The acceleration can be resolved into two components with respect to a set of tangential and normal axes:
$$a_c=v^2/r$$ (in the direction perpendicular to the velocity)
$$a_t=\frac{dv}{dt}$$ (In the direction of motion)
If the speed of the car is constant, then: $$a_t=\frac{dv}{dt}=0$$ and $$a=a_c=v^2/r$$
Therefore the car is accelerating towards the centre of the circular motion even though its speed is constant.