I am always leery of providing solutions to persons who do not show that they have even attempted a solution to the problem. I find it better to only help as much as necessary, otherwise the person gains little. But as burnedout has aready provided a solution for you, I will continue.
You have three forces in the problem, the weight of the car, W, the normal force from the road, N, and the frictional force, f. Since N and f are parallel/perpendicular to the road surface, it is useful to decompose the forces into horizontal and vertical components, based on the angle of inclination from the horizontal, theta.
There is no acceleration in the vertical, so a force balance gives:
N*cos(theta) - W - f*sin(theta) = 0
In the horizontal direction, the normal force and friction provide the centripetal acceleration to keep the car from slipping:
N*sin(theta) + f*cos(theta) = Fc = m*v^2/R
Using the fact that f = mu*N and W =m*g both these equations can be solved for the unknown normal force, and set equal. This gives
sin(theta) + mu*cos(theta)
--------------------------------------- = v^2/(g*R)
cos(theta) - mu*sin(theta)
Note that :
1) The mass drops out. It would be a tremendous difficulty if engineers had to worry about the mass of the vehicle when determining banking angle.
2) As mu ---> 0, the equation reduces to tan(theta) = v^2/(g*R)
3) As theta ---> 0, the equation reduces to mu = v^2/(g*R)
4) The equation can be solved for theta, or as burnedout has shown, you can arrive at the answer more simply by taking the frictionless banking angle and subtracting off the equivalent angle due to friction being the sole contribution to the centripetal acceleration.
Edit: Found a typo, minus sign in horizontal force eqn. changed to plus sign.