The work-energy theorem states that the minimum kinetic energy required for a particle to escape Earth's gravitational field is equal to the negative of the gravitational potential energy at that point.
The gravitational potential energy at a distance \( r \) from the center of Earth is given by:
\[
U = -\frac{GMm}{r}
\]
where:
- \( G \) is the gravitational constant,
- \( M \) is the mass of Earth,
- \( m \) is the mass of the particle, and
- \( r \) is the distance from the center of the Earth.
For the given question, the particle is at a distance \( 3R \) from the center of the Earth, where \( R \) is the radius of Earth. Therefore, the potential energy at this point is:
\[
U = -\frac{GMm}{3R}
\]
The minimum kinetic energy required for the particle to leave Earth's field is the amount of energy needed to overcome this gravitational potential energy. Thus, the minimum kinetic energy is:
\[
K = \left| U \right| = \frac{GMm}{3R}
\]
Now, using the relation \( g = \frac{GM}{R^2} \) (where \( g \) is the acceleration due to gravity at Earth's surface), we can rewrite the expression for kinetic energy as:
\[
K = \frac{gmR}{3}
\]
Thus, the minimum kinetic energy required for the particle to escape Earth's field is \( \frac{2}{3} mgR \).
Therefore, the correct answer is (3) \( \frac{2}{3} mgR \).