Correct options are (1), (2) and (3)


\(x = a\cos (pt) \Rightarrow \cos (pt) = \frac xa\quad....(i)\)
\(y = b\sin (pt) \Rightarrow \sin(pt) = \frac yb\quad....(ii)\)
Squaring and adding Eqs. (i) and (ii), we get
\(\frac{x^2}{a^2} + \frac{y^2}{b^2} = 1\)
Therefore, path of the particle is an ellipse. Hence, option (a) is correct.
From the given equations we can find
\(\frac {dx}{dt} = v_x = -ap \sin pt\)
\(\Rightarrow \frac{d^2 x}{dt^2} = a_x = -ap^2\cos pt\)
\(\frac {dy}{dt} = v_y = bp \cos pt\)
\(\Rightarrow \frac{d^2 y}{dt^2} = a_y = -bp^2\sin pt\)
At time t = π/2p or pt = π/2
ax and \(v - \nu\) become zero (because cos π/2 = 0)
only vx and ay are left.
or we can say that velocity is along negative x-axis and acceleration along y-axis.
Hence, at t = π/2p velocity and acceleration of the particle are normal to each other. So, option (b) is also correct.
At t = t, position of the particle
\(r(t) = x\hat i + y\hat j = a\cos pt\hat i + b \sin pt\hat j\)
and acceleration of the particle is
\(a(t) = a_x\hat i + a_y\hat j = - p^2 [a \cos pt\hat i + b\sin pt \hat j]\)
\(= -p^2[x\hat i + y\hat j]\)
\(= -p^2 r (t)\)
Therefore, acceleration of the particle is always directed towards origin.
Hence, option (c) is also correct.
At t = 0, particle is at (a, 0) and at t = π/2p particle is at (0, b).
Therefore, the distance covered is one-fourth of the elliptical path not a.
Hence, option (d) is wrong.