Chapter 20 Summary Essential Concepts and Formulas.

Slides:



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

Halliday/Resnick/Walker Fundamentals of Physics 8th edition
3/6 do now A piece of copper wire with a cross-sectional area of 3.0 x 10-5 meter2 is 25 meters long. How would changing the length of this copper wire.
Electric Circuits AP Physics 1.
Fundamentals of Circuits: Direct Current (DC)
Chapter 19 DC Circuits. Units of Chapter 19 EMF and Terminal Voltage Resistors in Series and in Parallel Kirchhoff’s Rules EMFs in Series and in Parallel;
Chapter 28 Direct Current Circuits TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAA.
DC circuits Physics Department, New York City College of Technology.
Direct Current Circuits
Fig 28-CO, p.858. Resistive medium Chapter 28 Direct Current Circuits 28.1 Electromotive “Force” (emf)
Electric Current and Direct-Current Circuits
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
Direct Current When the current in a circuit has a constant direction, the current is called direct current Most of the circuits analyzed will be assumed.
Current and Circuits. Current current: the flow of charged particles. E Current is measured in Amperes (A) which is made of the unit of a Coulomb/sec.
Chapter 20 Electric Circuits.
Electricty. Object gain or lose electrons to become charged. Opposite charge attract likes repel. Any charge will attract a neutral object. When touching.
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.
Chapter 28 Direct Current Circuits. Electromotive Force An electromotive force device, or emf device, is a source of constant potential. The emf describes.
Chapter 28 Direct Current Circuits 1.R connections in series and in parallel 2.Define DC (direct current), AC (alternating current) 3.Model of a battery.
MHS Physics Department AP Unit III C 2 Steady state direct current circuits with batteries and resistors only.
FCI. Direct Current Circuits: 3-1 EMF 3-2 Resistance in series and parallel. 3-3 Rc circuit 3-4 Electrical instruments FCI.
Lecture 13 Direct Current Circuits
An electric potential difference exists between battery terminals. The maximum potential difference is called the electromotive force (emf) of the battery.
Chapter 18 Direct Current Circuits. Chapter 18 Objectives Compare emf v potential difference Construct circuit diagrams Open v Closed circuits Potential.
10/9/20151 General Physics (PHY 2140) Lecture 10  Electrodynamics Direct current circuits parallel and series connections Kirchhoff’s rules Chapter 18.
ADT490 Metering Techniques. 2 Introduction ‣ Alarms ALS390 ‣ Foundation for Troubleshooting.
DC Circuits. EMF and Terminal Voltage Electric circuit needs a battery or generator to produce current – these are called sources of emf. Battery is a.
Current Electric Current (I)
19 Current, Resistance, & DC Circuits. Electric Current Current: net charge passing through a cross-section per unit time. Units: Ampere (A), 1 A = 1C/s.
Capacitors in a Circuit emf Resistors series parallel Circuit problems Capacitors in a circuit.
Chapter 28 Direct Current Circuits. Introduction In this chapter we will look at simple circuits powered by devices that create a constant potential difference.
Series wiring means that the devices are connected in such a way that there is the same electric current through each device. One loop only for the flow.
Current of Electricity Electric Current Potential Difference Resistance and Resistivity Electromotive Force.
Regents Physics Chapters 17/18 Circuits  Series Circuits.
Electric Current and Circuits. What is Current? Electric current is a flow of electric charge Electric current is a flow of electric charge I = Q/t I.
AP Physics C Electric Circuits.
Chapter 28 Direct Current Circuits CHAPTER OUTLINE 28.1 Electromotive Force 28.2 Resistors in Series and Parallel 28.3 Kirchhoff’s Rules.
Chapter 20 Electric Circuits Electromotive Force and Current Within a battery, a chemical reaction occurs that transfers electrons from one terminal.
Review Exam 4. Chapter 18 Electric Currents Resistance and Resistors The ratio of voltage to current is called the resistance: (18-2a) (18-2b)
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.
Lectures 7 to 10 The Electric Current and the resistance Electric current and Ohm’s law The Electromotive Force and Internal Resistance Electrical energy.
Electrical Circuits ~Moving Charge Put to Use The Circuit All circuits, no matter how simple or complex, have one thing in common, they form a complete.
Current- the movement of charge. Symbol is I, unit is the Ampere (A) I = q/t 1 A = 1 C/s Conventional current- from the positive terminal to the negative.
Current and Resistance A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.
DC Circuits AP Physics Chapter 18. DC Circuits 19.1 EMF and Terminal Voltage.
Electric Circuits AP Physics C. Potential Difference =Voltage=EMF In a battery, a series of chemical reactions occur in which electrons are transferred.
5.2.2 D.C. Circuits Practical circuits Electromotive force and internal resistance Kirchhoff’s laws Series and parallel arrangements Potential divider.
CIRCUIT ANALYSIS ENGR. VIKRAM KUMAR B.E (ELECTRONICS) M.E (ELECTRONICS SYSTEM ENGG:) MUET JAMSHORO 1 OHM’S LAW.
Physics 12 Circuits 3 – Series Mr. Jean. The plan: Video clip of the day Power Series Circuits Resistance in Series Application of Ohm’s Law.
CURRENT, RESISTANCE, AND ELECTROMOTIVE FORCE Chapter 4.
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.
Combinations of Resistors Series and Parallel Rules Ohm’s Law Current Divider Rules (CDR) Kirchhoff’s Laws.
The Series Circuit Summary 1. The sum of the _____________or voltage equals the potential rise of the source. 2. The current is ______________ everywhere.
Chapter 20 Electric Circuits Electromotive Force and Current In an electric circuit, an energy source and an energy consuming device are connected.
Electric Current and Resistance
Internal Resistance in EMF
General Physics (PHY 2140) Lecture 6 Electrodynamics
General Physics (PHY 2140) Lecture 10 Electrodynamics
Electric Circuits.
Circuit in DC Instruments
AP Physics L09_circuits containing resistors
Current Electricity & Circuits W. Sautter 2007.
Electric Current And Related Parameters
Electric Current And Related Parameters
Ohm’s Law This formula shows the relationship between current, voltage and resistance. Voltage (Volts) Current (Amps) Resistance (Ohms, )
Circuits.
Series and Parallel Circuits
Electric Circuits.
Presentation transcript:

Chapter 20 Summary Essential Concepts and Formulas

Electromotive Force and Current The maximum potential difference V is called the electromotive force emf (not not a force as the name implies) Flow of charge is called electric current, I Measured in C/s = Ampere 2 Types of currents: Direct (DC) and Alternating (AC)

Ohm's Law Analagous to water flowing in a hose. In water, great pressure means larger water flow In electricity, greater voltage means larger current R=resistance Resistor: device that offers resistance Used to control current and voltage levels

Resistance and Resistivity Like in a hose, resistance relates to length and area Rho is proportionality constant known as resistivity of material Rho is inherent property of material, like density Like density, changes with temperature

Electric Power Definition: When charge flows from A to B in a circuit, leading to current I and voltage V, the electric power is P=IV Unit: Watt (W) Substituting other expressions for I and V, we obtain equivalent expressions for power

Alternating Current Similar to DC current, but voltage and current oscillate Equations are basically analogous to dc equations rms=root mean square. Obtained by dividing peak value by sqrt(2) Eqns aren't as important as concept of oscillation

Series Wiring If devices are in series, the current is the same everywhere in the circuit Equivalent resistance is sum of individual resistors (R s >R n ) You can still find power delivered to the resistors. In general, total power delivered is equal to power delivered to equivalent resistance

Parallel Wiring If devices are in parallel, the voltage is the same across each branch Equivalent Resistance R p <R n In general, total power is equal to power delivered to equivalent resistor Smallest resistance has largest impact (if one equals 0, short out occurs)

Circuits Wired Partially in Both Strategy: Break it up into series/parallel parts Deal with isolated resistors, find equivalent resistance Slowly, keep adding one more part at a time, so slowly eliminating resistors Once again, easiest way is to break the circuit into manageable parts

Internal Resistance and Kirchhoff's Rule Internal resistance: resistance of the battery depends on the current; the terminal voltage (delivered to the circuit) is the emf of the battery minus the internal resistance Junction rule: Current into a junction equals current out of a junction (conservation of charge) Loop Rule: For a closed-circuit loop, the total of all the potential drops is the same as the total of all the potential rises (conservation of energy)

Measurement of Current and Voltage Ammeter: Measures current at some point in the circuit. Probes must be inserted in series with the circuit. Meter should have a negligible resistance. Voltmeter: Measures the voltage between two points. Probes must be inserted in parallel with the circuit. Meter should have a negligible resistance.

Capacitors in Series and in Parallel As with resistors, there are equivalent capacitance when multiple capacitors in series Capacitors in series all have the same amount of charge on each plate of the capacitor Capacitors in parallel are charged to the same voltage

Summary of Equations