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A/C Line Behavior

Module by: Bill Wilson. E-mail the author

If we are going to try to use phasors on a transmission line, then we have to allow for spatial variation as well. This is simple to do, if we just let the phasor be a function of xx, so we have V x V x . How the phasor varies in xx is one of the things we now have to find out.

Let's start with the Telegrapher's Equations again.

Vxt x =(L)Ixt x x V x t L x I x t
(1)
Ixt x =(C)Vxt x x I x t C x V x t
(2)
For Vxt V x t we can now substitute V xeiωt V x ω t and for Ixt I x t we plug in I xeiωt I x ω t . So we get:
( V xeiωt) x =eiωt t x V x ω t t ω t
(3)
and
( I xeiωt) x =eiωt t x I x ω t t ω t
(4)
We take the derivative with respect to time, which brings down a iω ω and then we cancel the eiωt ω t from both sides of each equation:
V x x =(iωL I x) x V x ω L I x
(5)
and
I x x =(iωC V x) x I x ω C V x
(6)
Viola! In one simple motion, we have completely eliminated the time variable, tt, from our equations! It is not really gone, of course, for once we figure out what V x V x is, we have to multiply it by eiωt ω t and then take the real part before we can extract once again, the actual Vxt V x t that we want. Nonetheless, insofar as the telegrapher's equations are concerned, tt has disappeared from the radar screen.

To solve these we do just as we did with the transient problem. We take a derivative with respect to xx of Equation 5, which gives us a I x x x I x on the right hand side, for which we can substitute Equation 6, which leaves us with

2 V x x 2 2 = V x x 2 2 V x V x
(7)
(- times - is +, but ii=-1 -1 and so we have a - in front of the ω2 ω 2 ). We then re-write Equation 7 as
2 V x x 2 2 +ω2LC V x=0 x 2 2 V x ω 2 L C V x 0
(8)
The simplest solution to this equation is
V x= V 0 e±iωLCx V x V 0 ± ω L C x
(9)
from which we can then get the actual voltage signal
Vxt= V xeiωt= V 0 ei(ωt±ωLCx) V x t V x ω t V 0 ± ω t ω L C x
(10)
Note that we could factor out an eiωLC ω L C , from the exponent, which, since it is just a constant, we could include in V 0 V 0 (and call it V 0 ' V 0 ' , switch the order of xx and tt, and write Equation 10 as
Vxt= V 0 ' ei(x±1LCt) V x t V 0 ' ± x 1 L C t
(11)
which looks a lot like the "general" fx±vt f ± x v t solution we were talking about earlier!

The number ωLC ω L C is special. It is usually represented with a Greek letter ββ and is called the propagation coefficient. Thus we have

Vxt= V 0 ei(ωt±βx) V x t V 0 ± ω t β x
(12)
As previously, a point on the wave of constant phase requires that the argument inside the parenthesis remains constant. Thus if V x 1 t 1 V x 1 t 1 is going to equal V x 2 t 2 V x 2 t 2 (i.e. what was at point x 1 x 1 at t 1 t 1 is now at x 2 x 2 at time t 2 t 2 it must be that
ω t 1 ±β x 1 =ω t 2 ±β x 2 ± ω t 1 β x 1 ± ω t 2 β x 2
(13)
or
x 2 x 1 t 2 t 1 =ΔxΔt=±ωβ=±ωωLC=±1LC v p x 2 x 1 t 2 t 1 Δ x Δ t ± ω β ± ω ω L C ± 1 L C v p
(14)
Which one again, defines the phase velocity of the wave. Other relationships to keep in mind are
β=2πλ β 2 λ
(15)
λ= v p f=ωβω2π=2πβ λ v p f ω β ω 2 2 β
(16)
The first comes from the fact that the wave varies in xx as eiβx β x . Thus when x=γ x γ , the wavelength, βγ β γ just increases by 2π 2 , to get the phasor to go through one full rotation. Note also, as before, the choice of the minus sign in the ± in Equation 12 represents a wave going in the x x direction, while the choice of the + sign will give a wave going in the x x direction. Clearly, by starting out taking the x-derivative of the equation for Ixt I x t we would end up with
Ixt= I 0 ei(ωt±βx) I x t I 0 ± ω t β x
(17)
Let's consider the two phasors then, and define the voltage phasor associated with the positive going voltage wave as
V plus x= V + e(iβx) V plus x V + β x
(18)
and the negative voltage phasor as
V minus x= V - eiβx V minus x V - β x
(19)
We should keep in mind that both V + V + and V - V - can be, and probably are, complex numbers. (From now on we will drop the little ~ over the variables because its very tedious to get it to show up with this word processor. You will just have to keep in mind that any variable we do not explicitly put inside absolute value markers (i.e. | V + | V + ) is going to be, in general, a complex number). We will, of course, have similar expressions for the positive and negative going current waves.

Let's consider the positive going current and voltage waves, and plug them into Equation 5.

( V + e(iβx)) x =(iωL I + e(iβx)) x V + β x ω L I + β x
(20)
The x-derivative brings down a (iβ) β , the e(iβx) β x 's cancel, and we have
V + =iωLiβ I + V + ω L β I +
(21)
But, since β=ωLC β ω L C we have
V + =LC I + Z 0 I + V + L C I + Z 0 I +
(22)
as we had before.

So, what has changed? Not much from the case of transients on a line. We will now assume we have a steady state problem. This means we turned on the generator a long time ago. We assume that it has been connected to the line long enough so that all transient behavior has died away, and that voltages and currents are not changing any more (except oscillating at frequency ωω, of course).

If the line is semi-infinite (or matched with a load equal to Z 0 Z 0 ) Figure 1 then it is pretty obvious that

V + = Z 0 Z 0 + Z g V g V + Z 0 Z 0 Z g V g
(23)
where Z g Z g is the source impedance, and V g V g is the source voltage phasor.
Figure 1
A Wave On a Semi-Infinite Line
A Wave On a Semi-Infinite Line (7.04.png)

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