• In general, the electric charge possesses a basic important property that it can not be created nor distroyed. In other words if the charge disappears from one point, then it must reappear at some other point. This basic property is called conservation of charge.
General Field Relations for Time Varying Electric and Magnetic
Fields
•
In general, the electric charge possesses a basic important property that it
can not be created nor distroyed. In other words if the charge disappears from
one point, then it must reappear at some other point. This basic property is
called conservation of charge.
•
The basic relation between an electric and magnetic field, starting from
Faraday's law is given by,

•
Intercharging operators at R.H.S. of above equation, we get,

•
But according to vector identity 'curl' of a gradient of a scalar is always
zero. Hence we can write,

•
As R.H.S. of the equation (9.4.3) including curl is zero, we can introduce
negative sign at R.H.S. of the equation (9.4.4).

•
Consider any closed surface. If the current is flowing out of the surface, we
can write
I
= dQ / dt A i.e. C/sec
•
As current is flowing out of the surface, it indicates that positive charge is
going out. So the positive charge is decreasing internally. Let QI
be the internal charge,
I
= - dQI / dt .... (9.4.7)
•
If there is a volume charge ρv, then we can write,

•
Using divergence theorem, converting surface integral to volume integral,
assuming that the volume V is enclosed by the same surface S.

•
Equation (9.4.11) is called equation of continuity of current in point or
differential form.
•
Consider Ampere's circuit law in point or differential form as,

•
Taking divergence on both sides of above equation, we get,

•
According to vector identity, 'divergence of curl' of vector is zero.
•
But
is valid only for static fields. This result is not
consistent with the continuity equation

In
otherwords, Ampere’s circuit
law
is not consistent and needs some modification. Let us consider some unknown
term
. Then we can modify Ampere's circuit law for time varying
fields as,

•
Taking divergence on both the sides, we get,

•
But from the continuity equation for time varying fields,

•
Hence the expression for unknown term can be obtained as,

•
Hence for time varying field, Ampere's circuit law can be written as,

Review Questions
1. What is displacement current ? How is Maxwell's equation
modified to account for it in time varying field ?
2. State and derive equation for continuity under dynamic field
conditions. Derive point form of equation of continuity for time varying
fields.
3. Explain inconsistency of Ampere's law. How it is overcome by
modifying equation of continuity ?
Electromagnetic Theory: Unit IV: Time Varying Fields and Maxwells Equations : Tag: : Time Varying Fields and Maxwell's Equations - General Field Relations for Time Varying Electric and Magnetic Fields
Electromagnetic Theory
EE3301 3rd Semester EEE Dept | 2021 Regulation | 3rd Semester EEE Dept 2021 Regulation