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Torque Velocity and Displacement of Body Under Time Varying Force

A body having mass 1.0 kg1.0\text{ kg} is initially at rest at the origin at time t=0t = 0. A force given by F⃗=(αt i^+β j^)\vec{F} = (\alpha t\,\hat{i} + \beta\,\hat{j}) acts on the body, with constants α=1.0 N s−1\alpha = 1.0\text{ N s}^{-1} and β=1.0 N\beta = 1.0\text{ N}. Let τ⃗\vec{\tau} be the torque acting on the body about the origin at t=1.0 st = 1.0\text{ s}. Which of the following statements is (are) true?

Options

A

∣τ⃗∣=13 N m|\vec{\tau}| = \frac{1}{3}\text{ N m}

Correct
B

The torque τ⃗\vec{\tau} points along the direction of unit vector +k^+\hat{k}

C

At t=1 st = 1\text{ s}, the velocity of the body is v⃗=12(i^+2j^) m s−1\vec{v} = \frac{1}{2}(\hat{i} + 2\hat{j})\text{ m s}^{-1}

Correct
D

The magnitude of displacement of the body at t=1 st = 1\text{ s} equals 16 m\frac{1}{6}\text{ m}

Step-by-Step Solution

To determine which of the given statements are correct, we analyze the motion of the body under the given time-dependent force.

1. Acceleration, Velocity, and Displacement

Given:

  • Mass of the body, m=1.0 kgm = 1.0\text{ kg}
  • Force acting on the body, F⃗=αt i^+β j^=(t i^+j^) N\vec{F} = \alpha t\,\hat{i} + \beta\,\hat{j} = (t\,\hat{i} + \hat{j})\text{ N} (since α=1.0 N s−1\alpha = 1.0\text{ N s}^{-1} and β=1.0 N\beta = 1.0\text{ N})
  • Initial conditions at t=0t = 0: r⃗(0)=0⃗\vec{r}(0) = \vec{0} and v⃗(0)=0⃗\vec{v}(0) = \vec{0}

From Newton's second law, the acceleration a⃗(t)\vec{a}(t) is: a⃗(t)=F⃗(t)m=t i^+j^1.0=t i^+j^ m s−2\vec{a}(t) = \frac{\vec{F}(t)}{m} = \frac{t\,\hat{i} + \hat{j}}{1.0} = t\,\hat{i} + \hat{j}\text{ m s}^{-2}

Integrating the acceleration with respect to time to find the velocity v⃗(t)\vec{v}(t): v⃗(t)=∫0ta⃗(t′) dt′=∫0t(t′ i^+j^) dt′=12t2 i^+t j^\vec{v}(t) = \int_0^t \vec{a}(t')\,dt' = \int_0^t (t'\,\hat{i} + \hat{j})\,dt' = \frac{1}{2}t^2\,\hat{i} + t\,\hat{j}

At t=1.0 st = 1.0\text{ s}, the velocity is: v⃗(1.0)=12(1.0)2 i^+(1.0) j^=12i^+j^=12(i^+2j^) m s−1\vec{v}(1.0) = \frac{1}{2}(1.0)^2\,\hat{i} + (1.0)\,\hat{j} = \frac{1}{2}\hat{i} + \hat{j} = \frac{1}{2}(\hat{i} + 2\hat{j})\text{ m s}^{-1} Thus, Option C is correct.

Now, integrating the velocity to find the position vector r⃗(t)\vec{r}(t): r⃗(t)=∫0tv⃗(t′) dt′=∫0t(12t′2 i^+t′ j^)dt′=16t3 i^+12t2 j^\vec{r}(t) = \int_0^t \vec{v}(t')\,dt' = \int_0^t \left(\frac{1}{2}{t'}^2\,\hat{i} + t'\,\hat{j}\right)dt' = \frac{1}{6}t^3\,\hat{i} + \frac{1}{2}t^2\,\hat{j}

At t=1.0 st = 1.0\text{ s}, the position (displacement from origin) is: r⃗(1.0)=16 i^+12 j^ m\vec{r}(1.0) = \frac{1}{6}\,\hat{i} + \frac{1}{2}\,\hat{j}\text{ m}

The magnitude of displacement at t=1.0 st = 1.0\text{ s} is: ∣r⃗(1.0)∣=(16)2+(12)2=136+14=1036=106 m≠16 m|\vec{r}(1.0)| = \sqrt{\left(\frac{1}{6}\right)^2 + \left(\frac{1}{2}\right)^2} = \sqrt{\frac{1}{36} + \frac{1}{4}} = \sqrt{\frac{10}{36}} = \frac{\sqrt{10}}{6}\text{ m} \neq \frac{1}{6}\text{ m} Thus, Option D is incorrect.


2. Torque About the Origin

The torque τ⃗\vec{\tau} about the origin is given by: τ⃗=r⃗×F⃗\vec{\tau} = \vec{r} \times \vec{F}

At t=1.0 st = 1.0\text{ s}: r⃗=16 i^+12 j^\vec{r} = \frac{1}{6}\,\hat{i} + \frac{1}{2}\,\hat{j} F⃗=1.0 i^+1.0 j^=i^+j^\vec{F} = 1.0\,\hat{i} + 1.0\,\hat{j} = \hat{i} + \hat{j}

Calculating the cross product: τ⃗=(16 i^+12 j^)×(i^+j^)\vec{\tau} = \left(\frac{1}{6}\,\hat{i} + \frac{1}{2}\,\hat{j}\right) \times (\hat{i} + \hat{j}) τ⃗=(16)(i^×j^)+(12)(j^×i^)=16 k^−12 k^=−13 k^ N m\vec{\tau} = \left(\frac{1}{6}\right)(\hat{i} \times \hat{j}) + \left(\frac{1}{2}\right)(\hat{j} \times \hat{i}) = \frac{1}{6}\,\hat{k} - \frac{1}{2}\,\hat{k} = -\frac{1}{3}\,\hat{k}\text{ N m}

  • The magnitude of the torque is: ∣τ⃗∣=∣−13 k^∣=13 N m|\vec{\tau}| = \left|-\frac{1}{3}\,\hat{k}\right| = \frac{1}{3}\text{ N m} Thus, Option A is correct.

  • The direction of the torque vector τ⃗\vec{\tau} is along the −k^-\hat{k} direction, not +k^+\hat{k}. Thus, Option B is incorrect.


Conclusion

The correct statements are A and C.