Topics: • Conductivity and Resistivity • Resistance and Ohm’s Law • • • Capacitors in series and parallel Resistors in series and parallel Kirchhoff’s Rules PHYS 1022: Chap. 31-32, Pg 2 1 PHYS 1022: Chap. 31-32, Pg 3 PHYS 1022: Chap. 31-32, Pg 4 2 New Topic PHYS 1022: Chap. 31-32, Pg 5 The electric field is directly proportional to the current density in the wire. ρ is called resistivity, R is the resistance a measure of how hard a charge can move in a material SI unit: V.m / A = Ω. m V = RI € A perfect conductor has zero resistivity. A perfect insulator has infinite resistivity The reciprocal of resistivity (1/ρ) is called conductivity σ. PHYS 1022: Chap. 31-32, Pg 6 3 The resistivity of a material depends on temperature. Metal near room temperature: PHYS 1022: Chap. 31-32, Pg 7 PHYS 1022: Chap. 31-32, Pg 8 4 PHYS 1022: Chap. 31-32, Pg 9 PHYS 1022: Chap. 31-32, Pg 10 5 PHYS 1022: Chap. 31-32, Pg 11 PHYS 1022: Chap. 31-32, Pg 12 6 Topics: • Conductivity and Resistivity • Resistance and Ohm’s Law • • • Capacitors in series and parallel Resistors in series and parallel Kirchhoff’s Rules PHYS 1022: Chap. 31-32, Pg 13 New Topic PHYS 1022: Chap. 31-32, Pg 14 7 Since Q = C V, we have C1V+ C2V + C3V = CV C is called an equivalent capacitor. PHYS 1022: Chap. 31-32, Pg 15 Since V = Q/C, we have Q/C1+ Q/C2 + Q/C3 = Q/C 1 1 1 1 = + + C C1 C2 C 3 PHYS 1022: Chap. 31-32, Pg 16 8 1) What is the equivalent capacitance of the combination shown ? 2) 3) 4) 5) 3C/2 2C/3 3C 2C C/2 o Ceq C C C o PHYS 1022: Chap. 31-32, Pg 17 How does the voltage V1 across the C1 compare to the voltage V2 across C2? 1) 2) 3) 4) V1 = V2 V1 > V2 V1 < V2 all voltages are zero PHYS 1022: Chap. 31-32, Pg 18 9 How does the charge Q1 across C1 compare to the charge Q2 across C2? 1) 2) 3) 4) Q1 = Q2 Q1 < Q2 Q1 > Q2 all charges are zero PHYS 1022: Chap. 31-32, Pg 19 PHYS 1022: Chap. 31-32, Pg 20 10 Find the charge, potential difference, and energy stored in each capacitor. PHYS 1022: Chap. 31-32, Pg 21 New Topic PHYS 1022: Chap. 31-32, Pg 22 11 PHYS 1022: Chap. 31-32, Pg 23 Req is the reciprocal of the sum of the reciprocals. PHYS 1022: Chap. 31-32, Pg 24 12 New Topic PHYS 1022: Chap. 31-32, Pg 25 (or: what goes in has to come out!) PHYS 1022: Chap. 31-32, Pg 26 13 “The sum of voltage drops and gains around any closed circuit loop must be zero” ΔV1 + ΔV2 + ΔV3 + ΔV4 + … = 0 Sign convention: – sign for voltage drop and + sign voltage gain. It depends on several factors: 1. emf or resistor 2. direction of current 3. direction of loop travel What is the current at point P? PHYS 1022: Chap. 31-32, Pg 27 5A P 8A 2A 1) 2) 3) 4) 2A 5A 6A 10 A PHYS 1022: Chap. 31-32, Pg 28 14 PHYS 1022: Chap. 31-32, Pg 29 PHYS 1022: Chap. 31-32, Pg 30 15 PHYS 1022: Chap. 31-32, Pg 31 PHYS 1022: Chap. 31-32, Pg 32 16 PHYS 1022: Chap. 31-32, Pg 33 PHYS 1022: Chap. 31-32, Pg 34 17 Current in each resistor? –IR = –8 V I Total resistance = 6 Ω –IR = – 4 V Ohm’s Law: I = V / R = 12 V / 6 Ω =2A 2Ω 4Ω 12 V Start Voltage drop across resistor? V=IR +ε = 12 V ΔV = + 12 V – 8 V – 4 V = 0 PHYS 1022: Chap. 31-32, Pg 35 The first thing we have to do is? Define currents! –I2R1 I2 I3 –I2R2 R1 –ε I1 +ε R3 Next: Define travel direction: top loop (CW) bottom loop (CW) R2 Now apply Loop rule to each loop Start ΔV = + ε – I2R1 – I2R2 = 0 Start ΔV = + I3 R3 – ε = 0 + I3R3 PHYS 1022: Chap. 31-32, Pg 36 18 PHYS 1022: Chap. 31-32, Pg 37 PHYS 1022: Chap. 31-32, Pg 38 19 PHYS 1022: Chap. 31-32, Pg 39 PHYS 1022: Chap. 31-32, Pg 40 20