Title: Physics Around the Home
1Physics Around the Home
- Electrostatics.
- Electricity.
- Heat and Temperature.
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3What is Electric Charge?
- The unit of electric charge is the coulomb.
- Ordinary matter is made up of atoms which have
positively charged nuclei and negatively charged
electrons surrounding them. - Charge is quantized as a multiple of the electron
or proton charge - Charge on a Proton p 1.602 x 10-19 coulombs
- Charge on an Electron e - 1.602 x 10-19
coulombs
4The Key to Electrostatics
- Like Charges Repel, Unlike Charges Attract.
- 1 Coulomb of charge contains 6.25 x 1018
elementary charges.
5Coulombs Force Law
- The force between two charges is proportional to
the size of those charges and inversely
proportional to the square of the distance
between them. This is known as an inverse square
law.
Q1
Q2
d - separation
6Problem using Coulombs Law
- What is the magnitude of the electric force on
the electron (Q1 1.6 x 10-19C) of a hydrogen
atom exerted by the single proton (Q2
1.6x10-19 C) that is its nucleus, when the
electron orbits the proton at its average
distance of 0.53 x 10-10 m.
7Problem II Coulombs Law involving 3 charges
- Calculate the net electric force on particle 3
(the 4.0 mC on the right) due to the other two
charges.
0.30m
0.20m
Q1 -3.0µC
Q2 5.0µC
Q3 -4.0µC
8Solution to 3 charge problem
- Logic The net force on the 4.0 mC particle will
be the vector sum of the force exerted by the
3.0 mC particle and the force exerted by 5.0 mC
particle.
-4.0mC
Due to the 5mC charge
Net force of 4.1N
Due to the -3mC charge
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10Electric Fields
- The Electric Field
- Energy and Electric Potential
- Millikans Oil Drop Experiment
11Electric Field Strength
- Field around a positive charge
- The Electric Field Strength at any point in space
is defined as the force F exerted on a tiny
positive test charge at that point divided by the
magnitude of the charge. - E F/q
q
12Electric Field Strength
- Field around a negative charge
- Electric Field Strength has units of Newtons per
coulomb (N/C) - It is a vector quantity
13Electric Field Strength
- The Electric Field Strength E due to a single
point charge Q at a distance d is given by - .
14Properties of Field Lines
- 1. The field lines indicate the direction of the
electric field the field points in the direction
tangent to the field lines at any point. - 2. The lines are drawn so that the magnitude of
the electric field, E, is proportional to the
number of lines crossing unit area perpendicular
to the lines. The closer the lines, the stronger
the field. - 3. Electric Field lines start on positive chares
and end on negative charges and the number
starting or ending is proportional tot he
magnitude of the charge.
15Fields between charges
- Field between two point charges
- Field between two parallel plates.
positive
negative
16Electric Potential
- Consider two parallel plates.
High P.E.
- - - - - - - - - - - - - -
Low P.E
Where is a small test charge
17Relationship between Electric Potential and
Electric Fields.
- The work done W by the electric field to move a
positive charge q from b to a is - W q Vba (1)
- We can also write the work done W as the force
F times distance d - W Fd (2)
- The Force F on a small positive test charge q
in an electric field E is - F q E (3)
- Consider two parallel plates.
High PE
b
a
- - - - - - - - - - - -
Low PE
18Relationship between Electric Potential and
Electric Fields.
- Substituting (3) into (2) we get
- W q E d (4)
- where d is the distance between points a and
b. - We now equate equation (4) to equation (1), we
get - qVba q Ed
? V Ed
19The Electron Volt - A Unit of Energy
- The joule is a very large unit when dealing with
energies of electrons, atoms or molecules. - One electron volt is defined as the energy
acquired by an electron as a result of moving
through a potential difference of 1 V. - 1 eV 1.6 x 10-19 J.
20Electric Potential Due to a Single Point Charge.
- The electric Potential at a distance r from a
single point charge Q is given by
r
Q
21Millikans Oil-drop Experiment.
- Consider two charged parallel plates.
- Millikan measured the charge of an electron.
- A drop is suspended if the electric and
gravitational forces are balanced. - Fw mg
- Fe Eq
- ? Eq mg
Fe
Fw
22Electricity
- Electric Current.
- Voltage
- Resistance
- Series and Parallel Ciruits.
- Kirchhoffs Laws
23Electric Current.
- The flow of charge in a wire is called current.
- It is expressed in terms of the number of
coulombs per second going past a given point on a
wire. - One coulomb/sec equals 1 ampere (symbol A) and
corresponds to a flow of about 6.24 1018
electrons per second past any point of the
circuit - The unit of electric current is named after the
French physicist André Marie Ampère.
André Marie Ampère (1775-1836)
24Voltage.
- When 1 coulomb of charge travels across a
potential difference of 1 volt, the work done
equals 1 joule. - The unit named after the English physicist James
Prescott Joule (1818-1889).
25Resistance and Ohms Law
- The unit used for expressing the quantity of
resistance is the ohm. The symbol for the ohm is
the Greek letter ?, omega. - It is defined as the amount of resistance that
will limit the flow of current to 1 ampere in a
circuit with a potential difference of 1 volt. - OHMS LAW V I R, in which V is the votage (in
volts), I is the current in amperes, and R is the
resistance in ohms.
26Resistors
- Measuring the value of the Resistance.
- Colour Code
- Series and Parallel Circuits
27Voltmeter-Ammeter Method
- The ratio of V/I gives the resistance.
- A graph of V vs I will produce a straight line
with the slope being the resistance, in ?
A
R1
V
V
28Wheatstone Bridge
- This is a slide-wire potentiometer.
- When the bridge is balanced, no current flows
through the Galvanometer.
L1
Rx
G
V
R1
L2
29Colour Code used on Resistors.
- Black 0 Brown 1 Red 2 Orange 3 Yellow
4 Green 5 Blue 6 Violet 7 Grey 8
White 9 - Associated error gold 5 silver 10 none 20
tolerance
multiplier
Second digit
First digit
30Series Circuits
- Rt R1 R2 R3 . .
-
- Vt V1 V2 V3 . .
- It I1 I2 I3 . .
R1
R2
V
R3
31Parallel Circuits
- Vt V1 V2 V3 . .
- It I1 I2 I3 . . .
R1
R2
V
R3
32Kirchhoffs JUNCTION Rule for Circuits
- G.R.Kirchhoff (1824-1887)
- It is based on the conservation of charge
- At any junction point, the sum of all currents
entering the junction must equal the sum of all
the currents leaving the junction.
33Kirchhoffs Loop Rule for Circuits
- It is based on the conservation of energy.
- The algebraic sum of the changes in potential
around any closed path of the circuit must be
zero.
34Power in Electric Circuits
- The electric power in watts associated with a
complete electric circuit or a circuit component
represents the rate at which energy is converted
from the electrical energy of the moving charges
to some other form, e.g., heat, mechanical
energy, or energy stored in electric fields or
magnetic fields.
35Heat and Temperature.
- Heat and Thermal Energy
- Law of heat exchange
- Specific Heat and Latent Heat.
36Heat as Energy Transfer
- Heat refers to energy that is transferred from
one body to another because of a difference in
temperature. - It is measured in JOULES.
- A common unit for heat was the CALORIE. It was
defined as the amount of heat necessary to raise
the temperature of 1 gram of water by 1 degree
Celsius. - 1 Calorie 4.189 Joules.
37Specific Heat Calorimetry
- The amount of heat Q required to change the
temperature of a system is found to be
proportional too the mass m of the system and to
the temperature change ?T, and can be expressed
in the equation - Q m c ?T
- where c is a quantity characteristic of the
material called specific heat.
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39Specific Heat Problem
Problem - How much heat is required to raise the
temperature of 20 kg of iron form 10oC to
90oC? Solution - Data - specific Heat for Iron c
450 J/kgoC Temperature Change ?T
(90-10) 80oC. Thus Q m c ?T 20 x 450 x 80
7.2 x 105 J. Therefore the amount of heat
required was 720 kJ.
40Law of Heat Exchange
- The law of heat exchange has its origins in the
law of conservation of energy. - If the system is completely isolated, no energy
can flow into or out of it the heat lost by one
part of the system is equal to the heat gained by
the other part of the system. - Heat lost heat gained.
41Heat Exchange Problem
- Problem - If 200 cm3 of tea at 95oC is poured
into a 150 g glass initially at 25oC, what will
be the final temperature of the mixture when
equilibrium is reached, assuming that no heat
flows to the surroundings?
42Solution Since tea is mainly water, its
specific heat is 4180 J/kg oC and its mass is its
density times its volume m ? V 1x103 x 200 x
10-6 0.20 kg Using the law of heat exchange
(and let T be the final Temperature of the
mixture) heat lost heat gained mtea ctea ?T
mcup ccup ?T 0.20 x 4180 x (95-T) 0.15 x 840 x
(T-25) 79 420 - 836T 126 T - 3150 T 85.8 oC
43Heat Exchange Problem
- We wish to determine the specific heat of a new
alloy. A 0.150 kg sample of the alloy is heated
to 540oC. It is then quickly placed in 400g of
water at 10.0oC which is contained in a 200 g
aluminum calorimeter cup. The final temperature
of the mixture is 30.5oC. Calculate the specific
heat of the alloy.
44Data Required for this problem to find Calloy
- Mass of alloy malloy 0.150 kg
- Temperature Change for alloy
- ?Talloy (540-30.5) 509.5oC
- Mass of water mwater 0.40kg
- Specific Heat of water cwater 4180 J/kg oC
- Temperature Change for water
- ?Twater (30.5 - 10) 20.5oC
- Mass of the calorimeter cup mcup 0.20kg
- Specific Heat of the cup ccup 900 J/kg oC
- Temperature Change for the cup
- ?Tcup (30.5 - 10.0)20.5oC
45Solution to the problem
- Heat Lost Heat Gained
- Heat lost by alloy heat gained by water and cup
- maca?Ta mwcw?Tw mccc?Tc
- 0.15 x ca x 509.5 0.4 x 4180 x 20.5 0.2 x 900
x 20.5 - 76.4 ca (34 300 3700)
- ca 500 J/kg oC.
- Therefore the specific heat of the alloy was 500
J/kg oC.
46Latent Heat
- The heat required to change the phase of a
substance (eg from solid to a liquid) is known as
Latent Heat. - When the substance is changing phase, there is no
change in the substances temperature. - The formula is simply
- Q m L
- where Q is the heat (in Joules), m is the mass
(in kg) and L is the Latent Heat (in J/kg)
47Latent Heat of Fusion Lv
- The Latent heat of fusion is the amount of heat
required to change 1.0kg of a substance from the
solid to the liquid state. - For example, when 5.00kg of water freezes at 0oC,
the water must release - Q m L 5.00 x 3.33 x 105
- ? Q 1.67 x 106 J of energy
48Latent Heat of Vaporisation Lv
- The Latent heat of vaporisation is the amount of
heat required to change 1.0kg of a substance from
the liquid to the gaseous state. - For example, when 5.00kg of water boils at 100oC,
the water must absorb - Q m L 5.00 x 22.6 x 105
- ? Q 1.13 x 107 J of energy
49Problem involving Latent Heats.
- Problem - How much energy does a refrigerator
have to remove from 1.5kg of water at 20oC to
make ice at -12oC? - Data -
- mass of water mw 1.5 kg
- specific heat of water cw 4180 J/kgoC
- Temperature change of water ?Twater 20oC
- latent heat of water/ice Lf 3.33 x 105 J/kg
- mass of ice mice 1.5 kg
- specific heat of ice ci 2100 J/kgoC
- Temperature change of the ice ?Tice 12oC
50Solution
Q mwater cwater ?Twater m Lf mice cice
?Tice Q 1.5 x 4180 x 20 1.5 x 3.33 x 105
1.5 x 2100 x 12 Q 6.6 x 105 J Therefore 660 kJ
must be removed by the refrigerator in order to
freeze ice, initially at 20oC down to -12oC.
51Amount of Heat Flow
- How much energy does it take to boil 1.0 litre of
water in a 1500W electric jug if the water is
originally at 20.0oC? - Data
- C 4180 J/kgoC
- m 1.0 kg
- ?T 100 20 80.0oC
- P 1500 W
- Find time, t
52Linear Thermal Expansion
- The change in length of a 1m length of a
substance due to a temperature change of 1oC is
called the coefficient of linear expansion (?). - The formula to help find the change in length of
a substance due to thermal expansion of solids is
- ?L Li ? ?T
53Linear Expansion Problem
- An electric company strung an aluminum wire
between two piers 200m apart on a day when the
temperature was 25oC. They strung it tight so
that it would not sag. Find the length of the
wire when the temperature fell to -25oC on a cold
winters night? What might happen? What should
have been done to prevent this from occurring?
54Volumetric Thermal Expansion
- The coefficient of volume expansion (?) is
normally associated with liquids. Liquids take
the shape of the container hence we are mainly
interested in the volume changes of liquids with
temperature. - As with solids, the change in volume of liquids
can be found using the formula - ?V Vi ? ?T
55Volume Expansion Problem
- What would be the increase in the volume of 0.20L
of acetone if it was heated form 10oC to 40oC? - Solution
- ?V Vi ? ?T
- 14.87 x 10-4 x 0.20 x (40-10)
- 89.2 x 10-4 L
- 8.9 x 10-3 L
56References
- All photographs, including those of the
Scientists are from the following sources - Microsoft Encarta.