For the rod to be in equilibrium, the sum of forces and the sum of moments must be zero. Considering the forces acting on the rod:
1. The weight \( w = 10 \, \text{kN} \) acts vertically downward through the center of mass of the rod.
2. The friction force \( f \) at point \( J \) acts horizontally, and the normal force \( N \) at point \( J \) acts vertically upward.
To find the minimum static friction coefficient \( \mu \), we first use the moment equation about point \( K \) (taking counterclockwise as positive):
\[
\text{Moment due to } w = w \times \frac{a}{2}
\]
The moment due to friction \( f \) is:
\[
\text{Moment due to } f = f \times b
\]
For equilibrium:
\[
w \times \frac{a}{2} = f \times b
\]
Substitute \( f = \mu N \), and \( N = w \), as the vertical forces balance:
\[
w \times \frac{a}{2} = \mu w \times b
\]
Solve for \( \mu \):
\[
\mu = \frac{a}{2b}
\]
Substitute the given values \( a = 4 \, \text{m} \) and \( b = 3 \, \text{m} \):
\[
\mu = \frac{4}{2 \times 3} = \frac{4}{6} = 0.6667
\]
Thus, the minimum coefficient of static friction is:
\[
\boxed{0.667}
\]