Electric current Physics 122 11/21/2018 Lecture VII.

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Presentation transcript:

Electric current Physics 122 11/21/2018 Lecture VII

Concepts Primary concepts: Electric current Resistor and resistivity Electric circuit 11/21/2018 Lecture VII

Laws Ohm’s law Power in electric circuits 11/21/2018 Lecture VII

Electric current - + A flow of charge is called an electric current Note: net charge =0 + - It is measured in ampere (A=C/s) Need free charge to have electric current. Use conductors. 11/21/2018 Lecture VII

Skiing  electric circuit High PE High PE Low PE Low PE Skiers Charges go from points with high PE to low PE To complete the circuit need a device that brings you back to high PE: Ski lift Battery 11/21/2018 Lecture VII

Electric circuit Need free charge  electric circuit must consist of conductive material (wires). Electric circuit must be closed. Battery supplies constant potential difference – voltage. e - Battery converts chemical energy into electric energy. Symbol for battery 11/21/2018 Lecture VII

Electric circuit a). Will not work, Circuit is not closed b). Will not work, Circuit is at the same potential (+), no potential difference - voltage. c). Will work. 11/21/2018 Lecture VII

Ohm’s law Electric current is proportional to voltage. Coefficient in this dependence is called resistance R Resistance is measured in Ohm (W = V/A) I R V 11/21/2018 Lecture VII

Resistors First digit Second digit Multiplier Tolerance 2.5 x103 W +- 5%. 11/21/2018 Lecture VII

Resistivity traffic  Electric current Long narrow street  high resistance Condition of the road  material property called resistivity r. r is measured in W m L – length of the conductor A – its area. 11/21/2018 Lecture VII

Resistance and Temperature When electrons move through the conductor they collide with atoms: Resistivity grows with temperature ( more collisions) r0 – resistivity measured at some reference temperature T0 a – temperature coefficient of resistivity 11/21/2018 Lecture VII

Resistance and Temperature When electrons move through the conductor they collide with atoms: Temperature of the conductor increases because of the current (through collisions) Electrical energy is transformed into thermal energy Resistors dissipate energy Power – energy per unit of time- (in W=J/s) dissipated by a resistor 11/21/2018 Lecture VII

Electric power Electric energy can be converted into other kinds of energy: Thermal ( toaster) Light (bulbs) Mechanical (washer) Chemical Electric power (energy per unit of time): 11/21/2018 Lecture VII

Test problem You have an open working refrigerator in your room. It makes your room A hotter B colder 11/21/2018 Lecture VII

Test problem P=IV P=I2R P=V2/R A light bulb is connected to a battery. It is then cooled and its resistance decreased. Brightness is proportional to consumed power. The light bulb burns A Brighter B dimmer P=IV P=I2R P=V2/R 11/21/2018 Lecture VII

Alternating current (AC) Voltage changes sign  current changes the direction I Req ~ 11/21/2018 Lecture VII

Electric circuits: resistors Current in=current out I1=I2 No electrons are lost inside Resistors dissipate power (energy/time) P=I2R Drop of voltage over a resistor DV=-IR: V2=V1-IR I1,V1 R I2,V2 11/21/2018 Lecture VII

Electric circuits: wires We assume that wire have very small resistance (R=0) Current in=current out I1=I2 Power dissipated in wires P=I2R=0 Drop of voltage over a resistor DV=-IR=0 V2=V1 From the point of electric circuit wires can be stretched, Bended Straightened Collapsed to a point without changing the electrical properties of the circuit I1,V1 I2,V2 I1,V1 I2,V2 I1,V1 I2,V2 11/21/2018 Lecture VII

Electric circuit: battery Energy conservation Drop of voltage in electric circuit is always equal to voltage supplied by an external source (e.g. battery). Current (the effective flow of positive charge) goes from + to – Electrons (negative charge!) go from – to + I R1 R2 R3 V 11/21/2018 Lecture VII

Electric circuits: branches Charge is conserved Current – what goes in, goes out I1 I I2 I I3 V 11/21/2018 Lecture VII