DC circuits Physics 122 10/16/13 Lecture X 1 Skills • Solve problems on parallel and series connections in DC circuits • RC circuits 10/16/13 Lecture X 2 1 Symbols • Circuits can be rearranged: – Wires with negligible resistance can be – Stretched – Bended – Collapsed to a point 10/16/13 Lecture X 3 Electric battery • • • • For idealized battery emf – supplied voltage Real life batteries have internal resistance r Terminal voltage (supplied to the circuit) Vab=emf-Ir 10/16/13 Lecture X 4 2 Skiing ßà electric circuit a i li ft b Batt ery Sk c Cannot stop at b, must get to c – ski lift: V=V1+V2 - Net voltage drop in a circuit is always equal to the supplied voltage (e.g. battery) 10/16/13 Lecture X 5 Series connection 10/16/13 • Charge conservation: – I=I1=I2=I3 • Ohm’s law – V1=IR1; V2=IR2; V3=IR3 • Energy conservation: – qV=qV1+qV2+qV3 – V=V1+V2+V3 • IReq=IR1+IR2+IR3 • Req=R1+R2+R3 Lecture X 6 3 Parallel connection 1 1 1 1 = + + Req R1 R2 R3 • Charge conservation: I=I1+I2+I3 • Energy conservation: V=V1=V2=V3 • Ohm’s law: I1=V/R1; I2=V/R2; I3=V/R3 V V V V = + + Req R1 R2 R3 10/16/13 Lecture X 7 Capacitor connections No DC current through capacitor, Just store charge. • Parallel connection: • • Same voltage – V1=V2=V3=V • • Different charges: • – Q1=C1V Q2=C2V Q3=C3V – Q=Q1+Q2+Q3=V(C1+C2+C3) Series connection: Same charge (QA=0 à -Q1+Q2=0) Different voltages V=V1+V2+V3 Q Q Q Q = + + Ceq C1 C2 C3 – Ceq=C1+C2+C3 10/16/13 Lecture X 1 1 1 1 = + + Ceq C1 C2 C3 8 4 RC circuit • RC circuit contains at least one capacitor (C ) and at least one resistor (R ). I= dQ dt VR = IR VC = Q / C VR + VC = Vbattery = const +Q dQ Q R + =V dt C RCQ '+Q = CV C -Q Q = CV (1 − e −t /τ ) τ = RC 10/16/13 Lecture X 9 DC circuits • • • • Series connection I=I1=I2=I3 V=V1+V2+V3 Req=R1+R2+R3 10/16/13 • • • • Parallel connection I=I1+I2+I3 V=V1=V2=V3 1 1 1 1 = + + Req R1 R2 R3 Lecture X 10 5 Series vs parallel - Req • R1=R2=R3=R • Req=3R • R1=R2=R3=R • Req=R/3 > Equivalent resistance is larger in series connection. 10/16/13 Lecture X 11 Series vs parallel - I • • • • R1=R2=R3=R Req=3R I=V/(3R) I1=I2=I3=I=V/(3R) < < • • • • R1=R2=R3=R Req=R/3 I=3V/R I1=I2=I3=I/3=V/R Total current and individual currents are smaller in series connection. 10/16/13 Lecture X 12 6 Series vs parallel - P P1=I2R Pnet=IV Brightness proportional to power • • • • R1=R2=R3=R Req=3R I=V/3R à Pnet=V2/3R I1=V/3Rà P1=V2/9R < < • • • • R1=R2=R3=R Req=R/3 I=3V/R à Pnet=3V2/R I1=V/R à P1=V2/R Total and individual power consumptions are smaller in series connection. Light bulbs are brighter in parallel connection. 10/16/13 Lecture X 13 Safety and grounding • Usually V is fixed • To reduce I – increase R • Dry surface – 1mA – “feel” • Insulating sole – 10mA – muscle contraction • Insulating floor – 70 mA – “ventricular fibrillation” – ~1A – hearts stops (not as harmful)• To avoid high V • Ground the case – >10A – “fry” (3prong plug) 14 10/16/13 Lecture X • Voltage does not kill. • Current kills 7 Kirchhoff’s rules • Junction rule (charge conservation): – At any junction point the sum of all current entering the junction must equal the sum of all currents leaving the junction • Do not disregard signs! • Assign initial signs based on your best guess – if you were wrong the currents will turn to be negative (opposite to initial guess) • Loop rule (energy conservation): – The sum of the changes in potential around any closed path of a circuit must be zero. • • • • • Choose a direction in which you circle the loop (random) For resistor Vab=-IR – negative if current along the loop direction For resistor Vab=+IR – positive if current opposite the loop direction For battery Vab – positive if the direction is from – to + For battery Vab –negative if the direction is from + to - 10/16/13 Lecture X 15 Series vs parallel - Req • R1=Rà2R • Req=3Rà4R R2=R3=R • R1=Rà2R R2=R3=R • Req=R/3=2R/6à2R/5 If any of R’s increased the equivalent resistance will increase in both parallel and series connection. 10/16/13 Lecture X 16 8 Series vs parallel - I • • • • R1=Rà2R R2=R3=R Req=3Rà4R I=V/Req=V/3RàV/4R I1=I2=I3=I 10/16/13 • • • • • R1=Rà2R R2=R3=R Req=R/3=2R/6à2R/5 I=V/Req=6V/2Rà5V/2R I1=V/R1=V/RàV/2R I2=I3=V/R – the same Lecture X 17 Test problem • For resistors connected in series, which of the following will be the same for each of the resistors? • A The current through. • B The potential difference across. • C The resistance of. • D The power dissipated by. 10/16/13 Lecture X 18 9 Test problem • For resistors connected in parallel, which of the following will be the same for each of the resistors? • A The current through. • B The potential difference across. • C The resistance of. • D The power dissipated by. 10/16/13 Lecture X 19 10