Equations VR Vin EvL v(z, t) - RAzi (z, t) - LAz- V₂(t) = 2 dil dt Δz →→ 0 av (z, t) az di (z, t) əz i(z, t)- GAzv(z + Az; t) - CAZ- di (z, t) at =-Ri(z, t) - L av (z + Az, t) at di (z, t) at av(z, t) at =-Gv(z, t) - C- Vot - v(z + Az, t) = 0 -i (z+Az, t) = 0 di (z, t) at = jwl(z) Phasor Form i(z, t) N v(z, t) ww RAZ dV (z) dz dI (z) dz m LAZ GAZ DZ RAHSOFT Z+AZ : i(z+Az, () CAZ.v(z+Az, t) = −(R+ jwL)I(z), = -(G+ jwC)V(z).

Introductory Circuit Analysis (13th Edition)
13th Edition
ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
Chapter1: Introduction
Section: Chapter Questions
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Explain the equations
Equations
Vect) = 2 dil
dt
VR
Vin
KvL v(z, t) - RAzi (z, t) - LAz-
Δz → 0
av (z, t)
əz
VL
di (z, t)
at
di (z, t)
əz
i(z, t)- GAzv(z + Az; t) - CAZ-
di (z, t)
at
=-Ri(z, t) - L-
av(z+Az, t)
at
av (z, t)
at
= -Gv (z, t) - C-
Vot
- v(z+Az, t) = 0
- i(z+Az, t) = 0
di(z, t)
at
= jwl(z)
Phasor Form
i(z, t)
Z
v(z, t)
www
RAZ
dV (z)
dz
dI (z)
dz
LAZ
GAZ
DZ
==
RAHSOFT
Z+AZ
:
i(z+Az, t)
CAZ.v(z+Az, t)
= −(R+ jwL)I(z),
-(G+ jwC)V(z).
Transcribed Image Text:Equations Vect) = 2 dil dt VR Vin KvL v(z, t) - RAzi (z, t) - LAz- Δz → 0 av (z, t) əz VL di (z, t) at di (z, t) əz i(z, t)- GAzv(z + Az; t) - CAZ- di (z, t) at =-Ri(z, t) - L- av(z+Az, t) at av (z, t) at = -Gv (z, t) - C- Vot - v(z+Az, t) = 0 - i(z+Az, t) = 0 di(z, t) at = jwl(z) Phasor Form i(z, t) Z v(z, t) www RAZ dV (z) dz dI (z) dz LAZ GAZ DZ == RAHSOFT Z+AZ : i(z+Az, t) CAZ.v(z+Az, t) = −(R+ jwL)I(z), -(G+ jwC)V(z).
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