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