An alternating flux is produced by the alternating current when flowing through a conductor.
Inductance
An alternating flux is produced by the
alternating current when flowing through a conductor. This flux links with the
conductor. The conductor possesses inductance due to these flux linkage. The
flux linkages per ampere is called the inductance.
Thus inductance is given by,
L = ψ / I
where ψ
= Flux linkage in weber-turns and I = Current in amperes.
The inductance of a transmission line is
also a distributed parameter over the length of line. For convenience in
analysis it is taken as lumped as shown in the Fig. 1.7.2.
The fundamental equation used to define
inductance is given by,
e = d τ / dt ....
(1.9.1)
where e is induced voltage in volts and
r is number of flux linkage of the circuit in weber-tums. The number of weber
turns is the product of each weber of flux and the number of turns of the
circuit linked. Each line of flux is multiplied by the number of turns it links
and these products are added to determine total flux linkages.
If constant permeability is assumed for
the medium in which the magnetic field is set up then we have,
Nτ ∝
i i.e. Nτ
= Li
The constant of proportionality is
called inductance
τ = Li / N
Substituting this value in the
fundamental equation we have,
e = d . dt [Li / N] = L/N di/dt
For N number of truns, e = L
(di/dt) .... (1.9.2)
If permeability is not constant then
above equation may also be used but then the inductance is not constant.
Solving equations (1.9.1) and (1.9.2) we
get,
L = (dτ / di) H
With the flux linkage varying linearly
with current then the magnetic circuit has constant permeability.
L = τ/i
H i.e τ = Li Wb-turns
In this equation, i is the instantaneous
value of current. So - represents instantaneous flux linkages. For sinusoidal
alternating current, flux linkages are also sinusoidal. Hence we have,
ψ = LI
The voltage drop due to flux linkage is,
V = j ω LI volts i.e. V = j ω ψ volts
The mutual inductance between the two
circuits is defined as the flux linkages of one circuit due to current in the
second circuit per ampere of current in the second circuit.
If current I2 produces ψ12
linkages with circuit 1, the mutual inductance is,
M12 = ψ12 / I2
The voltage drop in circuit 1 is given
by,
V1 = j ω M12 I2
= j ω ψ12 volts
Mutual inductance is important in
considering the influence of power lines on telephone lines and the coupling
between parallel power lines.
Review Question
1. Write a note on inductance of a transmission line.
Transmission and Distribution: Unit I: Transmission Line Parameters : Tag: : - Inductance
Transmission and Distribution
EE3401 TD 4th Semester EEE Dept | 2021 Regulation | 4th Semester EEE Dept 2021 Regulation