* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Sample Problem Topic: Thévenin and Norton
Mercury-arc valve wikipedia , lookup
Immunity-aware programming wikipedia , lookup
Audio power wikipedia , lookup
Power factor wikipedia , lookup
Electrification wikipedia , lookup
Ground (electricity) wikipedia , lookup
Pulse-width modulation wikipedia , lookup
Power inverter wikipedia , lookup
Electric power system wikipedia , lookup
Variable-frequency drive wikipedia , lookup
Two-port network wikipedia , lookup
Three-phase electric power wikipedia , lookup
Voltage regulator wikipedia , lookup
Electrical substation wikipedia , lookup
Opto-isolator wikipedia , lookup
Electrical ballast wikipedia , lookup
History of electric power transmission wikipedia , lookup
Resistive opto-isolator wikipedia , lookup
Power engineering wikipedia , lookup
Stray voltage wikipedia , lookup
Surge protector wikipedia , lookup
Power electronics wikipedia , lookup
Voltage optimisation wikipedia , lookup
Current source wikipedia , lookup
Switched-mode power supply wikipedia , lookup
Buck converter wikipedia , lookup
Mains electricity wikipedia , lookup
Sample Problem Topic: Thévenin and Norton equivalents (Maximum Power Delivery) Statement of Problem: Given the circuit shown in the figure below Knowing that RL has been tuned to get the maximum power transfer through itself: Find the numerical value of RL, as well as the maximum power transferred to RL. Solution In this problem, we have a dependent source. This means we need to solve for the Thevenin equivalent using different methods than when we did with all independent sources. First, we will determine the VTH voltage, then, we can determine RTH. Note: To get maximum power delivered, you want RLOAD to equal the RTH calculated. Essentially, we are load matching to ensure the maximum power delivered. Since we have a dependent voltage source, we use the Mesh Current analysis method to solve the circuit. We are going to determine the labeled currents in the diagram below, and then calculate the voltage across the load resistor. (Note: The Load resistor is in parallel with the 40 ohm resistor, we can calculate that voltage). We define the terminals as shown above. Mesh Current Analysis: Bottom left branch: 480 + 6 π1 β π2 + 40 π1 β π3 + 4 π1 Top Branch: 4 π2 + 8 π2 β π3 + 6 π2 β π1 = 0 Bottom Right Branch: β20 ππ½ + 2 π3 + 40 π3 β π1 + 8 π3 β π2 = 0 As before, with an added unknown, we need the constraint equation as follows: ππ½ = π1 β π2 Using a linear solve(r), I1 = -99.6A I2 = -78 A I3 = -100.8A iB = -21.6A Using these currents, we can solve for VTH: 40(i1-i3) = 40(-99.6A β (-100.8A)) = 48V Now that we have solved for the Open Circuit Voltage as seen by RL, we will proceed to short the terminal(s), and then perform another Mesh Current analysis to determine the RTH. Note: Since the terminals A and B have been shorted, the contribution of the 40 ohm resistor is ignored. Another Mesh Current Analysis: 480 + 6 π1 β π2 + 4 π1 = 0 4 π2 + 8 π2 β π3 + 6 π2 β π1 = 0 β20 ππ½ + 2 π2 + 8 π3 β π2 = 0 Again, there is a dependent constraint equation: ππ½ = π1 β π2 Again, solving the circuit with a linear solve function, I1 = -92A I2 = -73.33A I3 = -96A IΞ² = -18.67A iSC =-92A β( -96A) = 4A Solving for RTH: = VOC/ISC =12β¦ Note: We know that the maximum power dissipated is when RL is matched to RTH. Thus, we solve this circuit as if RL was attached to the Thevenin Equivalent. P delivered = I2R = (48V/24β¦)2 * 12 = 48 Watts.