applied physics chap 61 electricity and magnetism
TRANSCRIPT
Applied Physics Chap 6 1
Electricity and Magnetism
Applied Physics Chap 6 2
Video: Electricity
Applied Physics Chap 6 3
Static Electricity: Electrical charges that collect on the surface of some object.
Static electricity is most noticeable when:
Air is dry
Friction is involved.
Applied Physics Chap 6 4
Discovery of electricity
The Greek work for Amber is “Electron” hence our word “electricity”
Early experimenters knew that a rubber rod rubbed with fur could accumulate static electricity
Similarly, a glass rod rubbed with silk would accumulate static electricity
Amber: a clear, resinous, yellowish rock, known since ancient times, made of petrified tree sap would build up static electricity when rubbed on fur.
Amber
Applied Physics Chap 6 5
Benjamin Franklin
Believed that all things held electricity.
Friction rubbed electricity off of the rubber rod and onto the fur. Thus the rod had less or “negative” electricity and the fur had more or “positive” electricity.
Franklin determined that charges moved from positive, having more electricity to negative, having less.
American scientific experimenter.
Applied Physics Chap 6 6
Charge: the fundamental electrical property to which the mutual attractions or repulsions between electrons or protons is attributed.
Electrical Charge comes in two forms:
Positive: carried by particles called Protons that are usually found in the nucleus of an atom.
Negative: carried by particles called Electrons that are usually found in a cloud surrounding an atomic nucleus.
Electrical Charge
Applied Physics Chap 6 7
Electrically charged particles exert forces on other electrically charged particles.
Like charges repel
Unlike Charges attract
– +
Unlike
+ +
Like
Applied Physics Chap 6 8
Charge: a fundamental electrical property which causes like charges to repel and unlike charges to attract.
Atoms have a nucleus containing positively charged protons.
The nucleus is surrounded by a cloud of negatively charged electrons.
The protons mass is 2000 times more massive than the electron’.
The protons positive electrical charge is of equal magnitude but opposite sign from the electrons electrical charge.
Conservation of Electrical Charge: Charge can be transferred from one object to another but the total number of charges always remains unchanged.
Charge can neither be created nor destroyed.
Applied Physics Chap 6 9
Electrical Force: a force that one charge exerts on another. when the charges are the same sign, they repel; when the charges are opposite, they attract.
+ -
+ +
Like Charges Repel
-+
Unlike charges Attract
Applied Physics Chap 6 10
The strength of the electrical force
The strength of the electrical force decreases as the inverse of the square of the distance between the two charges
- -+ +Stronger Weaker
-+++
- -- -+ -+ +
and gets stronger as the amount of charge increases.
Applied Physics Chap 6 11
Electrical Charge Induction
Induction: the charging of an object without direct contact.
Like charges repel and unlike charges attract even when objects are not touching.
Applied Physics Chap 6 12
Van de Graff Generator: a device that uses friction to build up a charge on surface of the hallow metal sphere.
1.) Hallow Metal sphere
2.) Copper brush
4/5.) Rubber belt
7.) drive motor
8.) Wand
9.) Spark.
Applied Physics Chap 6 13
Electric Field: a “force field” that fills the space around every electric charge or group of charges.
Electrical fields surround all charged particles and interact with the electrical fields of other charged particles causing push (repulsion) or pull(attraction) forces to occur.
Michael Faraday: 1791 –1867 an English experimenter who first proposed the existence of electrical fields and discovered that electrical and magnetic force fields were related.
Applied Physics Chap 6 14
Electroscope: A device that uses electrical fields and induction to detect nearby electrical charges.
Negative charges on the rubber rod push away negative charges on the electroscope causing the gold leaves to repel
When charged the two foil leaves are pushed far apart since both leaves carry the same charge.
Applied Physics Chap 6 15
Winds carry charged particles of ice upward causing the upper cloud to become positively charged and the lower cloud to be negatively charged
The cloud bottom induces a positive charge on the ground. When the charges grow large enough we get lightning.
Induction in Thunderstorms
Applied Physics Chap 6 16
Conductors and Insulators:
In metals, free electrons can move freely through the metal without being attracted by other atoms.
Insulator: a material, usually a non-metal, like rubber, glass or plastic that is a poor conductor of electricity.
In insulators, free electrons are strongly attracted by adjacent atoms and cannot move freely.
Conductor: a material, usually a metal, through which electrons can move without hindrance.
Applied Physics Chap 6 17
Electrical Potential Energy: energy is stored as a result of the distance between two or more electrical charges and their strengths.
Electric Potential: the potential energy available per unit of charge, measured in “volts”
Coulomb
Joules
eargch
energypotentialelectricPEe
Is equal to an electrical potential of 1 Volt
Voltage: the difference in electric potential between any two points in an electric field.
Voltage = Vneg –Vpos
Applied Physics Chap 6 18
Voltmeter: An instrument used to measure the difference in electric potential between two points
Voltmeters are connected in parallel with voltage sources.
Applied Physics Chap 6 19
Selector switch
Voltage Scale
Applied Physics Chap 6 20
Andre Ampere (1775 – 1836)
was a French physicist who is generally credited as one of the main discoverers of electromagnetism. The SI measurement unit for electrical current, the ampere, is named after him.
Electric current: is a measurement of how many electrical charges are moving through a conductor each second in units called Ampere’s,
Ampere1C second1
Coulomb1
time
chargeelectricurrent
Applied Physics Chap 6 21
Voltage sources and Batteries:
Storage batteries accumulate charge from a chemical reaction. An electrolyte, usually an acid, reacts with the different metal electrodes located at the two ends of the battery.
Negative electrons accumulate at the Cathode (the negative electrode) and positively charged atoms accumulate at the anode (the positive electrode).
This potential difference between the positive and negative charges at the two electrodes creates the voltage.
The positive anode is said to be at 0 volts.
Applied Physics Chap 6 22
Wet Cell Battery
Automobile batteries have a liquid electrolyte solution composed of water and Sulfuric Acid, with lead and zinc electrodes.
Applied Physics Chap 6 23
Dry Cell battery
DRY CELL” batteries or Flashlight type batteries are sealed at the factory and have a thick paste that serves as the electrolyte.
Dry cells are portable and can be readily carried and changed whenever they discharge.
Applied Physics Chap 6 24
Electric resistance: the amount of resistance a material offers to the flow of electric charges moving through it. The lower the resistance, the smaller the voltage needed to push electrons to through it.
Applied Physics Chap 6 25
The resistance, R, of a length of wire is described by the
expression: R = ρL/A where
ρ = resistivity of the material composing the wire,
L = length of the wire in metersA = area of the conducting cross section of
the wire in m2.
Calculating wire resistance
Applied Physics Chap 6 26
Reading Resistor Codes.
Small resistors have a color code that describes their resistance
First Band10’s place
Second BandOne’s place
Third BandPower of 10
Fourth Bandtolerance
For example: a green first band means “50
A black second band means 0
A red third band means multiply by 102 or 100
Resistance = 50 x 100 or5000
Applied Physics Chap 6 27
Resistor tolerances:
Since resistors are very small, it is difficult to manufacture an exact resistance amount.
Tolerance gives the highest and lowest resistance that a given resistor may actually have.
Nominal value: the target resistance of a resistor say 5000.
A tolerance of 5% means that an acceptable resistor may actually be 5000 + 5% = 5000 + 250 = 5250 or
5000 – 5% = 5000 – 250 = 4750
Resistors are available with tighter tolerances but they are much more expensive.
Applied Physics Chap 6 28
Resistance is measured in units called Ohms.
Georg Ohm 1789 - 1854
As a high school teacher, Ohm worked with a battery invented by Alessandro Volta and equipment of his own invention to define the fundamental relationship among voltage, current, and resistance, which we now know as Ohm’s Law.
Applied Physics Chap 6 29
Ohm’s Law: Current in a simple circuit
R
VI
Ohms
Volts
Amperes
Resistance
VoltageCurrent
I
VR
R
VIIRV
Applied Physics Chap 6 30
Direct Current: Negative charges that flow continuously from the negative to the positive electrode of a battery.
Even though the electron moves slowly through the wire, the nudging of one electron on another travels through the circuit almost instantaneously.
The electrons in a light bulb instantly feel the full force of the voltage and react to lighting the light.
Negative charge
Positive charge
Push Pull
Applied Physics Chap 6 31
Conductor
Circuit: a complete continuous path of conductors through which electrical charges can flow
Voltage Source
Resistance or Load element
Control element or switch
Applied Physics Chap 6 32
Video: Series and Parallel
Applied Physics Chap 6 33
Voltage source: a battery or other form of power supply that provides a continuous source of electrical potential.
The symbol for a battery is:
Conductor: a metal wire or other device that creates a continuous path for electrons to flow through.
The symbol for a conductor is:
Applied Physics Chap 6 34
Load, or Resistance: any device that converts electrical energy into heat, light or motion.
Resistor: is a device that converts electrical energy into heat The symbol for a resistor is:
The symbol for a light bulb is:
Control or switch: an element that can interrupt, stop or reduce the flow of current in a circuit. Symbol for a closed switch is:
Symbol for an open switch is:
Applied Physics Chap 6 35
Series Circuit: A circuit arranged in such a way that there is only one path for current to flow and charges must flow through each element in turn.
Voltages in a Series Circuit Add
1.5 V + 1.5 V + 1.5 V = 4.5 V
If you reverse a battery then:
1.5 V - 1.5 V + 1.5 V = 1.5 V
Applied Physics Chap 6 36
Resistances in series: ADD UP
5 + 10 + 15 = 30
Resistances don’t care which way you install them.
Applied Physics Chap 6 37
Calculating Currents in a series Circuit:
Conductor 30 V
5
10
2.) Use Ohm’s Law to calculate current.
.Amperes215
V30
R
VI
1.) Add up any resistances: 5 + 10 = 15
Applied Physics Chap 6 38
Voltage drop: the voltage used by each load element in a series circuit. The voltage drop is equal to V = IR where I is the series current and R is the resistance of each load element.
Like voltages, voltage drops in a series circuit add up to the total voltage in the battery.
Kirchoff’s law of voltages
The sum of all voltage drops is equal to the voltage of the battery.
Applied Physics Chap 6 39
Voltage drops: V = IR
For the 10 resistor, V = (2A)(10 ) = 20 V
For the 5 resistor, V = (2A)(5 ) = 10 V
Total voltage = 30 V
Conductor 30 V
5
10
I = 2A
Applied Physics Chap 6 40
Series circuits:
Have one single path for current to follow
Voltage is used up by each load element in the circuit.
The sum of all voltage drops is equal to the battery voltage.
Current is the same for all load elements and must flow through all load elements in turn.
Resistance adds in a series circuit.
Applied Physics Chap 6 41
Parallel Circuits: A circuit with 2 or more paths for current to flow.
30 V 5 10
Each load element sees a full 30V of potential
Each load element has a current calculated as:
.Amperes65
V30
R
VI
.Amperes310
V30
R
VI
Applied Physics Chap 6 42
Voltage sources in parallel do not add.
1.5 V +
1.5 V +
1.5 V +
= 1.5 V
Currents In each of the parallel paths add to equal the total current: IT = I1 + I2
VI1
I2
IT
Kirchoff’s Law of Currents
Applied Physics Chap 6 43
Parallel Circuits:
Have two or more paths for current to flow.
Each load element sees full system voltage.
Currents divide to each load element in the circuit.
The sum of all individual currents equals the total system current.
Voltage sources in parallel do not add.
Applied Physics Chap 6 44
Equivalent Resistance: a resistance equal to the effect of placing two or more resistances in parallel.
Equivalent resistance is usually around half of the smaller of the parallel resistances.
Equivalent resistance: of two resistors R1 and R2 is found using the formula:
3333
1
12
1
101
51
111
1
21
....
RR
RT
X15 + 10
X1 =
X1
Calculator:
Applied Physics Chap 6 45
Calculating Currents in a Parallel Circuit
30V 5 10
Use Ohm’s law to find the current in each parallel path:
For the 2 resistors:
A
IIIcurrentTotal
AV
R
VI
AV
R
VI
T
963
310
30
65
30
21
22
11