According to Schmid's Law, the resolved shear stress (\( \tau \)) on a slip system depends on the orientation of the slip plane and slip direction with respect to the loading axis. The law is given by:
\[
\tau = \sigma \cdot \cos \phi \cdot \cos \lambda
\]
where:
- \( \sigma \) is the applied normal stress,
- \( \phi \) is the angle between the loading axis and the normal to the slip plane,
- \( \lambda \) is the angle between the loading axis and the slip direction.
When the slip plane is at \( 90^\circ \) to the loading axis, \( \phi = 90^\circ ⇒ \cos \phi = 0 \), hence:
\[
\tau = \sigma \cdot 0 \cdot \cos \lambda = 0
\]
Thus, the resolved shear stress becomes zero when the slip plane is perpendicular to the loading axis, and no slip can occur under such an orientation.