Title: 16.360 Lecture 8
116.360 Lecture 8
- short circuit line
- open circuit line
- quarter-wave transformer
- matched transmission line
216.360 Lecture 8
short circuit line
B
Ii
A
Zg
Vg(t)
sc
VL
Z0
Zin
ZL 0
l
z 0
z - l
ZL 0, ? -1, S ?
V(z) V0 )
-
-2jV0sin(?z)
i(z)
)
2V0cos(?z)/Z0
V(-l)
Zin
jZ0tan(?l)
i(-l)
316.360 Lecture 8
short circuit line
V(-l)
Zin
jZ0tan(?l)
i(-l)
- If tan(?l) gt 0, the line appears inductive,
j?Leq jZ0tan(?l),
- If tan(?l) lt 0, the line appears capacitive,
1/j?Ceq jZ0tan(?l),
- The minimum length results in transmission line
as a capacitor
416.360 Lecture 8
open circuit line
B
Ii
A
Zg
Vg(t)
oc
VL
Z0
Zin
ZL ?
l
z 0
z - l
ZL 0, ? 1, S ?
V(z) V0 )
-
i(z)
)
2jV0sin(?z)/Z0
V(-l)
oc
Zin
-jZ0cot(?l)
i(-l)
516.360 Lecture 8
Application for short-circuit and open-circuit
616.360 Lecture 8
Transmission line of length l n?/2
tan(?l) tan((2?/?)(n?/2)) 0,
Zin(-l)
ZL
Any multiple of half-wavelength line doesnt
modify the load impedance.
716.360 Lecture 8
Quarter-wave transformer l ?/4 n?/2
?l (2?/?)(?/4 n?/2) ?/2 ,
-j ?
e
?
)
(1
Zin(-l)
Z0
-j ?
e
-
?
(1
)
Z0²/ZL
816.360 Lecture 8
Matched transmission line
- ZL Z0
- ? 0
- All incident power is delivered to the load.
916.360 Lecture 8
Today Power flow on a lossless transmission line
- Instantaneous power
- Time-average power
j?z
e
V(z) V0 ( )
?
-
i(z)
)
?
At load z 0, the incident and reflected
voltages and currents
i
i
V V0
i
r
-
r
V V0
i
1016.360 Lecture 8
i
i
i
P(t) v(t) i(t) ReV exp(j?t) Re i
exp(j?t)
ReV0exp(j? )exp(j?t) ReV0/Z0 exp(j?
)exp(j?t)
(V0²/Z0) cos²(?t ? )
r
r
r
P(t) v(t) i(t) ReV exp(j?t) Re i
exp(j?t)
-
-
ReV0exp(j? )exp(j?t) ReV0/Z0 exp(j?
)exp(j?t)
- ?²(V0²/Z0) cos²(?t ? ?r)
1116.360 Lecture 8
Time-domain approach
i
?
T
T
i
Pav
P (t)dt
2?
0
0
(V0²/2Z0)
r
Pav
-?² (V0²/2Z0)
Net average power
i
r
Pav
Pav
Pav
(1-?²) (V0²/2Z0)
1216.360 Lecture 8
Phasor-domain approach
Pav
(½)ReV i
i
Pav (1/2) ReV0 V0 /Z0
(V0²/2Z0)
r
Pav
-?² (V0²/2Z0)
Pav
(1-?²) (V0²/2Z0)
1316.360 Lecture 8
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