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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

Power System Analysis and Design (MindTap Course List)
Power System Analysis and Design (MindTap Course List)
6th Edition
ISBN:9781305632134
Author:J. Duncan Glover, Thomas Overbye, Mulukutla S. Sarma
Publisher:J. Duncan Glover, Thomas Overbye, Mulukutla S. Sarma
Chapter6: Power Flows
Section: Chapter Questions
Problem 6.61P
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Pic 1: Circuit to analyze / Background Info

Pic 2: Table of data that I need help on, thank you

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