NVAMediumJEE 2025Gauss's Law Applications

JEE Physics 2025 Question with Solution

An electron is released from rest near an infinite non-conducting sheet of uniform charge density σ-\sigma. The rate of change of de-Broglie wavelength associated with the electron varies inversely as nthn^{th} power of time. The numerical value of nn is _____.

Answer

Correct answer:2

Step-by-step solution

Standard Method

Given: An electron is released from rest near an infinite non-conducting sheet of uniform charge density σ-\sigma.

Find: The numerical value of nn if the rate of change of de-Broglie wavelength varies inversely as the nthn^{th} power of time.

For an infinite non-conducting sheet, the electric field has constant magnitude

E=σ2ϵ0E = \frac{\sigma}{2\epsilon_0}

So the acceleration of the electron is constant and is given by

a=qEm=emσ2ϵ0a = \frac{qE}{m} = \frac{e}{m} \frac{\sigma}{2\epsilon_0}

If the electron starts from rest, then

v=atv = at

Now de-Broglie wavelength is

λ=hp\lambda = \frac{h}{p}

where momentum p=mvp = mv. Hence

λ=hmv=hm(at)\lambda = \frac{h}{mv} = \frac{h}{m(at)}

Substituting the value of aa,

λ=2ϵ0heσt\lambda = \frac{2\epsilon_0 h}{e\sigma t}

Differentiating with respect to time,

dλdt=2ϵ0heσt2\frac{d\lambda}{dt} = -\frac{2\epsilon_0 h}{e\sigma t^2}

Therefore,

dλdt1t2\frac{d\lambda}{dt} \propto \frac{1}{t^2}

So the rate of change varies inversely as the second power of time.

Therefore, the numerical value of nn is 22.

Using Momentum Relation

Given: The electron moves under constant acceleration due to the electric field of the sheet.

Find: How dλdt\frac{d\lambda}{dt} depends on time.

Let the momentum of the electron at time tt be pp and its de-Broglie wavelength be λ\lambda. Then

p=hλp = \frac{h}{\lambda}

Differentiating,

dpdt=hλ2dλdt\frac{dp}{dt} = -\frac{h}{\lambda^2} \frac{d\lambda}{dt}

But

dpdt=ma\frac{dp}{dt} = ma

So,

ma=hλ2dλdtma = -\frac{h}{\lambda^2} \frac{d\lambda}{dt}

Using

λ=hp\lambda = \frac{h}{p}

we get

ma=p2hdλdtma = -\frac{p^2}{h} \frac{d\lambda}{dt}

Since p=mvp = mv,

ma=m2v2hdλdtma = -\frac{m^2 v^2}{h} \frac{d\lambda}{dt}

Therefore,

dλdt=ahmv2\frac{d\lambda}{dt} = -\frac{ah}{mv^2}

For the charged sheet,

a=eσ2ϵ0ma = \frac{e\sigma}{2\epsilon_0 m}

And because the electron starts from rest,

v=atv = at

Substituting v=atv = at in the expression for dλdt\frac{d\lambda}{dt},

dλdt=2hϵ0σet2\frac{d\lambda}{dt} = -\frac{2h\epsilon_0}{\sigma e t^2}

Hence,

dλdt1t2\frac{d\lambda}{dt} \propto \frac{1}{t^2}

So, the required value is n=2n = 2.

Common mistakes

  • Using a variable electric field. For an infinite non-conducting sheet, the electric field is constant in magnitude, so the acceleration is constant. Do not apply inverse-square dependence as for a point charge.

  • Forgetting that de-Broglie wavelength is inversely proportional to momentum. Since λ=hp\lambda = \frac{h}{p}, as momentum increases with time, wavelength decreases. Treating λ\lambda as directly proportional to pp gives the wrong time dependence.

  • Missing the initial condition that the electron is released from rest. Because u=0u = 0, the velocity becomes v=atv = at. Using v=u+atv = u + at without setting u=0u = 0 can spoil the power of time.

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