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Resistance Is Futile! Physics 2113 Jonathan Dowling Physics 2113 Lecture 21: FRI 06 MAR Resistance Is Futile! Physics 2113 Jonathan Dowling Physics 2113 Lecture 21: FRI 06 MAR Current & Resistance III Georg Simon Ohm (1789 -1854)

Resistance is NOT Futile! Electrons are not “completely free to move” in a conductor. Resistance is NOT Futile! Electrons are not “completely free to move” in a conductor. They move erratically, colliding with the nuclei all the time: this is what we call “resistance”. The resistance is related to the potential we need to apply to a device to drive a given current through it. The larger the resistance, the larger the potential we need to drive the same current. Ohm’s laws Georg Simon Ohm (1789 -1854) "a professor who preaches such heresies is unworthy to teach science. ” Prussian minister of education 1830 Devices specifically designed to have a constant value of R are called resistors, and symbolized by

Resistivity and Resistance Metal “field lines” These two devices could have the same resistance Resistivity and Resistance Metal “field lines” These two devices could have the same resistance R, when measured on the outgoing metal leads. However, it is obvious that inside of them different things go on. resistivity: Resistivity is associated ( resistance: R=V/I ) with a material, resistance with respect to a device constructed with the material. Example: A - L V + Makes sense! For a given material:

b a Power in electrical circuits A battery “pumps” charges through the resistor (or b a Power in electrical circuits A battery “pumps” charges through the resistor (or any device), by producing a potential difference V between points a and b. How much work does the battery do to move a small amount of charge dq from b to a? Ohm’s laws d. W = –d. U = -dq×V = (dq/dt)×dt×V= i. V×dt The battery “power” is the work it does per unit time: P = d. W/dt = i. V P=i. V is true for the battery pumping charges through any device. If the device follows Ohm’s law (i. e. , it is a resistor), then V=i. R or i=V/R and P = i. V = i 2 R = V 2/R

Ohm’s Law and Power in Resistors Watt You Looking At!? Ohm’s Law Power Dissipated Ohm’s Law and Power in Resistors Watt You Looking At!? Ohm’s Law Power Dissipated by a Resistor:

Example, Rate of Energy Dissipation in a Wire Carrying Current: ICPP: Why is this Example, Rate of Energy Dissipation in a Wire Carrying Current: ICPP: Why is this unwise? ? ? Current i increases by 4. House Circuit Breaker 3 A.

ICPP: The figure here shows three cylindrical copper conductors along with their face areas ICPP: The figure here shows three cylindrical copper conductors along with their face areas and lengths. Rank them according to the power dissipated by them, greatest first, when the same potential difference V is placed across their lengths. Step I: The resistivity ρ is the same (all three are copper). Find the Resistance R=ρL/A for each case: Step II: Rank the power using P=V 2/R since V is same. Ranking is reversed since R is downstairs.

Example A P=1250 Watt radiant heater is constructed to operate at V=115 Volts. (a) Example A P=1250 Watt radiant heater is constructed to operate at V=115 Volts. (a) What will be the current in the heater? (b) What is the resistance of the heating coil? (c) How much thermal energy is produced in 1. 0 hr by the heater? • Formulas: P=i 2 R=V 2/R; V=i. R • Know P, V; need R to calculate current! • P=1250 W; V=115 V => R=V 2/P=(115 V)2/1250 W=10. 6 Ω • i=V/R= 115 V/10. 6 Ω=10. 8 A • Energy? P=d. U/dt => ΔU=P×Δt = 1250 W × 3600 sec= 4. 5 MJ = 1. 250 k. W • hr

Example A 100 W lightbulb is plugged into a standard 120 V outlet. (a) Example A 100 W lightbulb is plugged into a standard 120 V outlet. (a) What is the resistance of the bulb? (b) What is the current in the bulb? (c) How much does it cost per month to leave the light turned on continuously? Assume electric energy costs 6¢/k. W·h. (d) Is the resistance different when the bulb is turned off? • Resistance: same as before, R=V 2/P=144Ω • Current, same as before, i=V/R=0. 83 A • We pay for energy used (k. W h): U=Pt=0. 1 k. W × (30× 24) h = 72 k. W h => $4. 32 • (d): Resistance should be the same, but it’s not: resistivity and resistance increase with temperature. When the bulb is turned off, it is colder than when it is turned on, so the resistance is lower.

i V P = i. V U = Pt t in seconds V i i V P = i. V U = Pt t in seconds V i P = i. V [J/s is Watt] P = i. V [Watt is J/s]

I’m switching to white light LEDs! Nobel Prize 2014! My House Has Two Front I’m switching to white light LEDs! Nobel Prize 2014! My House Has Two Front Porch Lights. Each Light Has a 100 W Incandescent Bulb. The Lights Come on at Dusk and Go Off at Dawn. How Much Do these lights Cost Me Per Year? Two 100 W Bulbs @ 12 Hours Each = One 100 W @ 24 Hours. P = 100 W = 0. 1 k. W T = 365 Days x 24 Hours/Day = 8670 Hours Demco Rate: D = 0. 1797$/(k. W×Hour) (From My Bill!) Cost = Px. Tx. D = (0. 1 k. W)x(8670 Hours)x(0. 1797$/k. W×Hour) = $157. 42

 • Figure shows a person and a cow, each a radial distance D=60 • Figure shows a person and a cow, each a radial distance D=60 m from the point where lightning of current i=10 k. A strikes the ground. The current spreads through the ground uniformly over a hemisphere centered on the strike point. The person's feet are separated by radial distance Δrper=0. 50 m; the cow's front and rear hooves are separated by radial distance Δrcow=1. 50 m. The resistivity of the ground is ρgr=100 Ωm. The resistance both across the person, between left and right feet, and across the cow, between front and rear hooves, is R=4. 00 kΩ. (a) What is the current ip through the person? (b) What is the current ic through the cow? Recall that a current ≥ 100 m. A causes a heart attack and death. • Who Lives? Moo Dies!