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Insertion Loss and Transmission Co-Efficient: V Z I e e V Z V

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Insertion loss and Transmission co-efficient

[
V ( z ) = V0+ e − jβz + ΓL e + jβz ] (1)
V0+
I ( z) =
Z0
[e − jβ z
− ΓL e + jβz ] (2)

(3)
(4)
TRANSMISSION CO-efficient

(5)

Equ. 5 can be written as

(6)
Equating equ 3 and 6 at Z=0 gives
T=1+Γ (7)

(8)

Substituting (8) in (7)


(9)
INSERTION LOSS

(10)
VOLTAGE STANDING WAVE RATIO (VSWR(ρ))

ρ= (11)

(12)
VSWR
Substituting 12 in 11 gives

ρ= (13)
ISWR
We can express the current standing wave ratio as

I ( z ) max 1 + ΓL
ρ = ISWR = = (14)
I ( z ) min 1 − ΓL
where
I max ( z ) = I 0+ (1 + ΓL )
(15)
I min ( z ) = I (1 − ΓL )
+
0

INPUT IMPEDANCE OF TL

Zin Z=0
Z=-l
Voltage and current on any point in LOSSLESS TL
(1)

(2)
INPUT IMPEDANCE OF TL

(5)

(6)
(6)

(7)

(6)

(8)

(6)

(7 )and (8)
Maximum Impedance, Minimum Impedance and Normalized Impedance

Vmax V0 (1 + ΓL ) (1 + ΓL )
+

Z max = = + = Z0
I min V0 (1 − ΓL ) (1 − ΓL )
Z0
Vmin V0+ (1 − ΓL )
(1 − ΓL )
Z min = = + = Z0
I max V0 (1 + ΓL ) (1 + ΓL )
Z0

Normalized zmax and zmin are obtained by dividing


the Zmax and Zmin by Z0
(1 − ΓL ) = 1
(1 + ΓL ) = ρ z min( norm ) =
z max( norm ) = (1 + ΓL ) ρ
(1 − ΓL )
We can conclude that Vmax,Imin, Zmax and
VSWR(ρ) points in Transmission line are
same. Similarly Vmin,Imax, Zmin and
1/VSWR(1/ρ) are same point
Determination of Z0
Measure the sending end impedance with
receiving end short-circuited (ZL=0)
Z sc = jZ 0 tan βl

Measure the sending end impedance with


receiving end open-circuited (ZL=α)
Z oc = − jZ 0 cot βl

Thus
Z 0 = Z sc Z oc
General Form of input impedance
For lossless line
γ=jβ

We know
tanh(jβl)=jtan βl
Short circuited line
Z L + Z 0 tanh( jβl ) Z sc = Z 0 tanh γl
Z in = Z 0
Z 0 + Z L tanh( jβl )
Z + Z 0 tanh(γl )
Open circuited line
Z in = Z 0 L
Z 0 + Z L tanh(γl ) Z oc = Z 0 coth γl

We can find the propagation constant


1 Z sc
γ = tanh −1
l Z oc
P-1
The open circuit and short impedances measured at the input
terminals of a lossless transmission line of length 1.5 (m), which is
less than a quarter wavelength are –j54.6 (Ω) and j103 (Ω)
respectively. Find (i) Z0 and γ of the line. (ii) Without changing the
operating frequency find the input impedance of a short-circuited line
that is twice the given length and (iii) How long should the short-
circuited line be on order for it to appear as an open circuit at the
input terminals
P-2
Two half-wave dipole antenna each with an impedance of 75
Ω are connected in parallel through a pair of
transmission lines and the combination is connected to a
feed transmission line. All lines are 50 Ω and lossless.
(i) Calculate the input impedance of the antenna-terminated
line at the parallel juncture.
(ii) Calculate the input impedance of the feed line.

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