The torque \( \mathbf{\tau} \) exerted by the force \( \mathbf{F} = \hat{i} - \hat{j} + \hat{k} \) on a particle at \( \mathbf{r} = (1 \, \text{m}, 1 \, \text{m}, 1 \, \text{m}) \) with respect to the origin is calculated using the cross product \( \mathbf{\tau} = \mathbf{r} \times \mathbf{F} \).
The vectors are: \( \mathbf{r} = \hat{i} + \hat{j} + \hat{k} \) and \( \mathbf{F} = \hat{i} - \hat{j} + \hat{k} \).
The cross product is computed via the determinant:
Expanding the determinant yields:
Thus, the torque vector is \( \mathbf{\tau} = 2\hat{i} + 0\hat{j} - 2\hat{k} \).
The magnitude of the torque in the z-direction is \( |-2| = 2 \).
A square Lamina OABC of length 10 cm is pivoted at \( O \). Forces act at Lamina as shown in figure. If Lamina remains stationary, then the magnitude of \( F \) is: 