Electro Magnetic Wave, Cheat Sheet of Physics

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Typology: Cheat Sheet

2025/2026

Available from 05/22/2026

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Displacement Current
Maxwell observed that Ampere’s circuital law cannot
be applied between the plates of the capacitor.
When the circuit is closed, conduction current flows
from the plate P of the capacitor to the other plate
through the conducting wires. Maxwell suggested that
due to time varying electric field between the plates,
an electric current, called displacement current (ID),
also flows across the space between the plates of the
capacitor.
Maxwell pointed out that in Ampere’s circuital law, the
current I should be treated as total current i.e., the sum
of the conduction current IC and displacement current
ID and modified the law as 0
.( )
CD
B dl I I
=m+

It is called the Ampere-Maxwell’s circuital law.
The displacement current is defined as
0
E
D
d
I
dt
φ
= ε
( )
0.
DE
EA
I EA
t
ε
= φ=
0
VA V
E
dt d

=ε=


A
V
CC
td
0
ε

= =


Maxwell’s Equations
and Lorentz Force
Gauss’s law of magnetism: It states that the net
magnetic flux crossing any closed surface is always
zero.
Mathematically, .dS 0B=
Maxwell’s Equations
1. 0
/E dA Q= ε
(Gauss’s Law for electricity)
2. 0B dA =
(Gauss’s
Law for magnetism)
3.
B
d
Ed dt
Φ
=

(Faraday’s
Law)
4. 0 00
E
c
d
Bd i
dt
Φ
=m +m ε

(Ampere
- Maxwell Law)
Lorentz force: The vector sum of electric force and
magnetic force on any charged particle is called the
Lorentz force.
v
=
F qE B
The above five equations give a complete description of
all electromagnetic interactions.
Sources of Electromagnetic
Waves
Neither stationary charges nor charges in uniform motion
(steady currents) can be sources of electromagnetic waves.
The former produces only electrostatic field, while the latter
produces magnetic field that, however, do not vary with time.
It is an important result of Maxwell’s theory that accelerated
charges radiate electromagnetic waves.
The frequency of electromagnetic wave naturally
equals the frequency of oscillation of the charge. The
energy associated with the propagating wave comes at
the expense of the energy of the source-the accelerated
charge.
ELECTROMAGNETIC WAVES
8
Chapter
NCERT CRUX
pf2

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Displacement Current

 Maxwell observed that Ampere’s circuital law cannot

be applied between the plates of the capacitor.

 When the circuit is closed, conduction current flows

from the plate P of the capacitor to the other plate

through the conducting wires. Maxwell suggested that

due to time varying electric field between the plates,

an electric current, called displacement current ( I D

also flows across the space between the plates of the

capacitor.

 Maxwell pointed out that in Ampere’s circuital law, the

current I should be treated as total current i.e., the sum

of the conduction current I C and displacement current

I

D

and modified the law as B dl. = m 0 ( IC + ID ) ∫

It is called the Ampere-Maxwell’s circuital law.

 The displacement current is defined as

0

E D

d I dt

φ = ε

( )

0 . D E

EA

I E A

t

ε = φ =

0

VA V

E

dt d

= ε =    

V A

C C

t d

 ε 0  = =    

Maxwell’s Equations

and Lorentz Force

 Gauss’s law of magnetism: It states that the net

magnetic flux crossing any closed surface is always

zero.

Mathematically, (^) ∫ B .dS^^ =^0

Maxwell’s Equations

1. (^) ∫ E^  dA^ =^ Q /ε 0

(Gauss’s Law for electricity)

2. B^ dA^ =^0 ∫

(Gauss’s Law for magnetism)

B d E d dt

(Faraday’s Law)

E c

d B d i dt

= m + m ε ∫

(Ampere - Maxwell Law)

 Lorentz force: The vector sum of electric force and

magnetic force on any charged particle is called the

Lorentz force.

( v )

= ^ + × 

F q E B

The above five equations give a complete description of

all electromagnetic interactions.

Sources of Electromagnetic

Waves

Neither stationary charges nor charges in uniform motion

(steady currents) can be sources of electromagnetic waves.

The former produces only electrostatic field, while the latter

produces magnetic field that, however, do not vary with time.

It is an important result of Maxwell’s theory that accelerated

charges radiate electromagnetic waves.

 The frequency of electromagnetic wave naturally

equals the frequency of oscillation of the charge. The

energy associated with the propagating wave comes at

the expense of the energy of the source-the accelerated

charge.

ELECTROMAGNETIC WAVES

Chapter

NCERT CRUX

Electromagnetic W aves^2

Properties of Electromagnetic

Waves

 Electromagnetic waves travel through vacuum with the

speed of light, where

8

0 0

= = 3 ×10 m/s m ε

c

 The velocity of electromagnetic wave in a medium

v = m ∈ r r

where m r = relative permeability

r = relative permitivity

 The electric and magnetic fields of an electromagnetic

wave are perpendicular to each other and also

perpendicular to the direction of wave propagation.

Hence, these are transverse waves.

 The instantaneous magnitudes of E

and B

in an

electromagnetic wave are related by the expression

E

c B

= (velocity of light)

Energy Carried by Electromagnetic

Waves

 The total instantaneous energy density u is equal to the

sum of the energy densities associated with the electric

and magnetic fields.

2 2 0 0

= + = ε + m

E B

B

u u u E

The components of the electric and magnetic fields of a

plane electromagnetic wave are given by:

E = E

max.

cos ( kx – w t )

B = B

max.

. cos ( kx – w t )

Momentum and Radiation Pressure

First we consider that the electromagnetic wave strikes the

surface at normal incidence and transports a total energy U to

the surface in a time ‘ t ’, if the surface absorbs all the incident

energy, the total momentum ‘ p ’ transported to the surface has

a magnitude

U

p c

= (complete absorption) ...(1)

If the surface is a perfect reflector and incidence is normal

then the momentum transported to the surface is twice that

given by Eq.(1). Therefore,

2 U

p c

= (complete reflection) ...(2)

Intensity of electromagnetic wave is given by

2 4

av

P

I

r

π

( P

av -average power)

Electromagnetic Spectrum

Type Wavelength Range

( λ )

Frequency Range

(Hz)

1. Radiowaves 0.3 to 6 × 10 2 m 10 9 - 5 × 10 5 Hz 2. Microwaves 10 - to 0.3 m 3 × 10 11 - 1 × 10 9 Hz 3. Infrared 8 × 10 - to 10 - m 4 × 10 14 - 3 × 10 11 Hz 4. Visible light 4 × 10 - to 8 × 10 - m 8 × 10 14 - 4 × 10 14 Hz 5. Ultra violet 6 × 10 - to 4 × 10 - m 5 × 10 17 - 8 × 10 14 Hz 6. X-rays 10 - to 3 × 10 - m 3 × 10 21 - 1 × 10 16 Hz 7. γ-rays 0.6 × 10 - to 10 - m 5 × 10 22 - 3 × 10 18 Hz

A P P L E T O N L A Y E R

KENNELLY HEAVISIDE

LAYER

THERMOSPHERE

MESO SPHERE

STRATO SPHERE

TROPO SPHERE

Earth Surface

OZONE LAYER

IONOSPHERE

400km80km 50km 12km