CURRENT, RESISTANCE, AND ELECTROMOTIVE FORCE Chapter 4.

Slides:



Advertisements
Similar presentations
Circuits Electromotive Force Work, Energy and emf
Advertisements

Introduction to Current In AP C Current I = dq/dt I: current in Amperes (A) q: charge in Coulombs (C) t: time in seconds (s)
Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 18: Electric Current and Circuits.
1 Chapter Fifteen Electric Current. 2 Electric Current We consider the motion of electrons in a conductor (a metal) when there is a voltage difference.
Electric Currents and Resistance
Chapter 17 Current and Resistance. Electric Current Let us look at the charges flowing perpendicularly to a surface of area A The electric current is.
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Fundamentals of Circuits: Direct Current (DC)
DC circuits Physics Department, New York City College of Technology.
Current, Resistance, and Electromotive Force
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Electric Current and Direct-Current Circuits
AP Physics C: E&M. DC: Direct current. A constantly applied voltage causes charged particles to drift in one direction.
Chapter 26 DC Circuits Chapter 26 Opener. These MP3 players contain circuits that are dc, at least in part. (The audio signal is ac.) The circuit diagram.
Electric current and direct-current circuits A flow of electric charge is called an electric current.
Chapter 20: Circuits Current and EMF Ohm’s Law and Resistance
Chapter 27 Lecture 12: Circuits.
Chapter 20 Electric Circuits.
Fundamental Physics 2 Chapter 2 PETROVIETNAM UNIVERSITY FACULTY OF FUNDAMENTAL SCIENCES Vungtau 2012 Pham Hong Quang
Rumus yang dipakai.
My Chapter 18 Lecture Outline.
Chapter 22 Current Electricity.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Introduction to Current In AP C Current I = dq/dt I: current in Amperes (A) q: charge in Coulombs (C) t: time in seconds (s)
Lecture Outline Chapter 21 Physics, 4th Edition James S. Walker
Lecture 6 Direct Current Circuits Chapter 18 Outline Energy Source in Circuits Resistor Combinations Kirchhoff’s Rules RC Circuits.
Current Electricity Electric Current Circuit – continuous conducting path between terminals of a battery (or other source of EMF) Electric Current.
In conclusion, there are two requirements which must be met in order to establish an electric circuit. The requirements are: 1.There must.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Lecture 13 Direct Current Circuits
Unit 8: Part 2 Electric Circuits
Current, Resistance and Power
P212c26: 1 Charge carrier motion in a conductor in two parts Constant Acceleration Randomizing Collisions (momentum, energy) =>Resulting Motion Average.
Chapter 17 Current and Resistance. Electric Current Let us look at the charges flowing perpendicularly to a surface of area A The electric current is.
Current Electric Current (I)
the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal.
Phys 2180 Lecture (5) Current and resistance and Direct current circuits.
Current Electricity Electric Current Circuit – continuous conducting path between terminals of a battery (or other source of EMF) Electric Current.
Chapter 28 Direct Current Circuits. Introduction In this chapter we will look at simple circuits powered by devices that create a constant potential difference.
Lecture 11-1 Electric Current Current = charges in motion Magnitude rate at which net positive charges move across a cross sectional surface Units: [I]
Current of Electricity Electric Current Potential Difference Resistance and Resistivity Electromotive Force.
Chapter 20 Electric Current and Resistance. Units of Chapter 20 Batteries and Direct Current Current and Drift Velocity Resistance and Ohm’s Law Electric.
Electric Current and Resistance
Introduction to Current In AP C Current I = dq/dt I: current in Amperes (A) q: charge in Coulombs (C) t: time in seconds (s)
Current, Resistance, and Electromotive Force
Electricity did not become an integral Part of our daily lives until Scientists learned to control the Movement of electric charge. This is known as.
1 18 Overview resistor & capacitor circuits Kirchoff’s Rules voltmeters & ammeters household circuits & safety Homework: 17, 27, 31, 33, 55, 67, 71, 85.
Chapter 20 Electric Circuits Electromotive Force and Current Within a battery, a chemical reaction occurs that transfers electrons from one terminal.
Unit 8 : Part 1 Electric Current and Resistance. Outline Batteries and Direct Current Current and Drift Velocity Resistance and Ohm’s Law Electric Power.
Chapter 27 Lecture 23: Circuits: I. Direct Current When the current in a circuit has a constant direction, the current is called direct current Most of.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Lectures 7 to 10 The Electric Current and the resistance Electric current and Ohm’s law The Electromotive Force and Internal Resistance Electrical energy.
1 §18.1 Electric Current e-e- e-e- e-e- e-e- e-e- e-e- e-e- e-e- A metal wire. Assume electrons flow to the right. Current is a measure of the amount of.
Electricity and Circuit. Types of Electricity Static Electricity – no motion of free charges Current Electricity – motion of free charges – Direct Current.
1© Manhattan Press (H.K.) Ltd Potentiometer Comparing resistances Measuring the e.m.f. of a cell Measuring the internal resistance of a cell.
PHY 102: Lecture Voltage 5.2 Current 5.3 Resistance 5.4 Ohm’s Law 5.5 Electric Power 5.6 Series Circuits 5.7 Parallel Circuits 5.8 Combined Series/Parallel.
Chapter 18 Electric Currents © 2014 Pearson Education, Inc.
Chapter 6 & 7: Electricity. Electricity The flow of electric current. The flow of electric energy carried by electrons.
Electricity. The flow of electric current. The flow of electric energy carried by electrons.
Chapter 19 DC Circuits. EMF and Terminal Voltage Any device that can transform a type of energy into electric energy is called a source of electromotive.
Chapter 20 Electric Circuits Electromotive Force and Current In an electric circuit, an energy source and an energy consuming device are connected.
Current = charges in motion
DC circuit theory.
Chapter 25: Current, Resistance and Electromotive Force
Current, Resistance, and Electromotive Force
Direct-Current Circuits
PHYS 1902 Electromagnetism: 2 Lecturer: Prof. Geraint F. Lewis
Circuit in DC Instruments
Current and Simple Circuits Voltage Resistance Safety
Presentation transcript:

CURRENT, RESISTANCE, AND ELECTROMOTIVE FORCE Chapter 4

CURRENT AND CURRENT DENSITY Current is the amount of charge flowing through a specified area, per unit time. The SI unit of current is the ampere, equal to one coulomb per second (1 A = 1 C/s).

CURRENT AND CURRENT DENSITY

EXAMPLE An 18-gauge copper wire (the size usually used for lamp cords) has a nominal diameter of 1.02 mm. This wire carries a constant current of 1.67 A to a 200-watt lamp. The density of free electrons is 8.5 x electrons per cubic meter. Find the magnitudes of (a) the current density and (b) the drift velocity.

EXAMPLE

RESISTIVITY The resistivity ρ of a material is the ratio of the magnitudes of electric field and current density. Good conductors have small resistivity; good insulators have large resistivity.

RESISTIVITY

RESISTORS For materials obeying Ohm’s law, the potential difference V across a particular sample of material is proportional to the current I through the material. The ratio V/I = R is the resistance of the sample.

RESISTORS

EXAMPLE The 18-gauge copper wire in the previous example has a diameter of 1.02 mm and a cross-sectional area of 8.20 x m 2. It carries a current of 1.67 A. Find (a) the electric-field magnitude in the wire; (b) the potential difference between two points in the wire 50.0 m apart; (c) the resistance of a 50.0-m length of this wire.

EXAMPLE

CIRCUITS AND EMF A complete circuit has a continuous current-carrying path. A complete circuit carrying a steady current must contain a source of electromotive force (emf) ε.

CIRCUITS AND EMF The SI unit of electromotive force is the volt (1 V). An ideal source of emf maintains a constant potential difference, independent of current through the device, but every real source of emf has some internal resistance r.

CIRCUITS AND EMF

EXAMPLE The figure shows a source (a battery) with an emf ε of 12 V and an internal resistance r of 2 Ω. (For comparison, the internal resistance of a commercial 12-V lead storage battery is only a few thousandths of an ohm). The wires to the left of a and to the right of the ammeter A are not connected to anything. Determine the readings of the idealized voltmeter V and the idealized ammeter A.

EXAMPLE

ENERGY AND POWER IN CIRCUITS

EXAMPLE For the given figure, find the rate of energy conversion (chemical to electrical) and the rate of dissipation of energy in the battery and the net power output of the battery.

EXAMPLE

CONDUCTION IN METALS The microscopic basis of conduction in metals is the motion of electrons that move freely through the metallic crystal, bumping into ion cores in the crystal. In a crude classical model of this motion, the resistivity of the material can be related to the electron mass, charge, speed of random motion, density, and mean free time between collisions.

DIRECT-CURRENT CIRCUITS Chapter 4

RESISTORS IN SERIES AND PARALLEL When several resistors R 1, R 2, R 3, …, are connected in series, the equivalent resistance R eq is the sum of the individual resistances. The same current flows through all the resistors in a series connection.

RESISTORS IN SERIES AND PARALLEL

KIRCHHOFF’S RULES Kirchhoff’s junction rule is based on conservation of charge. It states that the algebraic sum of the current into any junction must be zero.

KIRCHHOFF’S RULES Kirchhoff’s loop rule is based on conservation of energy and the conservative nature of electrostatic fields. It states that the algebraic sum of potential difference around any loop must be zero.

KIRCHHOFF’S RULES

ELECTRICAL MEASURING INSTRUMENTS In a d’Arsonal galvanometer, the deflection is proportional to the current in the coil. For a larger current range, a shunt resistor is added, so some of the current bypasses the meter coil. Such an instrument is called an ammeter.

ELECTRICAL MEASURING INSTRUMENTS If the coil and any additional series resistance included obey Ohm’s law, the meter can also be calibrated to read potential difference or voltage. The instrument is then called a voltmeter.

ELECTRICAL MEASURING INSTRUMENTS A good ammeter has very low resistance; a good voltmeter has very high resistance.

R-C CIRCUITS When a capacitor is charged by a battery in series with a resistor, the current and capacitor charge are not constant. The charge approaches its final value asymptotically and the current approaches zero asymptotically.

R-C CIRCUITS

When the capacitor discharges, the charge and current are given as functions of time. The time constant is the same for charging and discharging.

R-C CIRCUITS

HOUSEHOLD WIRING In household wiring systems, the various electrical devices are connected in parallel across the power line, which consists of a pair of conductors, one “hot” and the other “neutral”. An additional “ground” wire is included for safety.

HOUSEHOLD WIRING The maximum permissible current in a circuit is determined by the size of the wires and the maximum temperature they can tolerate. Protection against excessive current and the resulting fire hazard is provided by fuses or circuit breakers.