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Electric Circuits Count Alessandro Volta (1745 - 1827) Georg Simon Ohm (1787 - 1854) André Marie AMPÈRE (1775 - 1836) Charles Augustin de Coulomb (1736 – 1806) Simple Electric Cell Carbon Electrode (+) wire _ _ _ + + + Zn Electrode (-) Zn+ Zn+ Zn+ Zn+ Sulfuric acid •Two dissimilar metals or carbon rods in acid •Zn+ ions enter acid leaving terminal negative •Electrons leave carbon leaving it positive •Terminals connected to external circuit •‘Battery’ referred to several cells originally Electric Current Electrons flow out of the negative terminal and toward the positive terminal electric current. (We will consider conventional current – positive charges move Electric current I is defined as the rate at which charge flows past a given point per unit time. 1 C/s = 1A (ampere) Electric Circuit • It is necessary to have a complete circuit in order for current to flow. • The symbol for a battery in a circuit diagram is: + _ “Conventional” current direction is opposite to actual electron flow direction which is – to +. Current Device 9 volts + Ohm’s Law • For wires and other circuit devices, the current is proportional to the voltage applied to its ends: IV • The current also depends on the amount of resistance that the wire offers to the electrons for a given voltage V. We define a quantity called resistance R such that V = I R (Ohm’s Law) • The unit of resistance is the ohm which is represented by the Greek capital omega (). V 1 A Resistors • A resistor is a circuit device that has a fixed resistance. Resistor Code Calculator Resistor Code Resistor Circuit symbol Resistors obey Ohm’s law but not all circuit devices do. I I 0 Resistor V 0 V non-ohmic device Resistivity Resistivity table • Property of bulk matter related to resistance of a sample is the resistivity (r) defined as: The resistivity varies greatly with the sort of material: e.g., for copper r ~ 10-8 -m; for glass, r ~ 10+12 -m; for semiconductors r ~ 1 -m; for superconductors, r = 0 [see Appendix] Ohm’s Law • Demo: • Vary applied voltage V. I R I • Measure current I V V • Does ratio remain I constant? R V V I slope = R How to calculate the resistance? Include “resistivity” of material I Include geometry of resistor Resistance R • Resistance I I Resistance is defined to be the ratio of the applied voltage to the current passing through. R V I UNIT: OHM = V • How do we calculate it? Recall the case of capacitance: (C=Q/V) depended on the geometry (and dielectric constant), not on Q or V individually Similarly, for resistance –part depends on the geometry (length L and cross-sectional area A) –part depends on the “resistivity” ρ of the material L R r A • Increase the length flow of electrons impeded • Increase the cross sectional area flow facilitated • What about r? Two cylindrical resistors are made from the same material, and they are equal in length. The first resistor has diameter d, and the second resistor has diameter 2d. 1) Compare the resistance of the two cylinders. a) R1 > R2 b) R1 = R2 c) R1 < R2 2) If the same current flows through both resistors, compare the average velocities of the electrons in the two resistors: a) v1 > v2 b) v1 = v2 c) v1 < v2 Strain Gauge • A very thin metal wire patterned as shown is bonded to some structure. • As the structure is deformed slightly, this stretches the wire (slightly). – When this happens, the resistance of the wire: (a) decreases (b) increases (c) stays the same Because the wire is slightly longer, R ~ L A is slightly increased. Also, because the overall volume of the wire is ~constant, increasing the length decreases the area A, which also increases the resistance. By carefully measuring the change in resistance, the strain in the structure may be determined. Power in Electric Circuits • Electrical circuits can transmit and consume energy. • When a charge Q moves through a potential difference V, the energy transferred is QV. • Power is energy/time and thus: Q P power V IV time t t energy and thus: P IV QV Notes on Power •The formula for power applies to devices that provide power such as a battery as well as to devices that consume or dissipate power such as resistors, light bulbs and electric motors. C J J A V Watt (W ) s C s •The formula for power can be combined with Ohm’s Law to give other versions: 2 V P IV I R R 2 Household Power •Electric companies usually bill by the kilowatthour (kWh.) which is the energy consumed by using 1.0 kW for one hour. •Thus a 100 W light bulb could burn for 10 hours and consume 1.0 kWh. •Electric circuits in a building are protected by a fuse or circuit breaker which shuts down the electricity in the circuit if the current exceeds a certain value. This prevents the wires from heating up when carrying too much current. The Voltage “drops”: Va Vb IR1 Resistors in Series I R1 Vb Vc IR2 b Va Vc I ( R1 R2 ) Whenever devices are in SERIES, the current is the same through both ! R2 a This reduces the circuit to: Hence: a Reffective ( R1 R2 ) c Reffective c e1 R I1 I2 e2 R I3 e3 R V n loop 0 I in I out Voltage Divider R1 V0 V R2 By varying R2 we can controllably adjust the output voltage! V ? V0 V IR2 R2 R1 R2 R2 R1 V=0 R2 R1 V0 V= 2 R2 R1 V=V0 Voltage Divider Two resistors are connected in series to a battery with emf E. The resistances are such that R1 = 2R2. Compare the current through R1 with the current through R2: a) I1 > I2 b) I1 = I2 c) I1 < I2 What is the potential difference across R2? a) V2 = E b) V2 = 1/2 E c) V2 = 1/3 E Resistors in Parallel • What to do? V IR • Very generally, devices in parallel have the same voltage drop • But current through R1 is not I ! Call it I1. Similarly, R2 I2. KVL V I1R1 0 I a I1 V I2 R1 I d V I 2 R2 0 • How is I related to I 1 & I 2 ? R2 I a Current is conserved! V I I1 I 2 V V V R R1 R2 1 1 1 R R1 R2 R d I Another way… Resistivity Consider two cylindrical resistors with cross-sectional areas A1 and A2 L R1 r A1 A1 V A2 R1 L R2 r A2 R2 Put them together, side by side … to make one “fatter”one, Reffective rL A1 A2 1 Reffective 1 1 1 R R1 R2 A1 A 1 1 2 rL rL R1 R2 Circuit Practice • Consider the circuit shown: 1 50 a – What is the relation between Va -Vd and Va -Vc ? b 12V (a) (Va -Vd) < (Va -Vc) (b) (Va -Vd) = (Va -Vc) (c) (Va -Vd) > (Va -Vc) 1B 2 (b) I1 = I2 20 80 d – What is the relation between I1 and I2? (a) I1 < I2 I2 I1 (c) I1 > I2 c Circuit Practice • Consider the circuit shown: 1 50 a – What is the relation between Va -Vd and Va -Vc ? (a) (Va -Vd) < (Va -Vc) (b) (Va -Vd) = (Va -Vc) (c) (Va -Vd) > (Va -Vc) b I2 I1 12V 20 80 d c • Do you remember that thing about potential being independent of path? Well, that’s what’s going on here !!! (Va -Vd) = (Va -Vc) Point d and c are the same, electrically Circuit Practice • Consider the circuit shown: 50 a – What is the relation between Va -Vd and Va -Vc ? b 12V (a) (Va -Vd) < (Va -Vc) (b) (Va -Vd) = (Va -Vc) (c) (Va -Vd) > (Va -Vc) 2 20 • Note that: Vb -Vd • Therefore, (b) I1 = I2 (c) I1 > I2 = Vb -Vc I1 (20) I 2 (80) 80 d – What is the relation between I1 and I2? (a) I1 < I2 I2 I1 I1 4I 2 c Summary of Simple Circuits • Resistors in series: Requivalent R1 R2 R3 ... Current thru is same; • Resistors in parallel: 1 R equivalent Voltage drop across is IRi Voltage drop across is same; 1 1 1 ... R1 R2 R3 Current thru is V/Ri Two identical light bulbs are represented by the resistors R2 & R3 (R2 = R3 ). The switch S is initially open. If switch S is closed, what happens to the brightness of the bulb R2? a) It increases b) It decreases c) It doesn’t change What happens to the current I, after the switch is closed ? a) Iafter = 1/2 Ibefore b) Iafter = Ibefore c) Iafter = 2 Ibefore