Electromotive Force Elliott.

Slides:



Advertisements
Similar presentations
Current Electricity & Ohm's Law.
Advertisements

Internal Resistance.
How We Load Power Supplies. All sources have an EMF. EMF is the open terminal voltage of the battery. All sources have a certain amount of internal resistance.
Unit 3 Day 5: EMF & Terminal Voltage, & DC Resistor Circuits Electromotive Force (EMF) Terminal Voltage Internal Resistance Series, Parallel, and Series-
+ V (Volt) = W (work done, J) Q (charge, C)
Current. Current Current is defined as the flow of positive charge. Current is defined as the flow of positive charge. I = Q/t I = Q/t I: current in Amperes.
Series and Parallel Circuits
T-Norah Ali Al-moneef King Saud University
What are we doing today? Internal Resistance Emf Using a graph to find the internal resistance and emf of a potato cell.
Week 04, Day 2 W10D2 DC Circuits Today’s Reading Assignment W10D2 DC Circuits & Kirchhoff’s Loop Rules Course Notes: Sections Class 09 1.
Year 12 Current Electricity Lesson 3 Potential difference and power
Current Electricity.
Lecture 12 Current & Resistance (2)
Electricity. Starter:  What is current?  What is it measured in?  What is it measured by?  Which is the series and parallel circuit? (see board)
Electricity and Magnetism Topic 5.2 Electric Circuits.
Topic 5.1 Electric potential difference, current and resistance
Current Electricity Electric Current Circuit – continuous conducting path between terminals of a battery (or other source of EMF) Electric Current.
Electric Currents Topic 5.2 Electric Circuits. Electromotive Force Defining potential difference Defining potential difference The coulombs entering a.
Electricity – Potential Difference
Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.
Direct Current And Resistance Electric Current The Battery Resistance And Ohm’s Law Power Internal Resistance Resistors In Combination RC Circuits Written.
Holt: Physics Ch. 20 – 1 Pages
19.4 Sources of electromotive force
Potential difference and electromotive force.
(1)A source voltage, that is, an electron pump usually a battery or power supply. [ ENERGY IN] (2) A conductor to carry electrons from and to the voltage.
Short circuiting a battery demo… Dangerous ? High current?
Phys 2180 Lecture (5) Current and resistance and Direct current circuits.
Physics ( ) Electrical Circuits Varying Resistance © SSER Ltd.
Current of Electricity Electric Current Potential Difference Resistance and Resistivity Electromotive Force.
2 But what makes the electrons flow? Any electrical circuit requires three things 1.A source 2.A load 3.A means of transmission A definition of a current.
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.
Electromotive Force and Internal Resistance Before we start, the golden rules from GCSE:  The ? through any components connected in series is the same.
Unfortunate book names:. A circuit must contain a source of potential difference, and a path for the flow of charge. It will probably also contain.
CH Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across.
Emf and Internal Resistance To do Work in groups of 4 or 5 to carry out Activity 2 – Internal Resistance. Internal Resistance V In theory… V = 12 V In.
EMF and Internal Resistance Electricity Lesson 8.
5.2.2 D.C. Circuits Practical circuits Electromotive force and internal resistance Kirchhoff’s laws Series and parallel arrangements Potential divider.
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.
Internal Resistance E r The battery produces an electromotive force (emf), E, however the electrons loose some of this energy in travelling through it.
Internal Resistance. electromotive force revisited Remember the e.m.f.(ε) is the amount of energy given by the cell to each coulomb of charge passing.
ELECTROMOTIVE FORCE. Consider the following diagram showing a circuit with an external resistance (R) internal resistance (r) and EMF ( ε ). When.
Internal Resistance Review Kirchhoff’s Rules DC Electricity.
1© Manhattan Press (H.K.) Ltd Potentiometer Comparing resistances Measuring the e.m.f. of a cell Measuring the internal resistance of a cell.
Chapter 20 Electric Circuits Electromotive Force and Current In an electric circuit, an energy source and an energy consuming device are connected.
1 TOPIC 7 Electric circuits. 2 Charges will flow to lower potential energy To maintain a current, something must raise the charge to higher potential.
Chapter 26 DC Circuits. I The wires used in homes to carry electricity have very low resistance. However, if the current is high enough, the power will.
Current = charges in motion
A –Level Physics: Electrical Quantities: Internal Resistance
Circuits!.
Potential Changes Around a Circuit.
Electronics Circuits.
Cell energy ☺ electron lamp.
Internal Resistance and the EMF of a cell
Electric Circuits AP Physics 1.
Calculate the current at point A
Electromotive Force and Potential Difference
University Physics: Waves and Electricity
Electric Circuits.
ELECTROMOTIVE FORCE AND POTENTIAL DIFFERENCE
Electric Circuits.
AP Physics Section 19-1 to 19-3 Simple DC Circuits.
E.M.F and Internal Resistance
Electromotive Force and Potential Difference
Current Electricity & Circuits W. Sautter 2007.
Ideal vs Real Battery Ideal battery: no internal energy dissipation
Electricity.
Electrical Circuits Varying Resistance
Unit 1 Electricity Electric Fields and Potential Difference
Electricity and Magnetism
Unit 1 Electricity Electric Fields and Potential Difference
Presentation transcript:

Electromotive Force Elliott

Work Done Batteries (or more strictly speaking cells) convert chemical energy into electrical energy.  Generators turn kinetic energy into electrical energy.  In doing so, they keep the negative terminal with an excess of electrons and the positive terminal with a deficiency of electrons. A battery does a job of work in pumping the electrons around the circuit.  Positive charges do not move.

EMF A battery is said to produce EMF (electromotive force) which is defined as: The energy converted into electrical energy when a unit charge passes through the source. It represents the total energy that can be supplied to a circuit

Check Your Progress What is the difference between emf and potential difference?

Answer Emf is the total energy supplied to the circuit  per unit charge, p.d. is the energy per unit charge converted to other energies by the components. 

Working Definition EMF is the open circuit terminal voltage of the battery, i.e. when there is zero current flowing. A digital multimeter will give you a good reading as it takes a very small current.

Equation for EMF The energy supplied to a circuit by a battery is given by: W is the energy in J Q is the charge in C E , curly E, is the physics code for emf.

Check Your Progress A battery converts 13 000 J of chemical energy into electrical energy.  It does so by giving a current of 0.5 A for 2 hours.  What is its emf?

Answer Convert 2 hours to seconds. 2 h = 7200 s Q = It = 0.50 * 7200 = 3600 C Emf = W/Q = 13 000 J ¸ 3600 C = 3.6 V

Internal Resistance All batteries and generators dissipate heat internally when giving out a current, due to internal resistance.  A perfect battery has no internal resistance, Unfortunately there is no such thing as a perfect battery! (Nickel-Cadmium and Lead-Acid batteries have very low internal resistance, and we can regard these as almost perfect.  These batteries can provide very high currents).

Check Your Progress Define a “perfect voltmeter” What is meant by a perfect battery?  Why are real batteries not perfect?

Kirchhoff's Laws

Answer A perfect voltmeter shows infinite resistance. A perfect battery has no internal resistance A real battery has internal resistance

Internal Resistance Cont. In this circuit the voltmeter reads (very nearly) the emf. Suppose we now add a load.  We will assume the wires have negligible resistance. This time we find that the terminal voltage goes down to V.  Since V is less than E, this tells us that not all of the voltage is being transferred to the outside circuit; some is lost due to the internal resistance which heats the battery up.  Emf = Useful volts  + Lost volts E  = V + v

Check Your Progress How is this statement consistent with Kirchhoff II?

Answer Kirchhoff II says that the voltages in a circuit add up to the emf . Here we see that there is a p.d. across a resistor and a p.d. across the internal resistance .

Representing internal Resistance we can represent this circuit as: We can now treat this as a simple series circuit and we know that the current, I, will be the same throughout the circuit.  We also know the voltages in a series circuit add up to the battery voltage. Emf = voltage across R + voltage across the internal resistance

Deriving the Equation E = IR + Ir E = I(R + r)       Emf = voltage across R + voltage across the internal resistance    E  =         V                        +                     v We also know from Ohm’s Law that V = IR and v = Ir, so we can write: E = IR + Ir   E = I(R + r)

Exam Tips Many students panic at the sight of internal resistance problems. All you have to do is turn the cell with the internal resistance into a perfect battery in series with its internal resistor, and treat it as a simple series circuit.

Worked Example A battery of emf 12 volts and internal resistance 0.5 W is connected to a 10 W resistor.  What is the current and what is the terminal voltage of the battery under load?

Check Your Progress A battery has an internal resistance of 0.50 W.  The battery has an emf of 1.52 V.  When it is connected to a resistor, the terminal voltage falls to 1.45 V.  What current is flowing.  What is the value of the resistor? 

Answer The current = 0.07 V ¸ 0.5 W = 0.14 A Terminal voltage = 1.45 V   Voltage drop = 1.52 V – 1.45 V = 0.07 V   The current = 0.07 V ¸ 0.5 W = 0.14 A    Terminal voltage = 1.45 V    External resistance = 1.45 V ¸ 0.14 A = 10.4 W = 10 W to 2 s.f.

Measuring Internal Resistance The graph is a straight line, of the form y = mx + c.  We can make the equation for internal resistance  V = -rI + E.  There are three features on the graph that are useful: The intercept on the y-axis tells as the emf. The intercept on the x-axis tells us the maximum current the cell can deliver when the p.d. is zero, i.e. a dead short circuit. The negative gradient tells us the internal resistance.

Resistance of Wires We assume that wires are perfect conductors, i.e. have zero resistance.  However wires have a definite value of resistance. This cord can carry a current of 13 A.  However it needs to be fully unwound to do so.  When carrying a heavy current, the cable gets warm.  If it were coiled up, the temperature rise could become excessive, which would be hazardous.  There is energy loss in the wires.   The resistances in this wire are: 0.4 W for the fuses (one fuse in each plug); 0.7 W for the live wire; 0.7 W for the neutral wire.

It is connected to the tumbler drier like this: A tumbler drier takes 12 A from the 230 V mains.  We can represent the power supply as a perfect source in series with resistances.  It is connected to the tumbler drier like this:  

Check Your Progress A tumbler drier of rated power 2300 W is connected to a plug using an extension lead that is 15 m long.  The resistance of each conductor is 0.7 W and there are two plugs, each of which has a fuse of resistance 0.1 W.  This is shown in the diagram above. a.  Show that the current flowing through the tumbler drier is about 9.4 A. b.  Calculate the voltage across the tumbler drier. c.  Calculate the power across each of the two fuses. d.  Calculate the power lost in the cable. e.  Work out the actual power of the tumbler drier.

Answer