Given:
- Angle of inclination, \( \theta = 60^\circ \)
- Block acceleration, \( a = \frac{g}{2} \)
- Gravitational acceleration, \( g \). Determine the coefficient of kinetic friction, \( \mu_k \).
Step 1: Force Analysis.
Forces acting on the block are:
- Gravitational force component along the incline: \( mg \sin \theta \).
- Normal force: \( N = mg \cos \theta \).
- Frictional force opposing motion: \( F_f = \mu_k N = \mu_k mg \cos \theta \). The net force driving the block down is: \[ F_{\text{net}} = mg \sin \theta - F_f \] This net force also equals mass times acceleration: \[ F_{\text{net}} = ma \]
Step 2: Equation Formulation.
Equating the expressions for \( F_{\text{net}} \): \[ mg \sin \theta - \mu_k mg \cos \theta = ma \] Substituting \( a = \frac{g}{2} \): \[ mg \sin \theta - \mu_k mg \cos \theta = m \cdot \frac{g}{2} \] Canceling mass \( m \) from both sides:
\[ g \sin \theta - \mu_k g \cos \theta = \frac{g}{2} \]
Step 3: Equation Simplification.
Substituting \( \theta = 60^\circ \):
\[ g \sin 60^\circ - \mu_k g \cos 60^\circ = \frac{g}{2} \]
Using \( \sin 60^\circ = \frac{\sqrt{3}}{2} \) and \( \cos 60^\circ = \frac{1}{2} \):
\[ g \cdot \frac{\sqrt{3}}{2} - \mu_k g \cdot \frac{1}{2} = \frac{g}{2} \]
Dividing by \( g \) and simplifying:
\[ \frac{\sqrt{3}}{2} - \frac{\mu_k}{2} = \frac{1}{2} \]
Multiplying by 2:
\[ \sqrt{3} - \mu_k = 1 \]
Step 4: Solving for \( \mu_k \).
\[ \mu_k = \sqrt{3} - 1 \]
Final Answer: \( \sqrt{3} - 1 \)