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Q.Two charged particles P and Q, having the same charge but different masses mPm_P and mQm_Q, start from rest and travel equal distances in a uniform electric field E⃗\vec{E} in time tPt_P and tQt_Q respectively. Neglecting the effect of gravity, the ratio tPtQ\dfrac{t_P}{t_Q} is : (A) mPmQ\dfrac{m_P}{m_Q} (B) mQmP\dfrac{m_Q}{m_P} (C) mPmQ\sqrt{\dfrac{m_P}{m_Q}} (D) mQmP\sqrt{\dfrac{m_Q}{m_P}}

BIHAR-BSEBCBSE Class XII Board 2024MCQ· 1mImportance★★★★★
✓ Free question

Both particles experience the same force (same charge, same field) but different accelerations inversely proportional to their masses. Since distance s=12at2s = \frac{1}{2}at^2 for motion from rest, time scales as 1a∝m\sqrt{\frac{1}{a}} \propto \sqrt{m}. The ratio is mPmQ\boxed{\sqrt{\dfrac{m_P}{m_Q}}}.

Why time depends on mass in a uniform field

When a charged particle moves in a uniform electric field, the force it experiences depends only on its charge: F=qEF = qE. But the resulting acceleration depends on mass through Newton's second law: a=Fm=qEma = \frac{F}{m} = \frac{qE}{m}.

Since both particles have the same charge qq and move in the same field EE, they experience identical forces. The lighter particle accelerates more; the heavier one accelerates less. When they travel the same distance starting from rest, the one with smaller acceleration (larger mass) takes longer.

The key insight is that for motion under constant acceleration from rest, distance grows as the square of time. This means time grows as the square root of the inverse of acceleration—and hence as the square root of mass.

Step-by-step solution

  1. Write the force on each particle. Both have charge qq (same magnitude), so:

FP=qE,FQ=qEF_P = qE, \quad F_Q = qE

  1. Find the acceleration of each particle. Using F=maF = ma:

aP=qEmP,aQ=qEmQa_P = \frac{qE}{m_P}, \quad a_Q = \frac{qE}{m_Q}

  1. Apply the kinematic equation for distance. Both start from rest (u=0u = 0) and travel the same distance ss. The equation of motion is:

s=ut+12at2=12at2s = ut + \frac{1}{2}at^2 = \frac{1}{2}at^2

For particle P:

s=12aPtP2=12⋅qEmP⋅tP2s = \frac{1}{2}a_P t_P^2 = \frac{1}{2} \cdot \frac{qE}{m_P} \cdot t_P^2

For particle Q:

s=12aQtQ2=12⋅qEmQ⋅tQ2s = \frac{1}{2}a_Q t_Q^2 = \frac{1}{2} \cdot \frac{qE}{m_Q} \cdot t_Q^2

  1. Equate the two expressions for ss. Since both travel the same distance:

12⋅qEmP⋅tP2=12⋅qEmQ⋅tQ2\frac{1}{2} \cdot \frac{qE}{m_P} \cdot t_P^2 = \frac{1}{2} \cdot \frac{qE}{m_Q} \cdot t_Q^2

The factors 12\frac{1}{2}, qq, and EE cancel:

tP2mP=tQ2mQ\frac{t_P^2}{m_P} = \frac{t_Q^2}{m_Q}

  1. Solve for the ratio tPtQ\dfrac{t_P}{t_Q}. Rearranging:

tP2tQ2=mPmQ\frac{t_P^2}{t_Q^2} = \frac{m_P}{m_Q}

Taking the square root of both sides:

tPtQ=mPmQ\frac{t_P}{t_Q} = \sqrt{\frac{m_P}{m_Q}}

Tip

A quick way to remember: in uniform acceleration from rest, t∝sat \propto \sqrt{\frac{s}{a}}. Since ss is constant and a∝1ma \propto \frac{1}{m}, we have t∝mt \propto \sqrt{m}.

Watch out

Don't confuse this with momentum or kinetic energy ratios. The time ratio depends purely on the kinematic relationship s=12at2s = \frac{1}{2}at^2, not on the final velocities or energies reached.

✓Final answer

The correct option is (C) mPmQ\sqrt{\dfrac{m_P}{m_Q}}.

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