MCQEasyJEE 2026Newton's Second Law & Force

JEE Physics 2026 Question with Solution

A 4kg4 \, \text{kg} mass moves under the influence of a force F=(4t3i^3t2j^)\vec{F} = (4t^3\hat{i} - 3t^2\hat{j}) N where tt is the time in second. If mass starts from origin at t=0t=0, the velocity and position after t=2st = 2 \, \text{s} will be:

  • A

    v=4i^32j^\vec{v} = 4\hat{i} - \frac{3}{2}\hat{j}, r=85i^j^\vec{r} = \frac{8}{5}\hat{i} - \hat{j}

  • B

    v=4i^2j^\vec{v} = 4\hat{i} - 2\hat{j}, r=85i^j^\vec{r} = \frac{8}{5}\hat{i} - \hat{j}

  • C

    v=4i^3j^\vec{v} = 4\hat{i} - 3\hat{j}, r=85i^2j^\vec{r} = \frac{8}{5}\hat{i} - 2\hat{j}

  • D

    v=4i^3j^\vec{v} = 4\hat{i} - 3\hat{j}, r=85i^j^\vec{r} = \frac{8}{5}\hat{i} - \hat{j}

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: m=4kgm = 4 \, \text{kg}, F(t)=(4t3i^3t2j^)N\vec{F}(t) = (4t^3\hat{i} - 3t^2\hat{j}) \, \text{N}, initial conditions v0=0\vec{v}_0 = 0 and r0=0\vec{r}_0 = 0.

Find: The velocity vector and position vector at t=2st = 2 \, \text{s}.

For a time-dependent force, use the chain:

Favr\vec{F} \rightarrow \vec{a} \rightarrow \vec{v} \rightarrow \vec{r}

First divide force by mass to get acceleration, then integrate twice using the initial conditions.

From Newton's second law,

a(t)=Fm=14(4t3i^3t2j^)=(t3i^34t2j^)m/s2\vec{a}(t) = \frac{\vec{F}}{m} = \frac{1}{4}(4t^3\hat{i} - 3t^2\hat{j}) = \left(t^3\hat{i} - \frac{3}{4}t^2\hat{j}\right) \, \text{m/s}^2

Now integrate acceleration to get velocity:

v(t)=0t(t3i^34t2j^)dt\vec{v}(t) = \int_0^t \left(t'^3\hat{i} - \frac{3}{4}t'^2\hat{j}\right) dt' v(t)=[t44i^34t33j^]0t=(t44i^t34j^)m/s\vec{v}(t) = \left[\frac{t'^4}{4}\hat{i} - \frac{3}{4}\frac{t'^3}{3}\hat{j}\right]_0^t = \left(\frac{t^4}{4}\hat{i} - \frac{t^3}{4}\hat{j}\right) \, \text{m/s}

At t=2st = 2 \, \text{s},

v(2)=244i^234j^=164i^84j^=(4i^2j^)m/s\vec{v}(2) = \frac{2^4}{4}\hat{i} - \frac{2^3}{4}\hat{j} = \frac{16}{4}\hat{i} - \frac{8}{4}\hat{j} = (4\hat{i} - 2\hat{j}) \, \text{m/s}

Next integrate velocity to get position:

r(t)=0t(t44i^t34j^)dt\vec{r}(t) = \int_0^t \left(\frac{t'^4}{4}\hat{i} - \frac{t'^3}{4}\hat{j}\right) dt' r(t)=[14t55i^14t44j^]0t=(t520i^t416j^)m\vec{r}(t) = \left[\frac{1}{4}\frac{t'^5}{5}\hat{i} - \frac{1}{4}\frac{t'^4}{4}\hat{j}\right]_0^t = \left(\frac{t^5}{20}\hat{i} - \frac{t^4}{16}\hat{j}\right) \, \text{m}

At t=2st = 2 \, \text{s},

r(2)=2520i^2416j^=3220i^1616j^=(85i^j^)m\vec{r}(2) = \frac{2^5}{20}\hat{i} - \frac{2^4}{16}\hat{j} = \frac{32}{20}\hat{i} - \frac{16}{16}\hat{j} = \left(\frac{8}{5}\hat{i} - \hat{j}\right) \, \text{m}

Therefore, the velocity is (4i^2j^)m/s(4\hat{i} - 2\hat{j}) \, \text{m/s} and the position is (85i^j^)m\left(\frac{8}{5}\hat{i} - \hat{j}\right) \, \text{m}. The correct option is B.

Stepwise Integration View

Given: A particle of mass 4kg4 \, \text{kg} is acted upon by F=(4t3i^3t2j^)\vec{F} = (4t^3\hat{i} - 3t^2\hat{j}) and starts from rest at the origin.

Find: v(2)\vec{v}(2) and r(2)\vec{r}(2).

Resolve the force into components and divide each by mass:

ax=4t34=t3,ay=3t24=34t2a_x = \frac{4t^3}{4} = t^3, \qquad a_y = \frac{-3t^2}{4} = -\frac{3}{4}t^2

Integrating componentwise,

vx=0tt3dt=t44,vy=0t34t2dt=t34v_x = \int_0^t t'^3 \, dt' = \frac{t^4}{4}, \qquad v_y = \int_0^t -\frac{3}{4}t'^2 \, dt' = -\frac{t^3}{4}

So,

v(t)=t44i^t34j^\vec{v}(t) = \frac{t^4}{4}\hat{i} - \frac{t^3}{4}\hat{j}

At t=2t=2,

v(2)=4i^2j^\vec{v}(2) = 4\hat{i} - 2\hat{j}

Now integrate again for position:

x(t)=0tt44dt=t520,y(t)=0tt34dt=t416x(t) = \int_0^t \frac{t'^4}{4} \, dt' = \frac{t^5}{20}, \qquad y(t) = \int_0^t -\frac{t'^3}{4} \, dt' = -\frac{t^4}{16}

Hence,

r(t)=t520i^t416j^\vec{r}(t) = \frac{t^5}{20}\hat{i} - \frac{t^4}{16}\hat{j}

At t=2t=2,

r(2)=85i^j^\vec{r}(2) = \frac{8}{5}\hat{i} - \hat{j}

Therefore, the required pair matches option B.

Common mistakes

  • Using F\vec{F} directly as velocity or position is incorrect because force must first be converted to acceleration using a=F/m\vec{a} = \vec{F}/m. Always divide by the mass before integrating.

  • Forgetting the initial conditions is wrong because the constants of integration are fixed by v0=0\vec{v}_0 = 0 and r0=0\vec{r}_0 = 0. Use the particle starting from rest at the origin while integrating.

  • Making a sign error in the j^\hat{j} component leads to the wrong option. The force has a negative j^\hat{j} term, so both acceleration and velocity components along j^\hat{j} remain negative after integration.

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