chapter 3 - electrical properties chapter 4 - electrical quantities

43
Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Upload: corey-reeves

Post on 19-Jan-2016

242 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Chapter 3 - Electrical PropertiesChapter 4 - Electrical Quantities

Page 3: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Elements and Compounds

Element - a substance that cannot be reduced to a simpler substance by chemical means

ie: iron, gold, silver...

Page 4: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Atoms

The smallest particle of an element that retains the characteristics of that element.

Atoms are like letters, molecules are like words

ie: the water molecule

Page 5: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Electrons vs. Protons

Electrons are negatively charged (-)

Protons are positively charged (+) Electrons and protons attract each

other

Page 6: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Atomic Number

Atomic Number is the number of protons in its nucleus

Page 7: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Electron orbits Electrons can only “jump” orbits or

shells in steps

The number of electrons in any particular orbit follows the equation:

# Electrons = 2n2

n = orbit number

Page 8: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Electron Orbits

There can be as many as 7 shells in an atom

– K, L, M, N, O, P, and Q How many electrons, if full, would be in 7th shell?

How many shells would the electrons in the silver atom fill?

Page 9: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Sub-shells of Orbits

–Each Orbit (K, L, M, N, O, P, and Q)

has sub-shells (s, p, d, f, g)

http://en.wikipedia.org/wiki/Electron_shell

–How many electrons in Orbit N

sub-shell f?14

Page 10: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Orbit 1Orbit 2

Orbit 3

Orbit 4Orbit 5

.

.

.

Subshell 1

Subshell 2

Subshell 3

Subshell 4

Subshell 5

Page 11: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Valence Electrons

The valence electron is the number of electrons in the outermost shell of an atom. (Not sub-shell) http://au.answers.yahoo.com/question/index?qid=20080327135829AA6jdpj Valence electrons may be easy or hard to be freed. Atoms tend to want to be neutral.

Page 12: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

How many valence electrons in copper?

1

Page 13: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Conductors vs. Insulators

Conductors usually have 3 or less valence electrons. Why? Insulators usually have 5 or more valence electrons.

Semiconductors?• How many valence electrons• Definition

Best Conductors:• Silver• Copper• Gold• Aluminum

Good Insulators• Rubber• Plastic• Glass

Common semiconductors• Germanium• Silicon

Page 14: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Semiconductors

Conductivity increases with increasing temperature• This is opposite of metal

Useful properties• Can pass current more easily in one direction than

the other, • Variable resistance• Sensitivity to light or heat.

Conductivity can be modified by adding impure atoms (atoms that are not purely semiconductive)

Page 15: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

ResistiveConstants

Page 16: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Static Electricity

Shielding wire EMI (ElectroMagnetic Interference) Grounding

Page 17: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Random Video of the Day

Lizard.wmv

Page 18: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

B * C

D2A

A = 2B = 3C = 4D = 2

F =

F = ?

Page 19: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Coulomb’s Law of Charges

Relational Force between particles

F = force in Newtonsq1, q2 = the charges in coulomb units

k = Coulomb’s constant = 8.988x109

d = distance in meters between charges

= ?= .4mC 56nC

= 5mm

1 Coulomb is like a large group of electrons6.25x10^18 electrons

d - Can also be imagined as the area in the electric field

Answer8053 N

So how many Coulomb’s is 1 electron??? 1.6 x 10-19 C

𝐹=𝑘𝑞1𝑞2

𝐷2

Page 20: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

More Coulomb’s Law practice problems...(aka worksheet)

Page 21: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Chapter 4 – Electrical Properties

What is Current?

What is Voltage?

What is Resistance?

Page 22: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Voltage, current & resistance analogy

- ------ --- -

-

Page 23: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Introduction Video

http://www.youtube.com/watch?v=EJeAuQ7pkpc&feature=fvw

http://www.youtube.com/watch?v=EJeAuQ7pkpc&feature=fvw

Page 24: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Current

Current is a movement of charged particles

Within metal conductors, the charged particles that are moving are electrons.

These electrons flow when there is a potential difference in the charges across a conductor. Aka: protons are on the other side.

Page 25: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Current – electron flow model The current you are used to working

with is nothing more than moving electrons, moving from a region of negative charge to an area of positive charge.

As a potential difference is impressed across the conductor, the positive terminal of the battery attracts electrons beyond point A. Point A becomes positive because it now has an electron deficiency. As a result, electrons are attracted from point B … and so on.

This is true for metal conductors.

Page 26: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Current – Conventional current flow If you Google “current” or look in a

friends electrical engineering book, you might find that current flows from positive to negative.

A few perspectives on this include:• Currents of positive ions• Hole Charge Current in p-type

semiconductors Arrows shown on diodes and transistors

are for current, not electron flow

Page 27: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Electron Flow vs. Conventional Current Flow

Which one do we use???• Electron Flow

However I will still call it current.

+-

+-

Electron FlowConventional Current Flow

Page 28: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Current Magnitude If the potential difference is

increased, the electric field is stronger, the amount of energy imparted to a valence electron is greater, and the magnitude of current is increased.

Page 29: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Current Magnitude If 6.25 x 1018 electrons pass a

given point in one second, then this is called one amp.

electrons second

6.25 x 1018 Coulomb second

= 1 = 1 Amp

Q t

I =

Page 30: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Voltage

So what causes there to be a potential difference in charges across a conductor?• (how do you get protons to be stored

on one side and electrons on the other?)

There are 6 ways this can be done, and this is part of your homework to look up.

Page 31: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Kinetic vs Potential Energy

Kinetic Energy Potential EnergyThe energy possessed by a

body because of its motion

The energy of a particle or system of particles derived from position, or condition, rather than motion.

ie: a roller coaster, a moving car ie: a stretched rubber band, a coiled

spring.

In our case, a BATTERY!

Page 32: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Voltage

Voltage is also known as• Electromotive Force (EMF)

– Usually associated with the voltage a battery makes

• Potential difference– Difference in charges

Page 33: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Voltage Example

How much voltage is produced when you shock someone?• When you feel it: 2,000 V• When you see it: 8,000 V• Maximum spark: 25,000 V

Page 35: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Voltage in a battery

Just like a rubber band that has been stretched, there is potential for it to do work when released.

This is similar to the storage of voltage in a battery

Batteries only have a certain amount of charge stored before they run out.

Page 36: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Voltage is Relative

Clapping example Without a reference point, a

voltage of 12V is meaningless. The reference point for voltage

most of the time is ground, or 0V. However, there are different types

of grounds. How is an airplane grounded?

Page 37: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Voltage is Relative (cont.)

For example, what is the voltage at this point, if each battery is 1.5V?

Depends, if its referenced to:• Ground• Negative side of same battery• Top of battery above…

+

-

Page 38: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Another RVOTD

https://www.youtube.com/watch?v=FGoaXZwFlJ4

Page 39: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Resistance

Resistance is an opposition to current flow Resistance can be made by:

• Varying the type of material, (think valence electrons)

• Varying the length of material• Varying the amount or cross-section of

material Resistors are like poor conductors. The

are somewhere between a conductor and an insulator

Page 40: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Resistors (cont.)

Resistors are a little like transducers in that they convert electrical energy into heat.

Voltage is converted into heat when electrons bump into each other so voltage is lost.

Page 41: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

What is the opposite of resistance?

Conductance

G = 1R

Measured in Siemens [S]

Page 42: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

A practical Electric Circuit

Below is a schematic diagram of a flashlight.

Page 43: Chapter 3 - Electrical Properties Chapter 4 - Electrical Quantities

Schematic Symbols (pg 59 of book)