Class 12 Physics Electrons Notes

Chapter 20 – Electrons | Nepal eNotes
PHYSICS • CHAPTER 20

Electrons

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Millikan’s Oil Drops Experiment

Principle

This experiment involves application of Stoke’s law on viscosity and it is based on the study of motion of oil drops under the action of gravity alone, gravity and electric field.

Experimental arrangement

Double wall chamber upper plate lower plate light x-rays Atomiser Clock oil Microscope

The experimental setup is as shown in the figure. It consists of a double walled chamber having three window one is for light, one is for x-rays and one is for microscope. There are two horizontal parallel plates, the upper plate having small hole on it. The clock oil is sprayed with the help of atomizer between the plates and motion of drops is observed with the help of microscope.

Case-I under the action of gravity alone

When the drop falls its velocity increases first. After some time the forces acting on it balances each other and the drop falls with terminal velocity (v1).

U + F W v₁ ↓

At equilibrium:

U + F = W
m′g + 6πηrv1 = mg
σ × 4/3 πr3g + 6πηrv1 = ρ × 4/3 πr3g
6πηrv1 = 4/3 πr3g(ρ − σ)
r = √[9ηv1 / 2g(ρ − σ)]
v = volume of displaced air
σ = air density
η = coefficient of viscosity
ρ = mass density

Case-II under the combined action of gravity and electric field

Now the uniform electric field is applied along with gravity such that the drop moves upward with velocity (v2).

U + Fₑ v₂ ↑ F + W

At equilibrium:

U + Fe = W + F
σ × 4/3 πr3g + qE = ρ × 4/3 πr3g + 6πηrv2
qE = 4/3 πr3g(ρ − σ) + 6πηrv2
From case-I:
qE = 6πηrv1 + 6πηrv2
q = 6πηr(v1 + v2) / E

Note: If the drop falls downward after applying electric field then,

q = 6πηr(v1 − v2) / E

Importance of Millikan’s Oil Drop Experiments

  1. Millikan’s oil drop experiment is a direct and precise method for determination of electronic charge and gives good result.
  2. This experiment shows that the smallest possible charge is the charge of an electron which is e = −1.6 × 10−19 C.
  3. This experiment proves the quantization of charges, i.e. q = ne, where n = 1, 2, 3 … an integer and e = −1.6 × 10−19 C, charge of an electron.
  4. Millikan’s oil drop experiment along with Thomson’s e/m experiment can be used to calculate the mass of an electron.

Motion of Charged Particle in Magnetic Field (B)

×××× ××××× ××××× ×××× ×××× v F B

Consider a beam of electron moving with velocity v enters normally into a uniform magnetic field B such that B ⟂ v as shown in fig. The magnetic force acting on electron is given by Fm = Bev. This force provides necessary centripetal force and deflect the electron in a circular path. So,

Fm = Fc
Bev = mv2/r
r = mv/Be    …(2)

This expression gives radius of circular path.

Since,

v = ωr
v = 2πf × mv/Be
f = Be/2πm    …(3)

This gives frequency of electron.

Also, time period:

T = 1/f
T = 2πm/Be
If θ = 0° or 180° (parallel or antiparallel), electron follows straight path.
If θ = 90°, electron follows circular path.
If θ is other than 0°, 180° and 90°, electron follows helical path.
Radius of helical path: r = mv sinθ / Be

Motion of Electron Beam in Electric Field

+ v P(x,y) y d D

Consider a beam of electron moving horizontally with velocity v enters normally into a uniform electric field E as shown in figure. Let the length of each plate is D and V be the potential difference between the plates separated by distance d.

The electric field between plates is E = V/d    …(1)

The electric force acting on electron is:

Fe = eE    …(2)

Let after time t, the electron is at point P(x,y).

Along x-axis

Sx = x,   ux = v,   ax = 0
Sx = uxt + 1/2 axt2
x = vt
t = x/v    …(3)

Along y-axis

Sy = y,   uy = 0,   ay = Fe/m = eE/m
Sy = uyt + 1/2 ayt2
y = 0 × t + 1/2 (eE/m)(x/v)2
y = (eE/2mv2)x2

This equation is similar to y = kx2 which is parabola.

Vertical component of velocity while coming out from electric field

Vy = uy + ayt
Vy = 0 + (eE/m)(D/v)
Vy = eED/mv

Resultant velocity with which electron comes out

Vr = √(Vx2 + Vy2)
Vr = √[v2 + (eED/mv)2]

Angle made by resultant velocity with horizontal

tanθ = Vy/Vx
tanθ = eED/mv2

Specific Charge

It is the ratio of charge to mass of a particle.

Specific charge = e/m

Principle: Cross-Field

It is the field in which both uniform electric field and uniform magnetic field are present kept perpendicular to each other such that the effect of one field is canceled by the other.

J.J. Thomson’s Experiment to Determine Specific Charge of an Electron

Principle

It is based on the principle of cross-field i.e. when an electron is passed through a cross-field the net force acting it is zero and it goes undeviated.

Construction

fluorescent screen C A + magnetic field S₁ S₂ O

It consist of an evacuated glass tube having a fluorescent screen. A cathode connected to a battery an anode having small hole on it.

Working

The cathode gets heated due to a battery electron are emitted. Those electrons are accelerated by the battery connected between cathode and anode.

  • In the absence of field the electron goes straight and strikes the screen at central pole.
  • In the presence of magnetic field electron bends downward and strikes the screen at S2.
  • In the presence of electric field electron bends upward and strikes the screen at S1.
  • In the presence of cross field electron goes straight and strikes the screen at O. At this condition Fm = Fe.
Bev = eE
v = E/B    …(1)

In cross field electric force is equal to magnetic field:

Fe = Fm
eE = Bev
v = E/B    …(1)

Here, work done by potential = K.E. of electrons.

eV = 1/2 mv2
e/m = v2/2V
e/m = (E/B)2/2V
e/m = E2/2VB2

Using E = V/d:

e/m = V2 / 2Vd2B2

This expression gives value of e/m which was found to be:

e/m = 1.8 × 1011 C/kg

Millikan’s Experiment Formulae

r = √[9ηv1 / 2g(ρ − σ)]
q = 6πηr(v1 + v2) / E
E = V/d    electric field between plates

Motion in Electric Field

Vr = √[v2 + (eED/mv)2]
θ = tan−1(eED/mv2)
y = (eE/2mv2)x2
Vy = eED/mv

Motion in B

r = mv/Be
f = Be/2πm
T = 2πm/Be

J.J. Thomson’s

e/m = 1.8 × 1011 C/kg
v = E/B

If drop remains stationary / balanced equilibrium / rest:

qE = mg

Exercise – 20

Conceptual Problem

1) Compare the specific charge of an electron with that of a proton.

Specific charge = e/m.

Electron:
e/m = −1.6 × 10−19 / 9.1 × 10−31
= −1.76 × 1011 C/kg

Proton:

charge = 1.6 × 10−19 C
mass = 1.67 × 10−27 kg
Specific charge of proton = 1.6 × 10−19 / 1.67 × 10−27
= 9.58 × 107 C/kg

Comparison

  • The magnitude of the specific charge of an electron is about 1836 times greater than that of a proton.
  • Electron’s specific charge is negative, while proton’s is positive.
  • The electron has a much higher specific charge than the proton due to its extremely small mass even though both have the same specific charge.
The final sentence above is preserved exactly from the source even though its wording is internally inconsistent.

2) Write down expressions for acceleration of a moving charge θ in parallel and perpendicular magnetic field.

θ = tan−1(eED/mv2)
The source provides the angle expression above under this question; no separate acceleration formula is written there.

3)

No answer is written for question 3 on this page.

What will be the expression for the charge of an oil drop if the electric field force is greater than its weight?

If the electric force acting on the oil drop is greater than its weight, then the drop will move upward.

4) Beams of electrons and protons having the same initial K.E. enter normally into an electric field, which beam will be more curved? Justify.

When beams of electron and proton with the same initial kinetic energy enter normally (perpendicular) into electric field, the electron beam will curve more than the proton beam.

Here force due to electric field:

The electric force on a charged particle is F = qE.
So force magnitude is same on both but in opposite direction due to opposite charge signs.

Acceleration:

a = F/m = qE/m
So, electron accelerates more than proton.

Now,

K.E. = 1/2 mv2
v = √(2 K.E./m)    since both have same K.E.

Electron beam curved more than proton beam in an electric field because:

  • much smaller mass
  • greater acceleration for the same force
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