To solve this problem, we must understand the concepts of force, position vector, and torque in the context of physics. The question provides us with a force vector \(\vec{F}\), a position vector \(\vec{r}\), and a torque \(\vec{\tau}\).
**Torque and Dot Product:***
Torque \(\vec{\tau}\) is defined as the cross product of the position vector \(\vec{r}\) and the force vector \(\vec{F}\):
\[\vec{\tau} = \vec{r} \times \vec{F}\]**Properties of Dot Product and Cross Product:***
**The Meaning of \(\vec{r} \cdot \vec{\tau} = 0$**\)
The position vector \(\vec{r}\) and the torque \(\vec{\tau}\) (which is perpendicular to \(\vec{r}\) and \(\vec{F}\)) are perpendicular, leading to:
\[\vec{r} \cdot \vec{\tau} = 0\]**The Meaning of \(\vec{F} \cdot \vec{\tau} = 0$**\)
Similarly, the force vector \(\vec{F}\) is also perpendicular to the torque vector \(\vec{\tau}\), hence:
\[\vec{F} \cdot \vec{\tau} = 0\]**Conclusion:***
The correct answer is that both \(\vec{r} \cdot \vec{\tau} = 0\) and \(\vec{F} \cdot \vec{\tau} = 0\) are true because the torque is perpendicular to both \(\vec{r}\) and \(\vec{F}\).
Thus, the correct answer is:
\(\vec{r} \cdot \vec{\tau} = 0\) and \(\vec{F} \cdot \vec{\tau} = 0\)
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 