Which of the following are correct expression for torque acting on a body?
A. $\ddot{\tau}=\ddot{\mathrm{r}} \times \ddot{\mathrm{L}}$
B. $\ddot{\tau}=\frac{\mathrm{d}}{\mathrm{dt}}(\ddot{\mathrm{r}} \times \ddot{\mathrm{p}})$
C. $\ddot{\tau}=\ddot{\mathrm{r}} \times \frac{\mathrm{d} \dot{\mathrm{p}}}{\mathrm{dt}}$
D. $\ddot{\tau}=\mathrm{I} \dot{\alpha}$
E. $\ddot{\tau}=\ddot{\mathrm{r}} \times \ddot{\mathrm{F}}$
( $\ddot{r}=$ position vector; $\dot{\mathrm{p}}=$ linear momentum; $\ddot{\mathrm{L}}=$ angular momentum; $\ddot{\alpha}=$ angular acceleration; $\mathrm{I}=$ moment of inertia; $\ddot{\mathrm{F}}=$ force; $\mathrm{t}=$ time $)$
Choose the correct answer from the options given below:
The objective is to determine the valid expressions for torque \( \vec{\tau} \) acting on a body from the provided choices.
Torque is the rotational equivalent of force. It can be expressed in several equivalent ways:
\[ \vec{\tau} = \frac{d\vec{L}}{dt} = \vec{r} \times \vec{F} \]Given that linear momentum \( \vec{p} = m\vec{v} \) and \( \vec{F} = \frac{d\vec{p}}{dt} \), torque can be represented in alternative forms using these relationships. For rotational motion, torque can also be stated as:
\[ \vec{\tau} = I \vec{\alpha} \]Step 1: Evaluation of Option A: \( \vec{\tau} = \vec{r} \times \vec{L} \)
This expression is invalid, as torque represents the time rate of change of angular momentum, not its cross product with the position vector.
\[ \vec{\tau} e \vec{r} \times \vec{L} \]Step 2: Evaluation of Option B: \( \vec{\tau} = \frac{d}{dt}(\vec{r} \times \vec{p}) \)
Recognizing that \( \vec{L} = \vec{r} \times \vec{p} \), we can differentiate with respect to time:
\[ \vec{\tau} = \frac{d\vec{L}}{dt} = \frac{d}{dt}(\vec{r} \times \vec{p}) \]Therefore, Option B is valid.
Step 3: Evaluation of Option C: \( \vec{\tau} = \vec{r} \times \frac{d\vec{p}}{dt} \)
Substituting \( \frac{d\vec{p}}{dt} = \vec{F} \), the expression becomes:
\[ \vec{\tau} = \vec{r} \times \vec{F} \]Consequently, Option C is valid.
Step 4: Evaluation of Option D: \( \vec{\tau} = I \vec{\alpha} \)
This is a formulation of Newton's second law for rotation, applicable to rigid bodies rotating about a fixed axis. Therefore, Option D is valid.
Step 5: Evaluation of Option E: \( \vec{\tau} = \vec{r} \times \vec{F} \)
This constitutes the fundamental definition of torque. Hence, Option E is valid.
The correct expressions for torque are identified as Options B, C, D, and E.
Final Answer: B, C, D and E Only
Two point charges 2q and q are placed at vertex A and centre of face CDEF of the cube as shown in figure. The electric flux passing through the cube is : 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
