When two mutually perpendicular simple harmonic motions of same frequency, amplitude and phase are superimposed
The resulting motion is a linear simple harmonic motion along a straight line inclined equally to the straight lines of motion of component ones.
Y1=A1 sin wt;y2=A2 sin(wt+π2)
A2=√A21+A22 θ=tan−1(A2A1)