + 4gL)}{L} + mg}{\frac{mv_t^2}{L} - mg} = 3
\]
Cancel \(m\):
\[
\frac{\frac{v_t^2}{L} + 4g + g}{\frac{v_t^2}{L} - g} = 3
\]
\[
\frac{\frac{v_t^2}{L} + 5g}{\frac{v_t^2}{L} - g} = 3
\]
Step 4: Solve equation.
Let \(x = \frac{v_t^2}{L}\)
\[
\frac{x + 5g}{x - g} = 3
\]
\[
x + 5g = 3x - 3g
\]
\[
2x = 8g \Rightarrow x = 4g
\]
\[
\frac{v_t^2}{L} = g \Rightarrow v_t^2 = gL
\]
Step 5: Conclusion.
\[
v_t = \sqrt{gL}
\]