1. 2. 3. 4. 5. In Rn Eth Rth VL(Min) VL(Max) IL(Min) IL(Max) RL max pwr
1. 2. 3. 4. 5. In Rn Eth Rth VL(Min) VL(Max) IL(Min) IL(Max) RL max pwr
Introductory Circuit Analysis (13th Edition)
13th Edition
ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
Chapter1: Introduction
Section: Chapter Questions
Problem 1P: Visit your local library (at school or home) and describe the extent to which it provides literature...
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Question
Pic 1: Circuit to analyze / Background Info
Pic 2: Table of data that I need help on, thank you

Transcribed Image Text:1.
2.
3.
4.
5.
In
Rn
Eth
Rth
wwww
VL(Min)
VL(Max)
IL(Min)
IL(Max)
RL max pwr

Transcribed Image Text:E = 15 V
R₁
W
4.7 ΚΩ
FIGURE 7-1
R3
680 Ω
RN = RTh
Emh
IN
R₂
ww
3.3 ΚΩ
a
RTh
b
Thévenin's theorem:
Any linear bilateral network may be reduced to a simplified two-terminal
network consisting of a single voltage source, Eh, in series with a single resis-
tor, Rh. Once the original network is simplified, any load connected to the
output terminals will behave exactly as if the load were connected in series
with FTh and RT
+
Norton's theorem:
Any linear bilateral network may be reduced to a simplified two-terminal
network consisting of a single current source, IN, in parallel with a single
resistor, RN. A Thévenin equivalent circuit is easily converted into a Norton
equivalent by performing a source conversion as follows:
VL
RL=0 10 k
(7-1)
(7-2)
When a load is connected across the output terminals, the circuit will behave
exactly as if the load were connected in parallel with IN and RN.
Maximum power transfer theorem:
Maximum power will be delivered to the load resistance when the load
resistance is equal to the Thévenin (or Norton) resistance.
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