1. 2. 3. 4. 5. In Rn Eth Rth VL(Min) VL(Max) IL(Min) IL(Max) R₁ max pwr
1. 2. 3. 4. 5. In Rn Eth Rth VL(Min) VL(Max) IL(Min) IL(Max) R₁ 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
I have included the circuit in question as well as the questions/data table, thanks.
![1.
2.
3.
4.
5.
In
Rn
Eth
Rth
wwww
VL(Min)
VL(Max)
IL(Min)
IL(Max)
RL max pwr](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F0e568bb0-d12e-4c46-a939-67d274aff65f%2F563b8695-7af5-4e2f-a548-1c95627413d7%2Frpfu2tk_processed.jpeg&w=3840&q=75)
Transcribed Image Text:1.
2.
3.
4.
5.
In
Rn
Eth
Rth
wwww
VL(Min)
VL(Max)
IL(Min)
IL(Max)
RL max pwr
![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.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F0e568bb0-d12e-4c46-a939-67d274aff65f%2F563b8695-7af5-4e2f-a548-1c95627413d7%2Fsiskvrv_processed.jpeg&w=3840&q=75)
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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Step 1: Summarize the data.
VIEWStep 2: 1. Determine E_th.
VIEWStep 3: Determine R_th.
VIEWStep 4: 2. Determine the Norton's equivalent circuit.
VIEWStep 5: 3. Determine V_L(min) and V_L(max).
VIEWStep 6: 4. Determine I_L(min) and I_L(max).
VIEWStep 7: 5. Determine the value of R_L so that maximum power transferred to it and P_max.
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