Physics 272 February 12 Spring 2015 www.phys.hawaii.edu/~philipvd/pvd_15_spring_272_uhm go.hawaii.edu/KO Prof. Philip von Doetinchem philipvd@hawaii.edu PHYS272 - Spring 15 - von Doetinchem - 267 Direct-current circuits ● ● ● Study networks of circuit elements: find voltages and currents Important: charge conservation Direct current: currents are not changing: – Flashlights – Automobile wiring PHYS272 - Spring 15 - von Doetinchem - 268 Resistors in series and parallel ● ● ● Combinations of resistors play an important role in many devices Series and parallel connection: What are the currents? (similar to the question with capacitors → charges) ● Series: currents are the same ● Parallel: potential differences are the same ● Similar to capacitors: equivalent resistance PHYS272 - Spring 15 - von Doetinchem - 269 Resistors in series ● ● ● Voltages are directly proportional to resistance and current The equivalent resistance of any number of resistors in series equals the sum of their individual resistances Equivalent resistance is greater than any individual resistance PHYS272 - Spring 15 - von Doetinchem - 270 Resistors in parallel ● ● ● ● Current is proportional to common voltages, but inversely proportional to the resistance For any number of resistors in parallel, the reciprocal of the equivalent resistance equals the sum of the reciprocals of their individual resistances. The equivalent resistance is always lower than any individual resistance. More current goes through the path of least of resistance. PHYS272 - Spring 15 - von Doetinchem - 271 Resistors in series and parallel https://phet.colorado.edu/en/simulation/circuit-construction-kit-dc PHYS272 - Spring 15 - von Doetinchem - 272 Resistors in series and parallel ● Network of resistors can be replaced by an individual one ● Make a drawing ● Identify groups of series and parallel connections ● ● ● Target variables: equivalent resistance, potential differences, currents Series: potential differences add up, current is the same Parallel: potential difference is the same, currents add up PHYS272 - Spring 15 - von Doetinchem - 273 Light bulbs in series and parallel http://www.youtube.com/watch?v=apHkG4T6QHM ● ● What makes a classic light bulb glow is the dissipation of energy in the filament: If current to light bulb is reduced (for what ever reason) by a factor of 2. The dissipated energy becomes smaller by a factor of 22 PHYS272 - Spring 15 - von Doetinchem - 275 Light bulbs in series and parallel Current and power in each light bulb: Voltage is the same for both light bulbs Current and power in each light bulb: The current per light bulb is half with respect to parallel connection. Also the potential drop over each light bulb is half as it is split between both light bulbs. Less power dissipation per light bulb in series connection with the same power source. PHYS272 - Spring 15 - von Doetinchem - 276 Equivalent resistance PHYS272 - Spring 15 - von Doetinchem - 281 An infinite network PHYS272 - Spring 15 - von Doetinchem - 282 An infinite network PHYS272 - Spring 15 - von Doetinchem - 283 An infinite network PHYS272 - Spring 15 - von Doetinchem - 284 ● ● ● Rules to calculate currents in more complicated networks Definitions: – Junction: three or more conductors meet – Loop: any closed path in a circuit Kirchhoff's junction rule: Source: http://de.wikipedia.org/wiki/Gustav_Robert_Kirchhoff Kirchhoff's rules Gustav Kirchhoff (1824-1887) Algebraic sum of currents is zero at any junction. Conservation of charge PHYS272 - Spring 15 - von Doetinchem - 285 ● ● Definitions: – Junction: three or more conductors meet – Loop: any closed path in a circuit Kirchhoff's loop rule: Source: http://de.wikipedia.org/wiki/Gustav_Robert_Kirchhoff Kirchhoff's rules Gustav Kirchhoff (1824-1887) Algebraic sum of potential differences is zero in any loop. ● Electrostatic force is conservative. Path does not matter → potential energy is the same after going around a loop PHYS272 - Spring 15 - von Doetinchem - 286