Lossless Transmission Lines (Part-V)

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Last updated 6:07 PM on 5/23/26
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27 Terms

1
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Ṽ_g

(i)

<p>(i)</p>
2
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Z_g

(ii)

<p>(ii)</p>
3
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Ĩ_i

(iii)

<p>(iii)</p>
4
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A’

(iv)

<p>(iv)</p>
5
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A

(v)

<p>(v)</p>
6
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Ṽ_i

(vi)

<p>(vi)</p>
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Z_in

(vii)

<p>(vii)</p>
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Generator

(viii)

<p>(viii)</p>
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d = l

(ix)

<p>(ix)</p>
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z = -l

(x)

<p>(x)</p>
11
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Transmission Line

(xi)

<p>(xi)</p>
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Z0

(xii)

<p>(xii)</p>
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d = 0

(xiii)

<p>(xiii)</p>
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z = 0

(xiv)

<p>(xiv)</p>
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Ĩ_L

(xv)

<p>(xv)</p>
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Ṽ_L

(xvi)

<p>(xvi)</p>
17
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Z_L

(xvii)

<p>(xvii)</p>
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z = 0

(xviii)

<p>(xviii)</p>
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Generator-End Equivalent Circuit

From the generator’s viewpoint, the transmission line can be replaced by its input impedance Z_in

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Ṽ_i = ((Ĩ_i)(Z_in))

Input Voltage Ṽ_i: Voltage at the generator end of the line

21
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Ṽ_i = ((Ṽ_g)(Z_in))/(Z_g + Z_in)

Voltage Divider Relation for Input Voltage: Generator-end voltage expressed using source and input impedances

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Ṽ_i = (V0^+)e^(jβl) + Γe^(-jβl)

Input Voltage from Traveling-Wave Expression: Voltage at the line input using incident and reflected waves

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V0^+ = (((Ṽ_g)(Z_in))/(Z_g + Z_in))(1/(e^(jβl) + Γe^(-jβl)))

Incident-Wave Amplitude (V0^+): Forward traveling-wave amplitude expressed in terms of source quantities

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Incident Wave

Wave traveling from the generator toward the load

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Reflected Wave

Wave traveling from the load back toward the generator.

26
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Transmission-Line Boundary Condition at the Load

Condition relating incident and reflected waves through the load impedance

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Transmission-Line Boundary Condition at the Source

Condition relating line voltage/current to the generator source and source impedance.