Circuit Theorems Circuit Theorems Overview z z z Dr. Mustafa Kemal Uyguroğlu Linearity Property z z Linearity Superpositions Source Transformation Thévenin and Norton Equivalents Maximum Power Transfer Linearity Property A linear element or circuit satisfies the properties of z Additivity: requires that the response to a sum of inputs is the sum of the responses to each input applied separately. If v1 = i1R and v2 = i2R then applying (i1 + i2) v = (i1 + i2) R = i1R + i2R = v1 + v2 z Homogeneity: If you multiply the input (i.e. current) by some constant K, then the output response (voltage) is scaled by the same constant. If v1 = i1R then K v1 =K i1R Linearity Property z Linearity Property - Example A linear circuit is one whose output is linearly related (or directly proportional) to its input. i0 vs + Linear Circuit i R Solve for v0 and i0 as a function of Vs Suppose vs = 10 V gives i = 2 A. According to the linearity principle, vs = 5 V will give i = 1 A. Linearity Property – Example (continued) Linearity Property - Example Ladder Circuit 3A 5A +6V- 2A +3V- 2A 1A + + + 14 V 8V 5V - - - This shows that assuming I0 = 1 A gives Is = 5 A; the actual source current of 15 A will give I0 = 3 A as the actual value. Superposition Superposition “In any linear circuit containing multiple independent sources, the current or voltage at any point in the circuit may be calculated as the algebraic sum of the individual contributions of each source acting alone.” 1kΩ 1kΩ + V1 + – Vout 1kΩ + – V2 – Superposition 1kΩ How to Apply Superposition 1kΩ 1kΩ + V1 + – V’out z 1kΩ + 1kΩ + – V’out = V1/3 V’’out = V2/3 Vout = V’out + V’’out = V1/3 + V2/3 V’’out 1kΩ + – V2 – z To find the contribution due to an individual independent source, zero out the other independent sources in the circuit. – Voltage source ⇒ short circuit. – Current source ⇒ open circuit. Solve the resulting circuit using your favorite technique(s). Superposition - Problem 2kΩ 2mA Source Contribution 12V 4mA 2kΩ – + 2mA 1kΩ 2kΩ 2mA 1kΩ I’0 I0 I’0 = -4/3 mA 4mA Source Contribution 2kΩ 2kΩ 12V Source Contribution 12V 2kΩ 4mA – + 1kΩ 1kΩ I’’0 I’’0 = 0 2kΩ I’’’0 I’’’0 = -4 mA 2kΩ Final Result I’0 = -4/3 mA I’’0 = 0 I’’’0 = -4 mA I0 = I’0+ I’’0+ I’’’0 = -16/3 mA Example z find v using superposition Superposition Procedure 1. For each independent voltage and current source (repeat the following): a) Replace the other independent voltage sources with a short circuit (i.e., V = 0). b) Replace the other independent current sources with an open circuit (i.e., I = 0). Note: Dependent sources are not changed! c) Calculate the contribution of this particular voltage or current source to the desired output parameter. 2. Algebraically sum the individual contributions (current and/or voltage) from each independent source. one independent source at a time, dependent source remains KCL: i = i1 + i2 Ohm's law: i = v1 / 1 = v1 KVL: 5 = i (1 + 1) + i2(2) KVL: 5 = i(1 + 1) + i1(2) + 2v1 10 = i(4) + (i1+i2)(2) + 2v1 10 = v1(4) + v1(2) + 2v1 v1 = 10/8 V Consider the other independent source KCL: i = i1 + i2 KVL: i(1 + 1) + i2(2) + 5 = 0 i2(2) + 5 = i1(2) + 2v2 Ohm's law: i(1) = v2 v2(2) + i2(2) +5 = 0 => i2 = -(5+2v2)/2 i2(2) + 5 = i1(2) + 2v2 -2v2 = (i - i2)(2) + 2v2 -2v2 = [v2 + (5+2v2)/2](2) + 2v2 -4v2 = 2v2 + 5 +2v2 -8v2 = 5 => v2 = - 5/8 V from superposition: v = -5/8 + 10/8 v = 5/8 V