Concept:
When a particle moves in a vertical circular path, the centripetal force at the top of the circle is provided by the sum of weight and the normal reaction.
\[
\frac{mv^2}{R} = mg + N
\]
Also, since the track is smooth, mechanical energy is conserved.
\[
\text{Loss of potential energy} = \text{Gain in kinetic energy}
\]
Step 1: Apply the centripetal force condition at the highest point.}
Given that the normal reaction is three times the weight:
\[
N = 3mg
\]
Substitute into the centripetal force equation:
\[
mg + N = \frac{mv^2}{R}
\]
\[
mg + 3mg = \frac{mv^2}{R}
\]
\[
4mg = \frac{mv^2}{R}
\]
\[
v^2 = 4gR
\]
Step 2: Apply conservation of energy.}
The particle starts from height \(h\) and reaches the highest point of the circular track which is at height \(2R\).
\[
mg(h-2R) = \frac{1}{2}mv^2
\]
Substitute \(v^2 = 4gR\):
\[
mg(h-2R) = \frac{1}{2}m(4gR)
\]
\[
mg(h-2R) = 2mgR
\]
Cancel \(mg\):
\[
h-2R = 2R
\]
\[
h = 4R
\]
Final Result
\[
h = 4R
\]