NVAEasyJEE 2023Electric Field & Field Lines

JEE Physics 2023 Question with Solution

A stream of positively charged particles having q/m=2×1011C/kgq/m = 2 \times 10^{11} \, \text{C/kg} and velocity v0=3×107m/sv_0 = 3 \times 10^7 \, \text{m/s} is deflected by an electric field E=1.8j^kV/m\vec{E} = 1.8 \, \hat{j} \, \text{kV/m}. The electric field exists in a region of 10cm10 \, \text{cm} along the xx-direction. Due to the electric field, the deflection of the charged particles in the yy-direction is _____ mm.

Answer

Correct answer:2

Step-by-step solution

Standard Method

Given: qm=2×1011C/kg\dfrac{q}{m} = 2 \times 10^{11} \, \text{C/kg}, v0=3×107m/sv_0 = 3 \times 10^7 \, \text{m/s}, E=1.8j^kV/m=1.8×103V/m\vec{E} = 1.8 \, \hat{j} \, \text{kV/m} = 1.8 \times 10^3 \, \text{V/m}, and the field region length is d=10cm=0.1md = 10 \, \text{cm} = 0.1 \, \text{m}.

Find: Deflection in the yy-direction.

The electric force acts only along the yy-direction, so the acceleration is

a=qEma = \frac{qE}{m}

Substituting the given values,

a=(2×1011)(1.8×103)=3.6×1014m/s2a = \left(2 \times 10^{11}\right)\left(1.8 \times 10^3\right) = 3.6 \times 10^{14} \, \text{m/s}^2

The time spent inside the electric field is

t=dv0t = \frac{d}{v_0}

So,

t=0.13×107=13×108st = \frac{0.1}{3 \times 10^7} = \frac{1}{3 \times 10^8} \, \text{s}

Now the deflection in the yy-direction is

y=12at2y = \frac{1}{2}at^2

Substituting,

y=12(3.6×1014)(13×108)2y = \frac{1}{2} \cdot \left(3.6 \times 10^{14}\right) \cdot \left(\frac{1}{3 \times 10^8}\right)^2 y=123.6×101419×1016y = \frac{1}{2} \cdot 3.6 \times 10^{14} \cdot \frac{1}{9 \times 10^{16}} y=0.002my = 0.002 \, \text{m}

Converting to millimetres,

y=2mmy = 2 \, \text{mm}

Therefore, the deflection in the yy-direction is 2mm2 \, \text{mm}.

Step-by-step Calculation

Given: Motion along the xx-direction with constant speed v0v_0, and electric field along the +y+y-direction.

Principle: The particle has no acceleration in xx, but it has uniform acceleration in yy due to the electric field.

  1. Force due to electric field:
F=qEF = qE
  1. Acceleration in the yy-direction:
a=Fm=qEma = \frac{F}{m} = \frac{qE}{m}
  1. Using the given ratio q/mq/m:
a=(2×1011)(1.8×103)=3.6×1014m/s2a = \left(2 \times 10^{11}\right)\left(1.8 \times 10^3\right) = 3.6 \times 10^{14} \, \text{m/s}^2
  1. Time to cross the field region:
t=0.13×107=13×108st = \frac{0.1}{3 \times 10^7} = \frac{1}{3 \times 10^8} \, \text{s}
  1. Vertical deflection during this time:
y=12at2y = \frac{1}{2}at^2 y=123.6×1014(13×108)2y = \frac{1}{2} \cdot 3.6 \times 10^{14} \cdot \left(\frac{1}{3 \times 10^8}\right)^2 y=1.8×10149×1016=2×103my = \frac{1.8 \times 10^{14}}{9 \times 10^{16}} = 2 \times 10^{-3} \, \text{m}
  1. Convert to millimetres:
2×103m=2mm2 \times 10^{-3} \, \text{m} = 2 \, \text{mm}

Therefore, the required numerical value is 2.

Common mistakes

  • Using the electric field length directly in the deflection formula is incorrect because the particle first needs the time inside the field. Always compute t=d/v0t = d/v_0 before using y=12at2y = \frac{1}{2}at^2.

  • Forgetting to convert 1.8kV/m1.8 \, \text{kV/m} into 1.8×103V/m1.8 \times 10^3 \, \text{V/m} gives the wrong acceleration by a factor of 10310^3. Convert all units to SI before substitution.

  • Assuming the velocity changes in both directions is wrong here. The electric field is along j^\hat{j}, so acceleration is only in the yy-direction, while motion along xx remains uniform.

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