Inductance of a Co-axial Line m.m.f. round any closed path = current enclosed.
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Transcript of Inductance of a Co-axial Line m.m.f. round any closed path = current enclosed.
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Inductance of a Co-axial Inductance of a Co-axial Line Line
m.m.f. round any closed path = current enclosed
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Inductance of a Co-axial Inductance of a Co-axial LineLine
And Flux density:And Flux density:
For 1 m length, axially, the flux linkages
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Inductance of a Co-axial Inductance of a Co-axial LineLine
This expression for inductance is validThis expression for inductance is valid
for the space between r and R. However,for the space between r and R. However,
flux is also "linked" inside the inner andflux is also "linked" inside the inner and
outer conductors. Internal flux linkagesouter conductors. Internal flux linkages
for radius x < r. for radius x < r.
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Inductance of a Co-axial Inductance of a Co-axial LineLine
since the flux links only ( ) of one turn since the flux links only ( ) of one turn
L2
Thus for h.f. applications the inductance of a coaxial line is taken as:
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Capacitance of a Coaxial Capacitance of a Coaxial Line Line
Assign a line charge of 1 C/m to inner and Assign a line charge of 1 C/m to inner and outerouter
conductors.conductors.
Electric flux density at x =Electric flux density at x =
Electric field intensity
Hence the Capacitance is
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Characteristic Impedance Characteristic Impedance Coaxial LineCoaxial Line
neglecting internal linkages
If r =1 and r = 1
If , for example. ( )
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Derivation of General Derivation of General Transmission Line Transmission Line
Equations Equations Representation of a Uniform Representation of a Uniform
Transmission Line Transmission Line
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Derivation of General Derivation of General Transmission Line Transmission Line
Equations Equations R = distributed resistance/metreR = distributed resistance/metre
G = distributed conductance/metreG = distributed conductance/metre
L = distributed inductance/metreL = distributed inductance/metre
C = distributed capacitance/metreC = distributed capacitance/metre
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Derivation of General Derivation of General Transmission Line Transmission Line
EquationsEquationsSetting up Differential EquationsSetting up Differential Equations
Potential drop across x is:-
The decrease in current across x is
where ix + vx are functions of both x and time.
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Derivation of General Derivation of General Transmission Line Transmission Line
EquationsEquations
LetLetand
where Ix + V x are phasor quantities and are functions of x alone.
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Derivation of General Derivation of General Transmission Line Transmission Line
EquationsEquationsHence differentiating with respect to xHence differentiating with respect to x
which becomes, on using
or
where
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Derivation of General Derivation of General Transmission Line Transmission Line
EquationsEquations is termed the propagation coefficient.is termed the propagation coefficient.
The general steady state solution of Equation is:-
Vx = Aex + Be-x
I =
A
z0ex e-x
z0
B-
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Lossless or High-frequency Lossless or High-frequency Lines Lines
Many transmission lines operate at Many transmission lines operate at relativelyrelatively
high frequencies. Under those high frequencies. Under those conditions theconditions the
lossy terms, R and G, pale intolossy terms, R and G, pale into
insignificance when compared with insignificance when compared with L L and and
C. C.
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Traveling Waves Traveling Waves The basic equations for the transmission The basic equations for the transmission
lineline
are: are:
Having solutions of the form
or knowing as we now do that we have 2 waves, incident, V+ and reflected, V- then we can rewrite the equations as:-
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Traveling WavesTraveling Wavesandand
If z = 0 and we define this as the receiving end, then:-
If the voltage reflection coefficient, , is defined as the ratio of the reflected wave to the incident wave then, = V-/V+ . Hence:-
&
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Traveling WavesTraveling WavesIf the line is considered as lossless then neither the If the line is considered as lossless then neither the
incidentincident
or reflective waves decay as they progress along the or reflective waves decay as they progress along the line.line. Considering the currents;
then
And at the load, z = 0 then
Hence the Current reflection Coefficient = - Voltage reflection Coefficient
Transmission Coefficients are 1 + reflection coefficients; = 1+
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Traveling WavesTraveling Waves
The value of the maximum voltage isThe value of the maximum voltage is
A + |A + ||A.|A.
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The condition for no standing waves is The condition for no standing waves is thatthat
||| = 0, no reflection and the line is | = 0, no reflection and the line is matched.matched.
Standing WavesStanding Waves
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Standing WavesStanding WavesUsing some imagination the current is Using some imagination the current is
seenseen
as being at right angles to the voltage, as being at right angles to the voltage, i.e.i.e.
space quadrature space quadrature
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Reflections on Unmatched Reflections on Unmatched Lines Lines
We have already seen that transmissionWe have already seen that transmission
lines that are not matched have bothlines that are not matched have both
incidentincident and and reflected wavesreflected waves on them. on them. WeWe
will now consider expressing the will now consider expressing the equationsequations
previously derived in terms of previously derived in terms of reflectionreflection
coefficients.coefficients.