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Networks I for M.E. ECE 09.201 - 2 James K. Beard, Ph.D. Rowan Hall 238A [email protected] http://rowan.jkbeard.com September 18, 2006 Admin 1 – week from tomorrow Test 1 Cruise course website Questions thus far? September 18, 2006 Class Name Slide 2 Networks I Today’s Learning Objectives – Analyze DC circuits with passive elements including: resistance -- DONE Learn about switches -- DONE Introduce KVL and KCL What is voltage and current division? Parallel and series sources Solve some more difficult problems September 18, 2006 Class Name Slide 3 chapter 2 - overview engineering and linear models - done active and passive circuit elements - done resistors – Ohm’s Law - done dependent sources – done independent sources – done transducers – done switches – in progress September 18, 2006 Class Name Slide 4 chapter 3 - overview electric circuit applications define: node, closed path, loop Kirchoff’s Current Law Kirchoff’s Voltage Law a voltage divider circuit parallel resistors and current division series V-sources / parallel I-sources resistive circuit analysis September 18, 2006 Class Name Slide 5 Gustav Robert Kirchhoff 1824-1887 two profound scientific laws published in 1847 how old was he? LC #1 September 18, 2006 Class Name Slide 6 Kirchhoff’s laws Kirchhoff’s Current Law (KCL): The algebraic sum of the currents into a node at any instant is zero. Kirchhoff’s Voltage Law (KVL): The algebraic sum of the voltages around any closed path in a circuit is zero for all time. September 18, 2006 Class Name Slide 7 KCL R1=10 Node 1 Node 2 + _ + + _ _ I=5A R3= 5 R2= 20 Node 3 Assume passive sign convention September 18, 2006 Class Name Slide 8 Node 1 I=5A R1=10 i1 + v1=50v _ Node 2 + + I i2 R2= 20 Node 1 +I - i1 = 0 Node 2 +i1 - i2 - i3 = 0 Node 3 +i2 + i3 - I = 0 i2 = v2/R2 September 18, 2006 R3= 5 _ i3 _ Node 3 Use KCL and Ohm’s Law i3 = v3/R3 Class Name Slide 9 Node 1 I=5A R1=10 Node 2 i1 + v1=50v _ + I v2 i2 R2= 20 + R3= 5 _ v3 i3 _ Node 3 Node 1 +I - i1 = 0 Node 2 +i1 - i2 - i3 = 0 Use KCL and Ohm’s Law Node 3 +i2 + i3 - I = 0 i2 = v2/R2 September 18, 2006 i3 = v3/R3 Class Name CURRENT DIVIDER Slide 10 Learning check #1 what is relationship between v2 and v3 in previous example? <, >, = September 18, 2006 Class Name Slide 11 KVL R1=10 _ + + V= 5v + _ LOOP 1 R2= 20 _ Start +V - vR1 - vR2 = 0 i = V/(R1 + R2) iV = iR1 = iR2 = i vR1 = iR1 = VR1 /(R1 + R2) +V = iR1 + iR2 V = i(R1 + R2) September 18, 2006 vR2 = iR2 = VR2/(R1 + R2) Class Name Slide 12 SERIES RESISTORS R1=10 _ + + V= 5v + _ LOOP 1 R2= 20 _ Start NOTE +V - vR1 - vR2 = 0 i = V/(R1 + R2) iV = iR1 = iR2 = i vR1 = iR1 = VR1 /(R1 + R2) +V = iR1 + iR2 vR2 = iR2 = VR2/(R1 + R2) V = i(R1 + R2) September 18, 2006 Class Name VOLTAGE DIVIDER Slide 13 SERIES RESISTORS resistors attached in a “string” can be added together to get an equivalent resistance. R = 2 R = 3 R = 9 R = 4 September 18, 2006 Class Name Slide 14 Learning check #2 what is value of Req in previous example when the three resistors are replaced with the following 4 new resistors? 1 k, 100, 10, and 1 September 18, 2006 Class Name Slide 15 PARALLEL RESISTORS resistors attached in parallel can be simplified by adding their conductances (G) together to get an equivalent resistance (R=1/G). Geq = Gr1 + Gr2 + etc.. R = 1 R = 9 When you only have two: Req = (R1*R2)/(R1+R2) September 18, 2006 Class Name Slide 16 Learning checks #3 & #4 4. what is value of Req in previous example? 5. what is the new value of Req when the two parallel resistors are replaced 2 new resistors shown below? 10 and 40 September 18, 2006 Class Name Slide 17 series voltage sources when connected in series, a group of voltage sources can be treated as one voltage source whose equivalent voltage = all source voltages unequal voltage sources are not to be connected in parallel September 18, 2006 Class Name Slide 18 Learning check #5 6a. What is effective value of V for the series voltage sources in the example on board? 6b. What is the power dissipated in the resistor of 30? September 18, 2006 Class Name Slide 19 Networks I Today’s Learning Objectives – Use KVL and KCL What is voltage and current division? Parallel and series sources September 18, 2006 Class Name Slide 20 chapter 3 - overview electric circuit applications - done define: node, closed path, loop - done Kirchoff’s Current Law - done Kirchoff’s Voltage Law- done a voltage divider circuit – in progress parallel resistors and current division series V-sources / parallel I-sources resistive circuit analysis September 18, 2006 Class Name Slide 21 Kirchhoff’s laws Kirchhoff’s Current Law (KCL): The algebraic sum of the currents into a node at any instant is zero. Kirchhoff’s Voltage Law (KVL): The algebraic sum of the voltages around any closed path in a circuit is zero for all time. September 18, 2006 Class Name Slide 22 KVL R1=10 Use KVL and Ohm’s Law VOLTAGE DIVIDER + V= 5v + _ LOOP 1 R2= 20 _ Start +V - vR1 - vR2 = 0 i = V/(R1 + R2) iV = iR1 = iR2 = i vR1 = iR1 = VR1 /(R1 + R2) +V = iR1 + iR2 V = i(R1 + R2) September 18, 2006 _ + vR2 = iR2 = VR2/(R1 + R2) Class Name Slide 23 SERIES RESISTORS R1=10 _ + + V= 5v + _ LOOP 1 R2= 20 _ Start NOTE +V - vR1 - vR2 = 0 i = V/(R1 + R2) iV = iR1 = iR2 = i vR1 = iR1 = VR1 /(R1 + R2) +V = iR1 + iR2 vR2 = iR2 = VR2/(R1 + R2) V = i(R1 + R2) September 18, 2006 Class Name VOLTAGE DIVIDER Slide 24 KCL Node 1 I=5A R1=10 Node 2 i1 + v1=50v _ + I v2 i2 R2= 20 + R3= 5 _ v3 i3 _ Node 3 Node 1 +I - i1 = 0 Node 2 +i1 - i2 - i3 = 0 Use KCL and Ohm’s Law Node 3 +i2 + i3 - I = 0 i2 = v2/R2 September 18, 2006 i3 = v3/R3 Class Name CURRENT DIVIDER Slide 25 PARALLEL RESISTORS resistors attached in parallel can be simplified by adding their conductances (G) together to get an equivalent resistance (R=1/G). Geq = Gr1 + Gr2 + etc.. R = 1 R = 9 When you only have two: Req = (R1*R2)/(R1+R2) September 18, 2006 Class Name Slide 26 Equivalent parallel resistors Example 3 parallel resistors: 6, 9, 18 what is the equivalent resistance? Geq = Gr1 + Gr2 + etc.. 1/6 + 1/9 + 1/18 = 6/18 = 1/3 If Geq = 1/3 then R = ? September 18, 2006 Class Name Slide 27 Learning check #1 What is effective resistance value of three parallel resistors with values of 4, 5, 20? Hint: calculate Geq , then R September 18, 2006 Class Name Slide 28 parallel current sources when connected in parallel, a group of current sources can be treated as one current source whose equivalent current = all source currents unequal current sources are not to be connected in series September 18, 2006 Class Name Slide 29 Learning check #2 2a. What is effective value of i for the example of parallel current sources on the board (5, 10, 7, 4)? 2b. What is the power dissipated in the resistor of 6? September 18, 2006 Class Name Slide 30 PROBLEM SOLVING METHOD + node1 va Ra ia ivs vs _ node2 + + _ loop1 + ic R c vb node3 Rb ib + vc _ _ loop2 is vis _ node4 September 18, 2006 Class Name Slide 31 steps taken Apply P.S.C. to passive elements. Show current direction at voltages sources. Show voltage direction at current sources. Name nodes and loops. Name elements and sources. Name currents and voltages. September 18, 2006 Class Name Slide 32 WRITE THE KCL EQUATIONS v _ + node1 a Ra vs node2 + ia ivs + _ loop1 vb + vc _ node3 Rb ib + ic R c _ loop2 is vis _ node4 node1: ivs ia 0 node3: ib i s 0 node2: ia ib ic 0 node4: ic i s ivs 0 September 18, 2006 Class Name Slide 33 WRITE THE KVL EQUATIONS + node1 va Ra ia ivs vs _ node2 + + _ loop1 + ic R c vb node3 Rb ib + vc loop2 _ _ is vis _ node4 loop1: loop2: vc vb vis 0 v s va vc 0 September 18, 2006 Class Name Slide 34 WRITE SUPPLEMENTARY EQUATIONS + node1 va Ra ia ivs vs _ node2 + + _ loop1 vb + vc _ node3 Rb ib + ic R c _ loop2 is vis _ node4 ia va / Ra September 18, 2006 ib vb / Rb Class Name ic vc / Rc Slide 35