INC 253 Digital and electronics laboratory I Laboratory 2 Kirchhoff’s Law Author: …………………………… ID ………………… Co-Authors: 1. …………………………… ID ………………… 2. …………………………… ID ………………… 3. …………………………… ID ………………… Experiment Date: ………………… Report received Date: ………………… Pre lab Full 10 Results 15 …………………………………… Discussion 25 …………………………………… Questions Conclusion 10 5 Total 65 Comments …………………………………… …………………………………… …………………………………… Marks …………………………………… …………………………………… …………………………………… For Instructor Department of Control System and Instrumentation Engineering Faculty of Engineering King Mongkut’s University of Technology Thonburi Objectives 1. To measure resistance, voltage and current. 2. To verify, experimentally, the relationship between the sum of the voltage drops across series-connected resistors, and the applied voltage. 3. To verify, experimentally, the relationship between the sum of the current entering any junction of an electric circuit and the current leaving that junction. 4. To introduce the concept of maximum power transfer. Equipments Required 1. DC power supply 2. VOM 3. Circuit construction breadboard 4. Digital multimeter Devices Required 1. Resistors; each for 270 Ω, 360 , 470 , 560 ,1 kΩ, 2.2 kΩ. All are 5 % tolerance. Basic Information 1. Kirchhoff’s Voltage Law Kirchhoff‟s voltage law is used to solve complex electric circuits. The law, named for Gustav Robert Kirchhoff (1824-1887), the physicist who formulated it, is the basis for modern circuit analysis. VOLTMETER + V2 V1 A - COM C B + R1 - + R2 IT + E R3 V3 DC D Figure 1 voltage across resistors in a series circuit. In the circuit of Figure 1 , the series resistors R1, R2 and R3 can be replaced by their total or equivalent resistance RT, where 2 INC, KMUTT Lab. 2: Kirchhoff‟s Law RT = R1 + R2 + R3 (1) Use of RT will not affect the total current IT. The relationship between source E is given by Ohm‟s law, , and the voltage (2) Substitute equation (1) in (2) gives E = IT (R1 + R2 + R3 ) = IT R1 + IT R2 + IT R3 (3) Where IT R1 = the voltage drop across R1 = IT R2 = the voltage drop across R2 = IT R3 = the voltage drop across R3 = Equation (3) can now be rewritten as V1 V2 V3 E = VAB + VBC + VCD (4) Equation (4) is the mathematical expression of Kirchhoff‟s voltage law and states that “In a closed circuit or loop the applied voltage equals the sum of the voltage drops in the circuit.” Or can be generalized as follows. “The algebraic sum of the voltages in a closed circuit equals zero.” Applying the convention on sign and Kirchhoff‟s law to closed circuit in Figure 1, we may write the following: - V1 - V2 - V3 + E = 0 (5) 2. Kirchhoff’s Current Law The total current I in a circuit containing resistors connected in parallel is equal to the sum of the currents in each of the parallel branch. This was one demonstration of Kirchhoff‟s current law. However the law is general and applies to any circuit. 3 INC, KMUTT Lab. 2: Kirchhoff‟s Law A IT I1 R1 E I2 R2 B Figure 2 Current through resistors in a parallel circuit. From Figure 2 voltage across the parallel circuit can be found using Ohm‟s law (6) Where is an equivalent resistance of the parallel circuit, From equation (6) is the current passing through . (7) By adding branch current gives (8) Since (9) Therefore (10) Kirchhoff‟s Current Law states that “The current entering any junction of an electric circuit is equal to the current leaving that junction.” States in another way: “The algebraic sum of the currents entering and leaving a junction is zero.” I4 A = 5 1 = A I2 3A I 1= I3 I5 = ? = 2 A Figure 3 Current entering and leaving a junction 4 INC, KMUTT Lab. 2: Kirchhoff‟s Law From Figure 3 Procedure Sections marked * are pre-lab preparation and must be completed BEFORE coming to the lab. 1. Part A. Resistance in a series circuit. 1.1. From the circuit in Figure 4, with E = 12 V, R1 = 470(1 ± 5 %) , R2 = 1(1 ± 5 %) k, compute equivalent resistance between points A and C. Calculate the uncertainty (Maximum permissible error) in the equivalent resistor due to the uncertainty of a given resistors. Enter the calculated value below. * Requivalent = (Rcalculated ± uncertainty) = ………………………… 1.2. Calculate current passing through points A, B and C including voltage drop VR1 and VR2. Record the calculated data in Table 1. A 470 R1 E = 12 V B R2 1k C Figure 4Experimental circuit of part A. * Table 1. IA (mA) IB (mA) IC (mA) VR1 (V) VR2 (V) 5 INC, KMUTT Lab. 2: Kirchhoff‟s Law 1.3. Connect the circuit as Figure 4 using the breadboard. Using your VOM measures equivalent resistance between points A and C (disconnect power supply) record the result at “Requivalent (ohmmeter)” below. Requivalent (ohmmeter) = ( Rmeasured ± uncertainty) = ……………………………… Set dc voltage E = 12.0 V using the digital multimeter. Then apply voltage E between points A and C, measure current using your ammeter and voltage using your voltmeter at specified points and record the data obtained in Table 2. Table 2. Meter range IA (mA) IB (mA) IC (mA) VR1 (V) VR2 (V) 1.4. Find “Requivalent(meas)” calculate using data from Table 2 and record as follow. Requivalent (meas) = ( Rmeas ± uncertainty) = ………………………… Question for part A Explain, if any, the difference of results between computation in step 2 and measurement in step 3. 2. Part B. Resistance in a parallel circuit. 2.1. Compute equivalent resistance between point ‟a„ and ‟d„ of the circuit in Figure 5, with E = 9 V, R1 = 470 (1 ± 5 %) , R2 = 2.2 (1 ± 5 %) k, Calculate the uncertainty (Maximum permissible error) in the equivalent resistor due to the uncertainty of a given resistors. Enter the calculated value below. * Requivalent = (Rcalculated ± uncertainty) = ………………………… 6 INC, KMUTT Lab. 2: Kirchhoff‟s Law a c b Ia E=9V R1 470 Ib R2 2.2 k Ic Id d Figure 5. Current and voltage in parallel circuit Then compute the current passing through points‟ a‟ and „d‟, passing through resistors R1 and R2, Ib and Ic respectively, including computation of voltage drop VR1 and VR2 .Record the calculated data in Table 3. * Table 3. Ia (mA) Ib (mA) Ic (mA) Id (mA) VR1 (V) VR2 (V) 2.2. Connect the circuit as in Figure 5, using your VOM measures equivalent resistance between point „a‟ and „d‟ (disconnect power supply) record the result at “Requivalent (using ohmmeter)”. Requivalent (using ohmmeter) = ( Rmeasured ± uncertainty) = ………………………… 2.3. Set dc voltage supply E = 9 V using the digital multimeter. Then apply the voltage E between points a and d, measure current using your ammeter (open circuit and connect the ammeter) and voltage using your voltmeter at specified points and record the data obtained with meter range in Table 4. Table 4. Meter range Measured Ia (mA) Ib (mA) Ic (mA) Id (mA) VR1 (V) VR2 (V) 2.4. Find “Requivalent(meas)” calculate using data from Table 4 from the relation 7 INC, KMUTT Lab. 2: Kirchhoff‟s Law and record as follow. Requivalent (meas) = ( Rmeas ± uncertainty) = ………………………… 3. Part C. Series – parallel circuit and Kirchhoff’s Law. 3.1. Instead of using direct method of current measurement using ammeter, the current passing through a resistor can be obtained indirectly using voltmeter and Ohm‟s law. From Figure 6, E = 15.0 V, R0 = 560(1 ± 5 %) , R1 = 1 (1 ± 5 %) k and R2 = 470(1 ± 5 %) . Calculate voltage across R0, R1 and R2, that is VR0, VR1, VR2 respectively, as the expected reading of an ideal voltmeter and record them in Table 5. Calculate the corresponding current passing through each resistor, IR0, IR1 and IR2 and record them in Table 5. Calculate the uncertainty in current due to the uncertainty of the given resistors. Show all of your calculations on a separate sheet of paper. a R0 b 560 1k E = 15 V R1 R2 470 c Figure 6. Series- parallel circuit * Table 5 VR0 (V) R0 () VR1 (V) 560 IR0 (mA) R1 () VR2 (V) 1k IR1 (mA) R2 () 470 IR2 (mA) 3.2. Connect the circuit as shown in Figure 6 using the breadboard. Set dc voltage E = 15.0 V using the digital multimeter. Measure voltage drop across each resistor using your voltmeter set to the appropriate range. Record the readings with the selected range in Table 6. Find the corresponding current through each resistor from its voltage drop and record the data in Table 6. * Table 6 Meter range Meter range Meter range VR0 (V) VR1 (V) VR2 (V) R0 () IR0 (mA) 560 R1 () IR1 (mA) 1k R2 () 470 IR2 (mA) 8 INC, KMUTT Lab. 2: Kirchhoff‟s Law Questions for part C 1. State in your own words, the relationship between the voltage drop across resistors and the voltage applied to the entire circuit, and then express your answer as a mathematical formula. 2. State in your own words, the relationship between the currents entering and leaving at junction point “a”, and then express your answer as a mathematical formula. 3. Do your experimental data support your answer in 1 and 2? If not, explain the discrepancy. 4. Part D. Voltage Divider. 4.1. Connect the circuit as shown in Figure 7 using the breadboard. Set dc voltage E = 15.0 V using the digital multimeter. Given R1 = 560 (1 ± 5 %) , R2 = 1(1 ± 5 % ) k . 4.2. Before connecting , estimate the suitable range of voltage before measurement. Ideal voltage drop at point B with respect to point C can be calculated from A R1 E = 15 V 560 B R2 1k RL C Figure 7. Voltage divider circuits. R2 E VBC R R 2 1 Record the result as VBC (calculated). * VBC (calculated) = __________ V Measure the voltage drop across R2 using your VOM as a voltmeter. Select the voltage range that is the most appropriate. Record the data with range as VBC (measured) below. Meter range = _______________V VBC (measured) = ___________ V 4.3. Connect RL = 270(1±5%) Ω as a load parallel to R2 (across point B and point C) of the divider circuit, calculate the voltage drop across RL and its power dissipation. Record the result in Table 7 as “Calculated voltage” and “Calculated 9 INC, KMUTT Lab. 2: Kirchhoff‟s Law power“ respectively. Calculate the uncertainty in power due to the uncertainty of the given resistors. Show all of your calculations on a separate sheet of paper. 4.4. Measure the voltage across the load RL using your voltmeter and record the result as “Measured voltage”. Find power dissipation from P = V2/R and record in Table 7 as “Measured power”. 4.5. Repeat step 3 and 4 with RL = 360 and 470 Ω ( All are ± 5 % tolerance). Table 7 * Calculated voltage (V) RL () * Calculated power (mW) Measured voltage (V) Measured power (mW) 270 360 470 Questions for part D 1. To use voltage divider circuit as in Figure 7 it is desired to have voltage output VBC across R2 when at maximum loaded differs from when at no-load not more than 10 %. How can you give the limit on resistance value or criteria for load selection? 2. Explain the concept of maximum power transfer from source to load using the circuit and data from part D. 3. From circuit of Figure 8. a) Find the current through each resistor. b) Determine the voltages and their proper polarities for each resistor R1 R3 470 820 R2 E1 560 E2 2V E3 4V 6V Figure 8. 10 INC, KMUTT Lab. 2: Kirchhoff‟s Law