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FOWLER CHAPTER 5 LECTURE 6 MULTIPLE LOAD CIRCUITS

FOWLER CHAPTER 5 LECTURE 6 MULTIPLE LOAD CIRCUITS. MULTIPLE LOAD CIRCUITS IF YOU HAVE TWO OR MORE LOADS, THEY CAN BE IN SERIES, PARALLEL OR SERIES-PARALLEL. SUBSCRIPTS: R 1, R 2, ……R N INCIDATES # OF DIFFERENT LOAD RESISTORS.

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FOWLER CHAPTER 5 LECTURE 6 MULTIPLE LOAD CIRCUITS

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  1. FOWLER CHAPTER 5LECTURE 6 MULTIPLE LOAD CIRCUITS

  2. MULTIPLE LOAD CIRCUITS IF YOU HAVE TWO OR MORE LOADS, THEY CAN BE IN SERIES, PARALLEL OR SERIES-PARALLEL. SUBSCRIPTS: R1, R2, ……RN INCIDATES # OF DIFFERENT LOAD RESISTORS. V1 , V2,……..V INCIDATES # OF DIFFERENT VOLTAGES. II , I2 ,………IN INCIDATES # OF DIFFERENT CURRENTS. VT: TOTAL VOLTAGE FOR CIRCUIT. IT : TOTAL CURRENT FOR CIRCUIT. POWER : PT = P1 +P2 …….PN TOTAL POWER FOR CIRCUIT. SERIES CIRCUITS: ONE PATH FOR CIRCUIT FLOW. - + P.99 R1 - - R2 VT + + IT + - R3 CURRENT IS THE SAME IN EACH ELEMENT: IT=I1=I2=I3

  3. IN SERIES CIRCUITS, CURRENT IS THE SAME IN EACH ELEMENT. P.100 AN AMPERE METER PLACED AT ANY POINT IN THE CIRCUIT WILL GIVE THE SAME CURRENT READING. TO FIND TOTAL RESISTANCE IN A SERIES CIRCUIT, ADD EACH RESISTANCE TOGETHER. 2A R1 5Ω R2 10Ω 90 VDC R3 30Ω EXAMPLE: • THERE ARE TWO WAYS TO FIND THE TOTAL RESISTANCE FOR THIS CIRCUIT. • USE OHM’S LAW V=IR, • R=V/I • =90V/2A • =45Ω • OR

  4. VOLTAGE IN SERIES CIRCUITS VOLTAGE IS DIVIDED UP ACROSS EACH LOAD. P.101 KIRCHOFF’S VOLTAGE LAW: THE SUM OF VOLTAGE DROPS AROUND THE CIRCUIT PATH = THE SOURCE VOLTAGE. R1 5Ω 2A THIS CONFIRMS KIRCHOFF VOLTAGE LAW. R2 10Ω 90 VDC R3 30Ω

  5. VOLTAGE DROP AND POLARITY POTENTIAL ENERGY DROP ACROSS A RESISTOR IS KNOW AS A VOLTAGE DROP. SOURCE VOLTAGE PROVIDES THE ENERGY. LOAD RESISTANCE VOLTAGE CONVERTS IT TO ANOTHER FORM. (HEAT IN THIS CASE) POLARITY IN THIS CASE INDCIATES THE DIRECTION OF CURRENT FLOW. CURRENT THRU A LOAD MOVES FROM – TO + (ENERGY CONVERTED FROM ELECTRICAL TO ANOTHER FORM). - + P.101 a b R1 - - I VDC R2 + c +

  6. MEASURING SERIES VOLTAGE. F.5-7 P-102 CHOOSE CORRECT FUNCTION, RANGE AND POLARITY ON THE METER. - + V - + R1 - - R2 VT + + IT - + R3 MEASURE VOLTAGE DROP ACROSS EACH RESISTOR.

  7. FINDING A OPEN IN A SERIES CIRCUITS F.5-8 P-103 IF ANY PART OF THE CIRCUIT IS OPEN CURRENT STOPS,VOLTAGE,POWER ARE REMOVED FROM ALL THE LOADS. 0V V R1 12 V R2 R2 V 0V R3 CIRCUIT PATH IS BROKEN V 0V

  8. FINDING SHORTS IN SERIES CIRCUITS F5-9 P-104 WHEN ONE LOAD IS SHORTED OUT, OTHERS MAY CONTINUE TO OPERATE. 10V,10W 1A L1 15V,25W L2 30V 10V,10W 1.5A L1 SHORT L3 L2 0V,0W 30V 10V,10W L3 IN THIS EXAMPLE LAMPS L1 AND L3 CURRENT AND VOLTAGE INCREASE 50%. THIS INCREASED PWR.TO THE LAMPS WILL LIKELY BURN THEM OUT. 15V,25W

  9. VOLTAGE DIVIDER EQ. CAN BE USED TO FIND VOLTAGE ACROSS ANY RESISITOR IN A SERIES CIRCUIT.( RN) FROM EXAMPLE 5-2 P-105 FIND VR1, P.105 VOLTAGE DIVIDER EQ R1 35Ω 70Ω R2 90V 45Ω R3 IF DOMINANT RESISTOR IS SO MUCH GREATER THEN THE OTHERS IN THE CIRCUIT,THE EFFECTS OF THE SMALLER RESISTOR CAN BE IGNORED.

  10. APPLICATIONS OF SERIES CIRCUITS F5-13,14 P-106 R IS A VARIABLE SERIES RESISTOR(RHEOSTAT) R AS R↓ MOTOR SPEED ↑ AS R↑ MOTOR SPEED ↓ NOT EFFICIENT SINCE R WASTES ENERGY AS HEAT.↑ M 120VAC S 24V L LIGHT INTENSITY CONTROL F.5-14 P-106 WORKS WELL FOR DC ONLY

  11. MAXIMUM PWR. TRANSFER (MPT) GETTING THE MAX. AMOUNT OF PWR. FROM A SOURCE TO A LOAD. MPT OCCURS WHEN THE SOURCE INTERNAL OPPOSITION TO THE CURRENT EQUALS THE LOAD’S OPPOSITION TO THE CURRENT . F.5-16 P-108 RB 3Ω SOURCE RL 3Ω LOAD 12V MPT OCCURS WHEN RB=R1=33Ω PR1=PRB= I x V=2AX12=24W SEE T 5-1 P.108

  12. PARALLEL CIRCUITS MULTILOAD CIRCUIT THAT HAS MORE THEN ONE CURRENT PATH. EACH PATH IS CALLED A BRANCH. EACH BRANCH HAS ITS OWN CURRENT. TOTAL CURRENT IS SPLIT ACROSS EACH BRANCH. EACH BRANCH CURRENT IS INDEPENDENT OF THE OTHERS. IT P.108 I1 I2 I3 R3 V R1 R2

  13. CURRENT IN PARALLEL CIRCUITS IT=IR1+IR2+IR3 : TOTAL CURRENT IS THE SUM OF THE BRANCH CURRENTS. P.109 A B IT IR1 IR3 IR2 V R1 R2 R3

  14. KIRCHHOFF’S CURRENT LAW:: THE SUM OF CURRENTS ENTERING A JUNCTION=SUM OF CURRENTS LEAVING A JUNCTION. (NODE) P.109 CURRENT GOING INTO NODE=CURRENT GOING OUT NODE. 3A+5A+2A=7A+3A 10A=10 A 5A 3A 2A NODE 3A 7A A B AT NODE A: IT IA IB AT NODE B: IR2 IR3 IR1 V R1 R2 R3

  15. KIRCHHOFF’S CURRENT LAW KIRCHHOFF’S VOLTAGE LAW

  16. IF A BREAK IN CURRENT FLOW OCCURS IN A SERIES CIRCUIT LIGHTS GO OUT! IN A PARALLEL CIRCUIT, IF ONE BRANCH IS CUT OFF.THE OTHER BRANCH STILL WORKS AND THAT LAMP GLOWS.

  17. SINCE THESE TWO SOLAR PANELS ARE WIRED IN PARALLEL THE CURRENT THEY PRODUCE IS DOUBLED AND THE VOLTAGE STAYS CONSTANT. IT= I FIRST PANEL +I SECOND PANEL VT=VFIRST PANEL = VSECOND PANEL

  18. UNLIKE SERIES CIRCUITS, THE BRANCH WITH THE LOWEST R VALUE DOMINATES THE CIRCUIT, USING THE MOST CURRENT AND POWER FROM THE SOURCE. R1 1KΩ 10V R2 10KΩ A 10mA A 11mA A 1mA R1 RESISTANCE IS 10 TIMES LESS THEN R2, BUT HAS 10 TIMES THE CURRENT FLOW THRU IT.

  19. RESISTANCE IN PARALLEL CIRCUITS THE TOTAL RESISTANCE OF A PARALLELCIRCUIT IS ALWAYS<THAT OF THE LOWEST BRANCH RESISTANCE. HOW IS THIS POSSIBLE? P.110 10V R1 10KΩ ADD A 2ND RESISTOR IN PARALLEL SINCE VOLTAGE IS THE SAME IN EACH BRANCH IR2=10V/100,000Ω=0.1mA FROM KIRCHHOFF’S CURRENT LAW IT=IRI+IR2 IT=1mA+0.1mA IT=1.1mA RT IS < THE LOWEST BRANCH RESISTANCE. 10V R1 10KΩ R2 100KΩ

  20. P.113 R1 10KΩ R2 100KΩ R3 1KΩ 10V ADD A 3TH RESISTOR R3 TO THIS CIRCUIT, FOLLOW THE SAME LOGIC AS ON THE LAST SLIDE. RT=VT/IT= VT/(I1+I2+I3) ,SINCE IN=VT/RN (OHM’S LAW) RT=VT/(VT/R1+VT/R2+VT/R3) USING ALGEBRAIC MAGIC GIVES RT=1/(1/R1+1/R2+1/R3) RECIPROCAL FORMULA

  21. EXAMPLE 5-3 P-112 R1=20Ω R2=30Ω R3=60Ω RT= 1/( 1/R1+ 1/R2+ 1/R3) RT= 1/( 1/20Ω+ 1/30Ω+ 1/60Ω) RT=1/(6/60)=10Ω IF WE HAVE ONLY TWO RESISTORS IN PARALLEL THEN WE CAN FIND RT USING; RT=R1xR2/(R1+R2) EXAMPLE 5-4 P112 GIVEN R1=27Ω R2=47Ω ,FIND RT RT=R1XR2/(R1+R2) =27X47/(27+47) =1269/74 =17.1Ω IF ALL THE RESISTORS IN A PARALLEL CIRCUIT HAVE THE SAME VALUE. YOU CAN USE THE EQUATION:` RT=R/n TO FIND THE TOTAL RESISTANCE. WHERE n =THE # OF RESISTORS IN THE CIRCUIT. EXAMPLE: GIVEN TWO 100Ω RESISTORS IN PARALLEL, FIND RT RT=R/n = 100/2 =50Ω 20Ω 30Ω 60Ω

  22. MEASURING RESISTANCE IN PARALLEL P.112 MUST DISCONNECT THE RESISTOR BEING MEASURED FROM THE LOAD TO READ THE INDIVIDUAL RESISTOR RESISTANCE,IF YOU DON’T, YOU WILL MEASURE RT R2 R1 R3 Ω R2 R1 R3 Ω RESISTOR LEAD DISCONNECTED

  23. CURRENT DIVIDER FORMULA FOR TWO PARALLEL RESISTORS P.114 2A P.114 IR2 IT IR1 IRI=ITxR2/(R1+R2) IR2=ITxR1/(R1+R2) R1 22Ω R2 47Ω VT FIND IR1= 2X47/(2+47) FIND IR2= 2X22/(2+47) IR1=1.36A IR2=0.897A SAVES THE TROUBLE OF HAVING TO FIND: RT USING 1/R OR: VT USING OHM’S LAW OR: IR1,IR2 USING OHM’S LAW APPLICATIONS OF PARALLEL CIRCUITS. HOME LIGHTING, WALL RECEPECTALES, AUTO WIRING, TV, ETC. CONDUCTANCE IS THE RECIPROCAL OF RESISTANCE,IS THE ABILITY TO CONDUCT CURRENT. G=1/R G IS MEASURED IN SIEMENS P.115

  24. SEE APPENDIX C USEFUL FORMULA’S FOR SERIES CIRCUITS IT=I1=I2…..=In VT=V1+V2…..+Vn RT=R1+R2…..+Rn PT=P1+P2……+Pn VOLTAGE DIVIDER EQ. TO FIND VOLTAGE ACROSS ONLY ONE RESISITOR IN A SERIES CIRCUIT. ____________________________________________________________________________________________________________________ FOR PARALLEL CIRCUITS IT=I1+I2…..+In VT=V1=V2…..=Vn RT=1/(1/R1+1/R2…+1/Rn) PT=P1+P2…….+Pn P.474-475 R1 VT RN V R1 R2 I1 IF ONLY TWO RESISTORS ARE IN PARALLEL, FIND RT USING: IF ALL RESISTORS ARE THE SAME: RT=R/n WHERE n=#OF RESISTORS IT I2 A I1 IT I2 CURRENT DIVIDER FORMULA FOR 2 PARALLEL RESISTORS A

  25. SERIES-PARALLEL CIRCUIT

  26. R1 SERIES PARALLEL CIRCUITS P.117 15Ω V R2 R3 20Ω 30Ω FIND RT FOR THIS CIRCUIT FIRST SOLVE FOR THE PARALLEL PAIR R2,R3 R2,3=R2XR3/(R2+R3) =20X30/(20+30) =600/50 =12Ω R1 15Ω V R2,R3 12Ω NOW FIND RT FOR THE SERIES CIRCUIT RT=R1+R2,3 =15Ω+12Ω =27Ω RT=27Ω V

  27. FIND RT FOR THIS SERIES PARALLEL CIRCUIT R1 40Ω R3 FIND SERIES RESISTANCE FOR R1 + R2 FIRST. V 22Ω R1,2=R1+R2 =40Ω+60Ω =100Ω R2 60Ω R1,2 100Ω R3 22Ω NEXT FIND RT FOR THIS PARALLEL CIRCUIT. V RT = R1,2XR3/(R1,2+R3) RT =100X22/122 =2200/122 =18Ω V RT=18Ω

  28. KIRCHHOFF’S LAWS IN SERIES- PARALLEL CIRCUITS F.5-30, P119 USING KIRCHHOFF’S LAW FIND VR1,VR3 GIVEN THE VAULES SHOWN ON THE SCHEMATIC FIND VR1: VT=VR1+VR2 VR1=VT-VR2 VR1=100V-40V VR1=60V FINDVR3: VR2=VR3+VR4 VR3=VR2-VR4 VR3=40V-30V VR3=10V USING KIRCHHOFF’S CURRENT LAW,FIND IR1,IR2,IR3 SINCE .6A FLOWS THRU NODE B, 0.6A FLOWS THRU R1(THIS LOOP IS A SERIES CIRCUIT) FIND I1, AT NODE A R1 A R3 VT 100V I1 R2 40V I2 R4 30V B IT=.6A I2=.2A IT=I1+I2 I1=IT-I2 I1=0.6A-0.2A=0.4A I1 IT I2 A

  29. VOLTAGE DIVIDERS AND REGULATORS P-121 USE VOLTAGE DIVIDER EQ. TO FIND VOLTAGE’S AT POINTS A,B,C. VRN=VTRN/RT C +50V FIND Va=VtXRa/Rt =50VX2KΩ/10KΩ =10V FIND Vb=Vtx(Ra+Rb)/Rt =50Vx(2KΩ+3KΩ)/10KΩ =25V FIND Vc=Vtx(Ra+Rb+Rc)/Rt =50Vx(2KΩ+3KΩ+5KΩ)/10KΩ =50V R1 5KΩ B +25V VT 50V R2 3KΩ ` A +10V R3 2KΩ http://www.youtube.com/watch?v=XxLKfAZrhbM YOU TUBE: Voltage divider tutorial

  30. PROBLEM: PLACE 5KΩ LOAD RESISTOR HERE; Rb=5kΩX5KΩ/10KΩ=2.5KΩ TWO RESISTORS IN PARALLEL 5KΩ B VT 50V 5KΩ 3KΩ Vb=VtxRb/Rt =50VX2.5KΩ/7.5KΩ =16.67V 5KΩ LOAD B A 2KΩ 2.5KΩ Va=VbxRa/Rb =16.67VX2KΩ/5KΩ =6.67V VOLTAGE DIVIDER IS NOT WORKING PROPERLY UNDER A LOAD. VOLTAGE VARATION OF A LOAD IS % OF VOLTAGE REGULATION. %REG.=VminL-VmaxL/VmaxL(100) WHERE VminL=V WITH MIN. LOAD Vmax =V WITH MAX.LOAD %REG@ PT. A WITH NO LOAD=10-6.67/10(100)=50% %REG@ PT. B WITH 5KΩ LOAD=25-16.67/10(100)=50%

  31. Voltage Divider The two resistor voltage divider is used often to supply a voltage different from that of an available battery or power supply. In application the output voltage depends upon the resistance of the load it drives. Where                                                        

  32. RESISTOR VOLTAGE DIVIDERS HAVE BEEN REPLACED WITH ZENER DIODES(POLARIZED DEVICE) P.121 CATHODE - IN4735 BREAKDOWN VOLTAGE=6.2V ANODE + A VOLTAGE DIVIDER CAN BE MADE WITH A RESISTOR AND A ZENER DIODE INSERIES. + 500Ω _ + 10V _ + D1 5V RLOAD 1KΩ _ A ZENER DIODE IS OPERATED WITH ITS POLARITY REVERSED, THIS IS CALLED REVERSE BAIS. WHEN A ZENER DIODE IS REVERSED BAISED, NO CURRENT FLOWS THRU IT. AS THE LOAD VOLTAGE INCREASES TO NEAR 5V, THE ZENER DIODE STARTS TO BREAK DOWN AND ALLOWS CURRENT TO FLOW THRU IT. THIS RESULT LETS THE LOAD VOLTAGE STAY NEAR ITS DESIRED VALUE, WHICH MAKES THIS A GOOD VOLTAGE REGULATOR.

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