The radius of curvature of the path of a charged particle in a uniform magnetic field is directly proportional to the
Answer & explanation
Correct answer: option 2
The correct answer is Option (2) → momentum of the particle
A charged particle moving perpendicular to a uniform magnetic field moves in a circle, because the magnetic force provides the centripetal force:
\( \displaystyle qvB = \frac{mv^{2}}{r} \;\Rightarrow\; r = \frac{mv}{qB} = \frac{p}{qB} \)
So \( r \) is directly proportional to the momentum \( p \) of the particle.
Option (1) charge of the particle — Incorrect. \( r \propto 1/q \); a larger charge gives a smaller radius.
Option (2) momentum of the particle — Correct. \( r = p/(qB) \), so \( r \propto p \).
Option (3) kinetic energy of the particle — Incorrect. \( r = \sqrt{2mK}/(qB) \) varies as \( \sqrt{K} \), not directly as \( K \).
Option (4) flux density of the field — Incorrect. \( r \propto 1/B \); a stronger field gives a smaller radius.
NCERT (2026-27):
Motion in a Magnetic Field – “… If the velocity v is perpendicular to the magnetic field B, the magnetic force is perpendicular to both v and B and acts like a centripetal force. It has a magnitude q v B. Equating the two expressions for centripetal force,
\( \displaystyle \frac{mv^2}{r} = qvB \)
which gives
\( \displaystyle r = \frac{mv}{qB} \qquad (4.5) \)
for the radius of the circle described by the charged particle. The larger the momentum, the larger is the radius and bigger the circle described.”