A 4 kg mass moves under the influence of a force F = (4t^3 î − 3t ĵ) N where t is the time in second. If mass starts from origin at t = 0, the velocity and position after t = 2 s will be:
Q. A 4 kg mass moves under the influence of a force \( \vec{F} = (4t^3 \hat{i} - 3t \hat{j}) \) N where t is the time in second. If mass starts from origin at t = 0, the velocity and position after t = 2 s will be:
(A) \( \vec{v} = 3\hat{i} + \frac{3}{2}\hat{j} \quad \vec{r} = \frac{6}{5}\hat{i} + \hat{j} \)
(B) \( \vec{v} = 4\hat{i} - \frac{3}{2}\hat{j} \quad \vec{r} = \frac{6}{5}\hat{i} - \hat{j} \)
(C) \( \vec{v} = 4\hat{i} - \frac{3}{2}\hat{j} \quad \vec{r} = \frac{8}{5}\hat{i} - \hat{j} \)
(D) \( \vec{v} = 4\hat{i} + \frac{5}{2}\hat{j} \quad \vec{r} = \frac{8}{5}\hat{i} + 2\hat{j} \)
Correct Answer: C

Explanation

Given mass \( m = 4 \) kg.

\[ \vec{F} = (4t^3 \hat{i} - 3t \hat{j}) \]

Using Newton’s second law:

\[ \vec{a} = \frac{\vec{F}}{m} \]

\[ \vec{a} = \left(t^3 \hat{i} - \frac{3}{4}t \hat{j}\right) \]

Velocity is integral of acceleration:

\[ \vec{v} = \int \vec{a} \, dt \]

\[ v_x = \int t^3 dt = \frac{t^4}{4} \]

\[ v_y = \int -\frac{3}{4}t dt = -\frac{3}{8}t^2 \]

At \( t = 2 \):

\[ v_x = \frac{16}{4} = 4 \]

\[ v_y = -\frac{3}{8} \times 4 = -\frac{3}{2} \]

\[ \vec{v} = 4\hat{i} - \frac{3}{2}\hat{j} \]

Position is integral of velocity:

\[ x = \int \frac{t^4}{4} dt = \frac{t^5}{20} \]

\[ y = \int -\frac{3}{8}t^2 dt = -\frac{t^3}{8} \]

At \( t = 2 \):

\[ x = \frac{32}{20} = \frac{8}{5} \]

\[ y = -\frac{8}{8} = -1 \]

\[ \vec{r} = \frac{8}{5}\hat{i} - \hat{j} \]

Therefore correct answer is (C).

Related Theory (Time Dependent Force & Vector Motion)

When force depends on time, acceleration also becomes time dependent. Newton’s second law in vector form is:

\[ \vec{F} = m\vec{a} \]

If force varies with time, we must integrate acceleration to obtain velocity and integrate velocity to obtain position. Initial conditions are extremely important.

For vector motion:

\[ \vec{a} = a_x \hat{i} + a_y \hat{j} \]

Each component is treated independently.

Velocity:

\[ \vec{v} = \int \vec{a} dt \]

Position:

\[ \vec{r} = \int \vec{v} dt \]

This topic connects calculus with mechanics and is highly important for JEE Main and Advanced. Many students forget to divide force by mass before integrating.

Common mistakes:

• Not dividing by mass
• Missing integration constants
• Arithmetic errors in powers
• Confusing vector components

This concept is foundation for advanced mechanics problems including variable force fields and motion in electric fields.

Related JEE Main Questions

Related Covered Topics

jee mains jee advanced iit jee neet engineering entrance exam medical entrance exam mechanics jee mains time dependent force vector motion integration in physics newton laws jee important jee mains question important jee advanced question kinematics calculus electrostatics jee modern physics jee coordinate geometry jee algebra jee organic chemistry jee physical chemistry numerical dimensional analysis
Scroll to Top