always radially outwards.
radially outwards initially and radially inwards later.
always radially inwards.
radially inwards initially and radially outwards later.
mgR(1−cosθ)=1/2mv²
So the normal force, N = mgcosθ−mv²/R
So, when θ is small, N is +ve so it is radially inwards.
When the θ gets large, N gets -ve, so it is radially outwards.