Angular momentum is the cross product of a radial vector and linear momentum vector.
If a body is rotating about a given axis, then the sum of the moments of the linear momentum of all the particles is known as the angular momentum of the body about that axis.

Since the direction of velocity is perpendicular to the orbital plane \(J \propto v\), hence, in an orbital motion, the angular momentum vector is perpendicular to the orbital plane.
The correct option is D, perpendicular to the orbital plane.
Orbital motion is a rotational motion of a body around another one. After an orbital period, the body traces its path again. Angular momentum is the cross product of a radial vector and linear momentum vector.
Angular momentum is a vector quantity having a direction perpendicular to the plane of revolution.

\(\overrightarrow{L} = I\overrightarrow{W}\)
\(\overrightarrow{L} \parallel \overrightarrow{W}\)
Hence, angular momentum is perpendicular to the plane of revolution.
A cylindrical tube \(AB\) of length \(l\), closed at both ends, contains an ideal gas of \(1\) mol having molecular weight \(M\). The tube is rotated in a horizontal plane with constant angular velocity \(\omega\) about an axis perpendicular to \(AB\) and passing through the edge at end \(A\), as shown in the figure. If \(P_A\) and \(P_B\) are the pressures at \(A\) and \(B\) respectively, then (consider the temperature to be same at all points in the tube) 
As shown in the figure, radius of gyration about the axis shown in \(\sqrt{n}\) cm for a solid sphere. Find 'n'. 
When rod becomes horizontal find its angular velocity. It is pivoted at point A as shown. 