Series-Parallel Circuits 2 February 2005 Series-Parallel Circuits Objectives • • • • • • Identify series-parallel configuration Analyze series-parallel circuits Apply KVL and KCL to the series-parallel circuits Analyze loaded voltage dividers Determine the loading effect of a voltmeter on a circuit Analyze a Wheatstone bridge circuit 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 2 1 Series-Parallel Circuits 2 February 2005 Analysis of Series-Parallel Circuits • Determine total resistance seen by the source • Determine all branch currents and the source current • Determine all voltage drops 2 February 2005 Series-Parallel Circuits 3 Total Resistance • Identify the parallel resistances, and calculate the equivalent resistance(s) • Identify the series resistance, and calculate the total resistance for the circuit 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 4 2 Series-Parallel Circuits 2 February 2005 Find RT RAB = R1 + R4 R 2 R3 R2 + R3 RT = RAC = RAB + RBC RBC = 2 February 2005 Series-Parallel Circuits 5 Resistance in the Series-Parallel Circuit 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 6 3 Series-Parallel Circuits 2 February 2005 Resistance in the Series-Parallel Circuit 2 February 2005 Series-Parallel Circuits 7 Identify the Nodes and Redraw Circuit Nodes connected only by a short are the same node 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 8 4 Series-Parallel Circuits 2 February 2005 Redrawn Circuit from Slide 8 2 February 2005 Series-Parallel Circuits 9 Current in the Series-Parallel Circuit • Using the total resistance and the source voltage, find the total current by applying Ohm’s law IT = VS RT • Using the current-divider formula, Kirchhoff’s current law (KCL), Ohm’s law, or combinations of these, you can find the current in any branch of a series-parallel circuit 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 10 5 Series-Parallel Circuits 2 February 2005 Write the KCL Equation for Node A ITRAB = I2R2 ITRAB = I3R3 2 February 2005 Series-Parallel Circuits 11 Apply KCL to Each Node • At Node B I2 = I3 + I4 • At Node A IT = I1 + I2 • At Node C IT = I1 + I3 + I4 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 12 6 Series-Parallel Circuits 2 February 2005 Apply KVL to the Series-Parallel Circuit VS = VAB + VBC 2 February 2005 Series-Parallel Circuits 13 KVL in the Series-Parallel Circuit VS = VAB + VBC VBC = VR4 + VR5 = VR3 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 14 7 Series-Parallel Circuits 2 February 2005 Unloaded Voltage Dividers • A voltage divider produces an output which depends upon the values of the dividing resistors • All resistors in an unloaded voltage divider are connected in series • This voltage is the unloaded output voltage 2 February 2005 Series-Parallel Circuits 15 Loaded Voltage Dividers • When a load resistor RL is connected between the output terminal and ground, the output voltage is reduced by an amount that depends on the value of RL • Solve the circuit for RT between node A and ground. • Then solve for the desired voltages or currents 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 16 8 Series-Parallel Circuits 2 February 2005 Load Current and Bleeder Current • Bleeder current is the current left (I3) after the total load current is subtracted from the total current into the circuit • In Power Supply circuits, R3 is used to discharge the filter capacitor when power is removed. • The typical range for the Bleeder current is 0.1IRL2 ≤ IR3 ≤ .2IRL2 2 February 2005 Series-Parallel Circuits 17 Loading Effect of a Voltmeter • When measuring across a resistor, a voltmeter is connected in parallel with the resistor • Being in parallel, the internal resistance of the voltmeter will have a loading effect on the circuit that is being measured • Modern digital voltmeters (DMM) have an internal resistance of 10MΩ 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 18 9 Series-Parallel Circuits 2 February 2005 Loading Effect of a Voltmeter • If the meter resistance is at least one hundred times greater than the resistance across which it is connected, the loading effect can be neglected – the measurement error is less than 1% 2 February 2005 Series-Parallel Circuits 19 Analog Voltmeter Loading In the circuits above, R2 in circuit C is most affected by the Voltmeter Loading, and least affected by circuit A 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 20 10 Series-Parallel Circuits 2 February 2005 Wheatstone Bridge • A Wheatstone bridge is used to precisely measure resistance • A Wheatstone bridge is also applied with transducer measurements, to measure physical quantities such as temperature, strain, and pressure, where small transducer resistance changes may need to be precisely measured – Tiny changes in transducer resistance will unbalance the bridge, thereby providing a measurement reading 2 February 2005 Series-Parallel Circuits 21 Wheatstone Bridge with Transducer Input 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 22 11 Series-Parallel Circuits 2 February 2005 Temperature Transducer 2 February 2005 Series-Parallel Circuits 23 Balancing the Bridge for 0V Output 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 24 12 Series-Parallel Circuits 2 February 2005 Find All Currents and Voltages 2 February 2005 Series-Parallel Circuits 25 Find VL for Each Position of the Switch 2 February 2005 Professor Andrew H. Andersen Series-Parallel Circuits 26 13