Uploaded by Asad Khan

Copy of cie-as-physics-9702-theory-v1-znotes

advertisement
TABLE OF CONTENTS
3
CHAPTER 1
3
CHAPTER 2
4
CHAPTER 3
5
CHAPTER 4
6
CHAPTER 5
7
CHAPTER 6
Physical Quantities & Units
Measurement Techniques
Kinematics
Dynamics
Forces
Work, Energy, Power
8 Deformation of Solids
CHAPTER 7
9
CHAPTER 8
10
CHAPTER 9
11
Waves
Superposition
CHAPTER 10
Electric Fields
CIE AS-LEVEL PHYSICS//9702
,
12
CHAPTER 11
13
CHAPTER 12
14
CHAPTER 13
Current of Electricity
D.C. Circuits
Nuclear Physics
PAGE 2 OF 16
CIE AS-LEVEL PHYSICS//9702
,
1. PHYSICAL QUANTITIES AND UNITS
1.4 Scalar and Vector
ο‚· A physical quantity is made up of magnitude and unit
ο‚· Scalar: has magnitude only, cannot be –ve
e.g. speed, energy, power, work, mass, distance
ο‚· Vector: has magnitude and direction, can be –ve
e.g. displacement, acceleration, force, velocity
momentum, weight, electric field strength
1.2 Base Units
1.5 Vectors
1.1 Physical Quantities
ο‚· The following are base units:
Quantity
Basic Unit
Name
Symbol Name
Symbol
Mass
π‘˜π‘”
π‘š Kilogram
Length
𝑙 Meter
π‘š
Time
𝑑 Second
𝑠
Temperature
Kelvin
𝑇
𝐾
Electric Current
𝐼 Ampere
𝐴
ο‚· All units (not above) can be broken down to base units
ο‚· Homogeneity can be used to prove equations.
ο‚· An equation is homogenous if base units on left hand
side are the same as base units on right hand side.
ο‚· This may not work every time due to the fact that it does
not take pure numbers into account (πΈπ‘˜ formula)
1.3 Multiples and Submultiples
Multiple
1012
109
106
103
Submultiple
10-3
10-6
10-9
10-12
Prefix
Tera
Giga
Mega
Kilo
Prefix
Milli
Micro
Nano
Pico
Symbol
𝑇
𝐺
𝑀
π‘˜
Symbol
π‘š
πœ‡
𝑛
𝑝
Quantity
Accuracy
1 cm
0.1 cm
Length
0.01 cm
0.001 cm
1 cm3
Volume
0.05 cm3
Angle
0.5o
1 min
Time
0.01 sec
π‘₯-axis scale
1oC
Temperature
0.5oC
P.d.
0.01 V
0.01 A
Current
0.0001 A
Instrument
Tape
Ruler
Vernier caliper
Micrometer screw gauge
Measuring cylinder
Pipette/burette
Protractor
Clocks
Stopwatch
Time base of c.r.o
Thermometer
Thermocouple
Voltmeter
Ammeter
Galvanometer
2.1 Using a Cathode Ray Oscilloscope
1.4 Estimations
Mass of a person
Height of a person
Walking speed
Speed of a car on the motorway
Volume of a can of a drink
Density of water
Density of air
Weight of an apple
Current in a domestic appliance
e.m.f of a car battery
Hearing range
Young’s Modulus of a material
2. MEASUREMENT TECHNIQUES
70 kg
1.5 m
1 ms-1
30 ms-1
300 cm3
1000 kgm-3
1 kgm-3
1N
13 A
12 V
20 Hz to 20,000 Hz
Something × 1011
Example: A supply of peak value 5.0 V and of frequency 50
Hz is connected to a c.r.o with time-base at 10 ms per
division and Y-gain at 5.0V per division. Which trace is
obtained?
Maximum value is 5.0V ∴ eliminate A and B
1
1
𝐹 = and 𝑇 = π‘‡π‘–π‘šπ‘’π‘π‘Žπ‘ π‘’ × π·π‘–π‘£π‘–π‘ π‘–π‘œπ‘›π‘  so 𝐹 =
𝑇
π‘‡π‘–π‘šπ‘’π‘π‘Žπ‘ π‘’ × π·π‘–π‘£π‘–π‘ π‘–π‘œπ‘›π‘ 
1
1
π·π‘–π‘£π‘–π‘ π‘–π‘œπ‘›π‘  =
=
=2
𝐹 × π‘‡π‘–π‘šπ‘’π‘π‘Žπ‘ π‘’ 50 × 10 × 10−3
Trace must have period of 2 divisions and height of 1 division ∴ D
PAGE 3 OF 16
CIE AS-LEVEL PHYSICS//9702
,
2.1 Systematic and Random Errors
2.4 Micrometer Screw Gauge
ο‚· Systematic error:
o Constant error in one direction; too big or too small
o Cannot be eliminated by repeating or averaging
o If systematic error small, measurement accurate
o Accuracy: refers to degree of agreement between
result of a measurement and true value of quantity.
ο‚· Random error:
o Random fluctuations or scatter about a true value
o Can be reduced by repeating and averaging
o When random error small, measurement precise
o Precision: refers to degree of agreement of repeated
measurements of the same quantity (regardless of
whether it is correct or not)
2.1 Calculations Involving Errors
For a quantity π‘₯ = (2.0 ± 0.1)π‘šπ‘š
ο‚· Absolute uncertainty = βˆ†π‘₯ = ±0.1π‘šπ‘š
βˆ†π‘₯
= 0.05
π‘₯
βˆ†π‘₯
=
× 100%
π‘₯
2π‘₯+𝑦
3
or 𝑝 =
2π‘₯−𝑦
,
3
then βˆ†π‘ =
2βˆ†π‘₯+βˆ†π‘¦
3
o When values multiplied or divided, add % errors
o When values are powered (e.g. squared), multiply
percentage error with power
If π‘Ÿ = 2π‘₯𝑦 3 or π‘Ÿ =
2π‘₯
,
𝑦3
then
βˆ†π‘Ÿ
π‘Ÿ
=
βˆ†π‘₯
π‘₯
+
Measures objects up to 0.1mm
ο‚· Place object on rule
ο‚· Push slide scale to edge of object.
ο‚· The sliding scale is 0.9mm long & is
divided into 10 equal divisions.
ο‚· Check which line division on sliding scale
matches with a line division on rule
ο‚· Subtract the value from the sliding scale
(0.09 × π·π‘–π‘£π‘–π‘ π‘–π‘œπ‘›π‘ ) by the value from the rule.
3.1 Linear Motion
= 5%
ο‚· Combining errors:
o When values added or subtracted, add absolute error
If 𝑝 =
2.5 Vernier Scale
3. KINEMATICS
ο‚· Fractional uncertainty =
ο‚· Percentage uncertainty
ο‚· Measures objects up to 0.01mm
ο‚· Place object between anvil & spindle
ο‚· Rotate thimble until object firmly held by jaws
ο‚· Add together value from main scale and rotating scale
3βˆ†π‘¦
𝑦
ο‚· Distance: total length moved irrespective of direction
ο‚· Displacement: distance in a certain direction
ο‚· Speed: distance traveled per unit time, no direction
ο‚· Velocity: the rate of change of displacement
ο‚· Acceleration: the rate of change of velocity
ο‚· Displacement-time graph:
o Gradient = velocity
2.3 Treatment of Significant Figures
ο‚· Actual error: recorded to only 1 significant figure
ο‚· Number of decimal places for a calculated quantity is
equal to number of decimal places in actual error.
ο‚· During a practical, when calculating using a measured
quantity, give answers to the same significant figure as
the measurement or one less
3.2 Non-linear Motion
ο‚· Velocity-time graph:
o Gradient = acceleration
o Area under graph = change in displacement
PAGE 4 OF 16
CIE AS-LEVEL PHYSICS//9702
,
ο‚· Uniform acceleration and straight line motion equations:
𝑣 = 𝑒 + π‘Žπ‘‘
𝑠 = 𝑒𝑑 +
1
π‘Žπ‘‘ 2
2
1
𝑠 = 2 (𝑒 + 𝑣)𝑑
𝑠 = 𝑣𝑑 −
1
π‘Žπ‘‘ 2
2
3.5 Projectile motion
ο‚· Projectile motion: uniform velocity in one direction and
constant acceleration in perpendicular direction
𝑣 2 = 𝑒2 + 2π‘Žπ‘ 
ο‚· Acceleration of free fall = 9.81ms-2
3.3 Determining Acceleration of Free Fall
ο‚· A steel ball is held on an electromagnet.
ο‚· When electromagnet
switched off, ball
interrupts a beam
of light and a timer
started.
ο‚· As ball falls, it
interrupts a second
beam of light &
timer stopped
ο‚· Vertical distance 𝒉 is
plotted against π’•πŸ
1
𝑠 = 𝑒𝑑 + π‘Žπ‘‘ 2 and 𝑒 = 0
β„Ž
𝑑2
1
1
2
2
𝑠 = π‘Žπ‘‘ 2 i.e. β„Ž = π‘Žπ‘‘ 2
2
πΊπ‘Ÿπ‘Žπ‘‘π‘–π‘’π‘›π‘‘ =
ο‚· Horizontal motion = constant velocity (speed at which
projectile is thrown)
ο‚· Vertical motion = constant acceleration (cause by weight
of object, constant free fall acceleration)
ο‚· Curved path – parabolic (𝑦 ∝ π‘₯ 2 )
1
= 𝑔
2
𝐴𝑐𝑐𝑒𝑙. = 2 × πΊπ‘Ÿπ‘Žπ‘‘π‘–π‘’π‘›π‘‘
displacement
ο‚· Continues to curve as it
accelerate
ο‚· Graph levels off as it
reaches terminal
velocity
velocity
ο‚· Continues to
accelerate constantly
ο‚· Graph curves as it
decelerates and levels
off to terminal velocity
acceleration
3.4 Motion of Bodies Free Falling
ο‚· Straight line
ο‚· Graph curves down to
zero because resultant
force equals zero
Without air
Resistance
With air
Resistance
Component of Velocity
Horizontal
Vertical
Increases at a
Constant
constant rate
Decreases to zero
Increases to a
constant value
3.6 Motion of a Skydiver
4. DYNAMICS
4.1 Newton’s Laws of Motion
ο‚· First law: if a body is at rest it remains at rest or if it is in
motion it moves with a uniform velocity until it is acted
on by resultant force or torque
PAGE 5 OF 16
CIE AS-LEVEL PHYSICS//9702
,
ο‚· Second law: the rate of change of momentum of a body
is proportional to the resultant force and occurs in the
direction of force; 𝐹 = π‘šπ‘Ž
ο‚· Third law: if a body A exerts a force on a body B, then
body B exerts an equal but opposite force on body A,
forming an action-reaction pair
4.2 Mass and Weight
Mass
Weight
ο‚· Measured in kilograms
ο‚· Measured in Newtons
ο‚· Scalar quantity
ο‚· Vector quantity
ο‚· Not constant
ο‚· Constant throughout
the universe
ο‚· π‘Š = π‘šπ‘”
ο‚· Mass: is a measure of the amount of matter in a body, &
is the property of a body which resists change in motion.
ο‚· Weight: is the force of gravitational attraction (exerted
by the Earth) on a body.
4.5 Inelastic Collisions
relative speed of approach > relative speed of separation
o Total momentum is conserved
ο‚· Perfectly inelastic collision: only momentum is
conserved, and the particles stick together after collision
(i.e. move with the same velocity)
ο‚· In inelastic collisions, total energy is conserved but πΈπ‘˜
may be converted into other forms of energy e.g. heat
4.6 Collisions in Two Dimensions
4.3 Momentum
ο‚· Linear momentum: product of mass and velocity
𝑝 = π‘šπ‘£
ο‚· Force: rate of change of momentum
π‘šπ‘£ − π‘šπ‘’
𝐹 =
𝑑
ο‚· Principle of conservation of linear momentum: when
bodies in a system interact, total momentum remains
constant provided no external force acts on the system.
π‘šπ΄ 𝑒𝐴 + π‘šπ΅ 𝑒𝐡 = π‘šπ΄ 𝑣𝐴 + π‘šπ΅ 𝑣𝐡
4.4 Elastic Collisions
ο‚· Total momentum conserved
ο‚· Total kinetic energy is conserved
Example: Two identical spheres collide elastically. Initially,
X is moving with speed v and Y is stationary. What
happens after the collision?
ο‚· Change in momentum (impulse) affecting each sphere
acts along line of impact
ο‚· Law of conservation of momentum applies along line of
impact
ο‚· Components of velocities of spheres along plane of
impact unchanged
5. FORCES, DENSITY, PRESSURE
ο‚· Force: rate of change of momentum
ο‚· Density: mass per unit of volume of a substance
ο‚· Pressure: force per unit area
ο‚· Finding resultant (nose to tail):
o By accurate scale drawing
o Using trigonometry
X stops and Y moves with speed v
relative velocity
relative velocity
(
)= −(
)
before collision
after collision
𝑒𝐴 − 𝑒𝐡 = 𝑣𝐡 − 𝑣𝐴
ο‚· Forces on masses in gravitational fields: a region of
space in which a mass experiences an (attractive) force
due to the presence of another mass.
PAGE 6 OF 16
CIE AS-LEVEL PHYSICS//9702
,
ο‚· Forces on charge in electric fields: a region of space
where a charge experiences an (attractive or repulsive)
force due to the presence of another charge.
ο‚· Upthrust: an upward force exerted by a fluid on a
submerged or floating object
ο‚· Origin of Upthrust:
Pressure on Bottom Surface > Pressure on Top Surface
∴ Force on Bottom Surface > Force on Top Surface
⇒ Resultant force upwards
ο‚· Frictional force: force that arises when two surfaces rub
o Always opposes relative or attempted motion
o Always acts along a surface
o Value varies up to a maximum value
ο‚· Viscous forces:
o A force that opposes the motion of an object in a fluid;
o Only exists when there is motion.
o Its magnitude increases with the speed of the object
ο‚· Centre of gravity: point through which the entire weight
of the object may be considered to act
ο‚· Couple: a pair of forces which produce rotation only
ο‚· To form a couple:
o Equal in magnitude
o Parallel but in opposite directions
o Separated by a distance 𝑑
ο‚· Moment of a Force: product of the force and the
perpendicular distance of its line of action to the pivot
π‘€π‘œπ‘šπ‘’π‘›π‘‘ = πΉπ‘œπ‘Ÿπ‘π‘’ × ⊥ π·π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’ π‘“π‘Ÿπ‘œπ‘š π‘ƒπ‘–π‘£π‘œπ‘‘
ο‚· Torque of a Couple: the product of one of the forces of
the couple and the perpendicular distance between the
lines of action of the forces.
π‘‡π‘œπ‘Ÿπ‘žπ‘’π‘’ = πΉπ‘œπ‘Ÿπ‘π‘’ × ⊥ π·π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’ 𝑏𝑒𝑑𝑀𝑒𝑒𝑛 πΉπ‘œπ‘Ÿπ‘π‘’π‘ 
ο‚· Conditions for Equilibrium:
o Resultant force acting on it in any direction equals zero
o Resultant torque about any point is zero.
ο‚· Principle of Moments: for a body to be in equilibrium,
the sum of all the anticlockwise moments about any
point must be equal to the sum of all the clockwise
moments about that same point.
5.1 Pressure in Fluids
ο‚· Fluids refer to both liquids and gases
ο‚· Particles are free to move and have 𝐸𝐾 ∴ they collide
with each other and the container. This exerts a small
force over a small area causing pressure to form.
5.2 Derivation of Pressure in Fluids
Volume of water = 𝐴 × β„Ž
Mass of Water = density × volume = 𝜌 × π΄ × β„Ž
Weight of Water = mass × π‘” = 𝜌 × π΄ × β„Ž × π‘”
Pressure =
Force
𝜌×𝐴×β„Ž×𝑔
=
Area
𝐴
Pressure = πœŒπ‘”β„Ž
6. WORK, ENERGY, POWER
ο‚· Law of conservation of energy: the total energy of an
isolated system cannot change—it is conserved over
time. Energy can be neither created nor destroyed, but
can change form e.g. from g.p.e to k.e
6.1 Work Done
ο‚· Work done by a force: the product of the force and
displacement in the direction of the force
π‘Š = 𝐹𝑠
ο‚· Work done by an expanding gas: the product of the
force and the change in volume of gas
π‘Š = 𝑝. 𝛿𝑉
o Condition for formula: temperature of gas is constant
o The change in distance of the piston, 𝛿π‘₯, is very small
therefore it is assumed that 𝑝 remains constant
6.2 Deriving Kinetic Energy
π‘Š = 𝐹𝑠
&
𝐹 = π‘šπ‘Ž
∴ π‘Š = π‘šπ‘Ž. 𝑠
2
2
𝑣 = 𝑒 + 2π‘Žπ‘  ⟹ π‘Žπ‘  = 1⁄2 (𝑣 2 − 𝑒2 )
∴ π‘Š = π‘š. 1⁄2 (𝑣 2 − 𝑒2 )
𝑒=0
∴ π‘Š = 1⁄2 π‘šπ‘£ 2
6.3 g.p.e and e.p
ο‚· Gravitational Potential Energy: arises in a system of
masses where there are attractive gravitational forces
between them. The g.p.e of an object is the energy it
possesses by virtue of its position in a gravitational field.
ο‚· Elastic potential energy: this arises in a system of atoms
where there are either attractive or repulsive shortrange inter-atomic forces between them.
ο‚· Electric potential energy: arises in a system of charges
where there are either attractive or repulsive electric
forces between them.
PAGE 7 OF 16
CIE AS-LEVEL PHYSICS//9702
,
6.4 Deriving Gravitational Potential Energy
π‘Š = 𝐹𝑠
&
𝑀 = π‘šπ‘” = 𝐹
∴ π‘Š = π‘šπ‘”. 𝑠
𝑠 in direction of force = β„Ž above ground
∴ π‘Š = π‘šπ‘”β„Ž
6.5 Internal Energy
ο‚· Internal energy: sum of the K.E. of molecules due to its
random motion & the P.E. of the molecules due to the
intermolecular forces.
ο‚· Gases: π‘˜. 𝑒. > 𝑝. 𝑒.
o Molecules far apart and in continuous motion = π‘˜. 𝑒
o Weak intermolecular forces so very little 𝑝. 𝑒.
ο‚· Liquids: π‘˜. 𝑒. ≈ 𝑝. 𝑒.
o Molecules able to slide to past each other = π‘˜. 𝑒.
o Intermolecular force present and keep shape = 𝑝. 𝑒.
ο‚· Solids: π‘˜. 𝑒. < 𝑝. 𝑒.
o Molecules can only vibrate ∴ π‘˜. 𝑒. very little
o Strong intermolecular forces ∴ high 𝑝. 𝑒.
ο‚· According to Hooke’s law, the extension produced is
proportional to the applied force (due to the load) as
long as the elastic limit is not exceeded.
𝐹 = π‘˜π‘’
Where π‘˜ is the spring constant; force per unit extension
ο‚· Calculating effective spring constants:
Series
Parallel
1
1
1
= +
π‘˜πΈ = π‘˜1 + π‘˜2
π‘˜πΈ π‘˜1 π‘˜2
7.3 Determining Young’s Modulus
Measure diameter of wire using micrometer screw gauge
Set up arrangement as diagram:
Attach weights to end of wire and measure extension
6.6 Power and a Derivation
ο‚· Power: work done per unit of time
π‘ƒπ‘œπ‘€π‘’π‘Ÿ =
π‘Šπ‘œπ‘Ÿπ‘˜ π·π‘œπ‘›π‘’
π‘‡π‘–π‘šπ‘’ π‘‡π‘Žπ‘˜π‘’π‘›
Calculate Young’s Modulus using formula
ο‚· Deriving it to form 𝑃 = 𝑓𝑣
𝑃 = π‘Š. 𝑑⁄𝑇
&
π‘Š. 𝑑. = 𝐹𝑠
∴ 𝑃 = 𝐹𝑠⁄𝑇 = 𝐹(𝑠⁄𝑑) &
𝑣 = 𝑠⁄𝑑
7.4 Stress, Strain and Young’s Modulus
∴ 𝑃 = 𝐹𝑣
ο‚· Efficiency: ratio of (useful) output energy of a machine
to the input energy
π‘ˆπ‘ π‘’π‘“π‘’π‘™ πΈπ‘›π‘’π‘Ÿπ‘”π‘¦ 𝑂𝑒𝑝𝑒𝑑
𝐸𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑐𝑦 =
× 100
π‘‡π‘œπ‘‘π‘Žπ‘™ πΈπ‘›π‘’π‘Ÿπ‘”π‘¦ 𝐼𝑛𝑝𝑒𝑑
7. DEFORMATION OF SOLIDS
ο‚· Stress: force applied per unit cross-sectional
area
𝐹
𝜎 = 𝐴 in Nm-2 or Pascals
ο‚· Strain: fractional increase in original length of wire
𝑒
πœ€=
no units
𝑙
ο‚· Young’s Modulus: ratio of stress to strain
𝜎
𝐸 = πœ€ in Nm-2 or Pascals
ο‚· Stress-Strain Graph:
7.1 Compressive and Tensile Forces
ο‚· Deformation is caused by a force
Tensile
Compressive
a pair of forces that
act away from each other,
act towards each other,
object stretched out
object squashed
7.2 Hooke’s Law
ο‚· A spring produces an extension when a load is attached
Gradient = Young’s modulus
ο‚· Elastic deformation: when deforming forces removed,
spring returns back to original length
ο‚· Plastic deformation: when deforming forces removed,
spring does not return back to original length
PAGE 8 OF 16
CIE AS-LEVEL PHYSICS//9702
,
ο‚· Strain energy: the potential energy stored in or work
done by an object when it is deformed elastically
ο‚· Strain energy = area under force-extension graph
π‘Š = 1⁄2 π‘˜βˆ†πΏ2
𝐼𝑛𝑑𝑒𝑛𝑠𝑖𝑑𝑦 ∝ (π΄π‘šπ‘π‘™π‘–π‘‘π‘’π‘‘π‘’)2
8.4 Transverse and Longitudinal
Transverse Waves
Longitudinal Waves
8. WAVES
ο‚· Displacement: distance of a point from its undisturbed
position
ο‚· Amplitude: maximum displacement of particle from
undisturbed position
ο‚· Period: time taken for one complete oscillation
ο‚· Frequency: number of oscillations per unit time
1
𝑓=
𝑇
ο‚· Wavelength: distance from any point on the wave to the
next exactly similar point (e.g. crest to crest)
ο‚· Wave speed: speed at which the waveform travels in
the direction of the propagation of the wave
ο‚· Progressive waves transfer energy from one position to
another
ο‚· Oscillation of wave
ο‚· Oscillations of wave
particles perpendicular to particle parallel to
direction of propagation
direction of propagation
ο‚· Polarization can occur
ο‚· Polarization cannot occur
ο‚· E.g. light waves
ο‚· E.g. sound waves
ο‚· Polarization: vibration of particles is confined in one
direction in the plane normal to direction of propagation
8.1 Deducing Wave Equation
8.5 The Doppler Effect
π·π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’
π‘‡π‘–π‘šπ‘’
ο‚· Distance of 1 wavelength is πœ† and time taken for this is 𝑇
πœ†
1
∴ 𝑣 = = πœ†( )
𝑇
𝑇
1
𝑓=
so 𝑣 = π‘“πœ†
𝑆𝑝𝑒𝑒𝑑 =
ο‚· Arises when source of waves moves relative to observer
ο‚· Can occur in all types of waves, including sound & light
ο‚· Source stationary relative to Observer:
𝑇
8.2 Phase Difference
ο‚· Source moving towards Observer:
ο‚· Phase difference between two waves is the difference in
terms of fraction of a cycle or in terms of angles
A
B
ο‚· Source moving away from Observer:
Wave A leads wave B by πœƒ or Wave B lags wave A by πœƒ
8.3 Intensity
ο‚· Rate of energy transmitted per unit area perpendicular
to direction of wave propagation.
π‘ƒπ‘œπ‘€π‘’π‘Ÿ
𝐼𝑛𝑑𝑒𝑛𝑠𝑖𝑑𝑦 =
πΆπ‘Ÿπ‘œπ‘ π‘  π‘†π‘’π‘π‘‘π‘–π‘œπ‘›π‘Žπ‘™ π΄π‘Ÿπ‘’π‘Ž
ο‚· Change in wavelength leads to change in frequency
ο‚· Observed frequency (𝑓0) is different from actual
frequency (𝑓𝑠 ); related by equation:
𝑓𝑠 𝑣
𝑓0 =
𝑣 ± 𝑣𝑠
where 𝑣 is speed of wave & 𝑣𝑠 is speed of source relative
to observer
PAGE 9 OF 16
CIE AS-LEVEL PHYSICS//9702
,
8.6 Electromagnetic Waves
9.4 Formation of Stationary waves
wavelength decreases and frequency increases οƒ 
πœ†=
All electromagnetic waves:
ο‚· All travel at the speed of light: 3 × 108m/s
ο‚· Travel in free space (don’t need medium)
ο‚· Can transfer energy
ο‚· Are transverse waves
ο‚· A stationary wave is formed when two progressive
waves of the same frequency, amplitude and speed,
travelling in opposite directions are superposed.
ο‚· Node: region of destructive superposition where waves
always meet out of phase by πœ‹, ∴ displacement = zero
ο‚· Antinode: region of constructive superposition where
waves meet in phase ∴ particle vibrate with max amp
9. SUPERPOSITION
9.1 Principle of Superposition
ο‚· When two or more waves of the same type meet at a
point, the resultant displacement is the algebraic sum of
the individual displacements
9.2 Interference and Coherence
ο‚· Neighboring nodes & antinodes separated by 1⁄2 πœ†
ο‚· Between 2 adjacent nodes, particles move in phase and
they are out of phase with the next two nodes by πœ‹
Stationary wave at different times:
ο‚· Interference: the formation of points of cancellation and
reinforcement where 2 coherent waves pass each other
ο‚· Coherence: waves having a constant phase difference
Constructive
Destructive
πœ†
πœ†
Phase difference = even 2
Phase difference = odd 2
Path difference = even
Path difference = odd
πœ†
2
πœ†
2
9.3 Two-Source Interference
9.5 Stationary Wave Experiments
ο‚· Conditions for Two-Source Interference:
o Meet at a point
o Must be of the same type
o Must have the same plane of polarization
ο‚· Demonstrating Two-Source Interference:
Water
Ripple generators in a tank
Light
Double slit interference
Microwaves
Two microwave emitters
Stretched String:
ο‚· String either attached to wall or attached to weight
ο‚· Stationary waves will be produced by the direct and
reflected waves in the string.
PAGE 10 OF 16
CIE AS-LEVEL PHYSICS//9702
,
Microwaves:
ο‚· A microwave emitter placed a distance away from a
metal plate that reflects the emitted wave.
ο‚· By moving a detector along the path of the wave, the
nodes and antinodes could be detected.
9.8 Double-Slit Interference
πœ†=
Air Columns:
ο‚· A tuning fork held at the
mouth of an open tube
projects a sound wave into
the column of air in the tube.
ο‚· The length can be changed by
varying the water level.
ο‚· At certain lengths tube, the air
column resonates
ο‚· This is due to the formation of
stationary waves by the incident
and reflected sound waves at the water surface.
ο‚· Node always formed at surface of water
π‘Žπ‘₯
𝐷
Where π‘Ž = split separation
𝐷 = distance from slit to screen
π‘₯ = fringe width
9.9 Diffraction Grating
9.6 Stationary and Progressive Waves
Stationary Waves
Stores energy
Have nodes & antinodes
Amplitude increases from
node to antinode
Phase change of πœ‹ at node
Progressive Waves
Transmits energy
No nodes & antinodes
Amplitude constant along
length of the wave
No phase change
9.7 Diffraction
ο‚· Diffraction: the spreading of waves as they pass through
a narrow slit or near an obstacle
ο‚· For diffraction to occur, the size of the gap should be
equal to the wavelength of the wave.
𝑑 sin πœƒ = π‘›πœ†
Where 𝑑 = distance between successive slits
= reciprocal of number of lines per meter
πœƒ = angle from horizontal equilibrium
𝑛 = order number
πœ† = wavelength
Comparing to double-slit to diffraction grating:
ο‚· Maxima are sharper compared to fringes
ο‚· Maxima very bright; more slits, more light through
10. ELECTRIC FIELDS
10.1 Concept of Electric Field
ο‚· Can be described as a field of force; it can move charged
particles by exerting a force on them
ο‚· Positive charge moves in direction of the electric field:
they gain EK and lose EP
PAGE 11 OF 16
CIE AS-LEVEL PHYSICS//9702
,
ο‚· Negative charge moves in opposite direction of the
electric field: they lose EK and gain EP
11.1 Current-Carrying Conductors
10.2 Diagrammatic Representation
ο‚· Parallel plates:
ο‚· Points:
10.3 Electric Field Strength
ο‚· Force per unit positive charge acting at a point; a vector
ο‚· Units: 𝑁𝐢 −1 or π‘‰π‘š−1
𝐸=
𝐹
π‘ž
𝐸=
𝑉
𝑑
ο‚· 𝐸 is the electric field strength
ο‚· 𝐹 is the force
ο‚· 𝑉 is potential difference
ο‚· π‘ž is the charge
ο‚· 𝑑 is distance between
plates
ο‚· The higher the voltage, the stronger the electric field
ο‚· The greater the distance between the plates, the weaker
the electric field
ο‚· Electrons move in a certain direction when p.d. is
applied across a conductor causing current
ο‚· Deriving a formula for current:
𝑄
𝐼=
𝑑
𝐿
π‘£π‘œπ‘™. π‘œπ‘“ π‘π‘œπ‘›π‘‘π‘Žπ‘–π‘›π‘’π‘Ÿ = 𝐿𝐴
𝑑=
π‘›π‘œ. π‘œπ‘“ π‘“π‘Ÿπ‘’π‘’ π‘’π‘™π‘’π‘π‘‘π‘Ÿπ‘œπ‘›π‘  = 𝑛𝐿𝐴
𝑣
π‘‘π‘œπ‘‘π‘Žπ‘™ π‘β„Žπ‘Žπ‘Ÿπ‘”π‘’ = 𝑄 = π‘›πΏπ΄π‘ž
π‘›πΏπ΄π‘ž
∴𝐼=
𝐿 ⁄𝑣
𝐼 = π΄π‘›π‘£π‘ž
Where 𝐿 = length of conductor
𝐴 = cross-sectional area of conductor
𝑛 = no. free electrons per unit volume
π‘ž = charge on 1 electron
𝑣 = average electron drift velocity
11.2 Current-P.D. Relationships
Metallic Conductor
Filament Lamp
11. CURRENT OF ELECTRICITY
ο‚· Electric current: flow of charged particles
ο‚· Charge at a point: product of the current at that point
and the time for which the current flows,
𝑄 = 𝐼𝑑
ο‚· Coulomb: charge flowing per second pass a point at
which the current is one ampere
ο‚· Charge is quantized: values of charge are not continuous
they are discrete
ο‚· All charges are multiples of charge of 1e: 1.6x10-19C
ο‚· Potential Difference: two points are a potential
difference of 1V if the work required to move 1C of
charge between them is 1 joule
ο‚· Volt: joule per coulomb
π‘Š = 𝑉𝑄
𝑃 = 𝑉𝐼
𝑃 = 𝐼2 𝑅
𝑃=
𝑉2
𝑅
Ohmic conductor
V/I ratio constant
Thermistor
Non-ohmic conductor
Volt ↑, Temp. ↑, Released
e- ↑, Resistance ↓
PAGE 12 OF 16
Non-ohmic conductor
Volt ↑, Temp. ↑, Vibration
of ions ↑, Collision of ions
with e- ↑, Resistance ↑
Semi-Conductor Diode
Non-ohmic conductor
Low resistance in one
direction & infinite
resistance in opposite
CIE AS-LEVEL PHYSICS//9702
,
ο‚· Ohm’s law: the current in a component is proportional
to the potential difference across it provided physical
conditions (e.g. temp) stay constant.
11.3 Resistance
ο‚· Resistance: ratio of potential difference to the current
ο‚· Ohm: volt per ampere
𝑉 = 𝐼𝑅
ο‚· Resistivity: the resistance of a material of unit crosssectional area and unit length
𝜌𝐿
𝑅=
𝐴
12.4 Kirchhoff’s 2nd Law
Sum of e.m.f.s in a closed circuit
IS EQUAL TO
Sum of potential differences
nd
ο‚· Kirchhoff’s 2 law is another statement of the law of
conservation of energy
12.5 Applying Kirchhoff’s Laws
Example: Calculate the current in each of the resistors
12. D.C. CIRCUITS
ο‚· Electromotive Force: the energy converted into
electrical energy when 1C of charge passes through the
power source
12.1 p.d. and e.m.f
Potential Difference
Electromotive Force
work done per unit charge
energy transformed from
energy transformed from
electrical to other forms
other forms to electrical
per unit charge
12.2 Internal Resistance
Internal Resistance: resistance to current flow within the
power source; reduces p.d. when delivering current
𝑉 = πΌπ‘Ÿ − 𝐸
Using Kirchhoff’s 1st Law:
𝐼3 = 𝐼1 + 𝐼2
nd
Using Kirchhoff’s 2 Law on loop 𝑨𝑩𝑬𝑭:
3 = 30𝐼3 + 10𝐼1
nd
Using Kirchhoff’s 2 Law on loop π‘ͺ𝑩𝑬𝑫:
2 = 30𝐼3
Using Kirchhoff’s 2nd Law on loop 𝑨π‘ͺ𝑫𝑭:
3 − 2 = 10𝐼1
Solve simulataneous equations:
𝐼1 = 0.100
𝐼2 = −0.033 𝐼3 = 0.067
12.6 Deriving Effective Resistance in Series
Voltage across resistor:
Voltage lost to internal resistance:
Thus e.m.f.:
𝐸 = 𝐼(𝑅 + π‘Ÿ)
12.3 Kirchhoff’s
1st
𝑉 = 𝐼𝑅
𝑉 = πΌπ‘Ÿ
𝐸 = 𝐼𝑅 + πΌπ‘Ÿ
Law
From Kirchhoff’s 2nd Law:
𝐸 = ∑𝐼𝑅
𝐼𝑅 = 𝐼𝑅1 + 𝐼𝑅2
Current constant therefore cancel:
𝑅 = 𝑅1 + 𝑅2
12.7 Deriving Effective Resistance in Parallel
From Kirchhoff’s 1st Law:
𝐼 = ∑𝐼
𝐼 = 𝐼1 + 𝐼2
IS EQUAL TO
𝑉
𝑉
𝑉
=
+
Sum of currents out of junction.
𝑅 𝑅1 𝑅2
ο‚· Kirchhoff’s 1st law is another statement of the law of
Voltage constant therefore cancel:
conservation of charge
1
1
1
=
+
𝑅 𝑅1 𝑅2
PAGE 13 OF 16
Sum of currents into a junction
CIE AS-LEVEL PHYSICS//9702
,
13. NUCLEAR PHYSICS
12.8 Potential Divider
ο‚· A potential divider divides the voltage into smaller parts.
13.1 Geiger-Marsden 𝜢-scattering
ο‚· Experiment: a beam of 𝛼-particles is fired at thin gold foil
π‘‰π‘œπ‘’π‘‘
𝑅2
=
𝑉𝑖𝑛
π‘…π‘‡π‘œπ‘‘π‘Žπ‘™
ο‚· Usage of a thermistor at R1:
o Resistance decreases with increasing temperature.
o Can be used in potential divider circuits to monitor
and control temperatures.
ο‚· Usage of an LDR at R1:
o Resistance decreases with increasing light intensity.
o Can be used in potential divider circuits to monitor
light intensity.
12.9 Potentiometers
ο‚· A potentiometer is a continuously variable potential
divider used to compare potential differences
ο‚· Potential difference along the wire is proportional to the
length of the wire
ο‚· Can be used to determine the unknown e.m.f. of a cell
ο‚· This can be done by moving the sliding contact along the
wire until it finds the null point that the galvanometer
shows a zero reading; the potentiometer is balanced
Example: E1 is 10 V, distance XY is equal to 1m. The
potentiometer is balanced at point T which is 0.4m from X.
Calculate E2
ο‚· Results of the experiment:
o Most particles pass straight through
o Some are scattered appreciably
o Very few – 1 in 8,000 – suffered deflections > 90o
ο‚· Conclusion:
o All mass and charge concentrated in the center of
atom ∴ nucleus is small and very dense
o Nucleus is positively charged as 𝛼-particles are
repelled/deflected
13.2 The Nuclear Atom
ο‚· Nucleon number: total number of protons and neutrons
ο‚· Proton/atomic number: total number of protons
ο‚· Isotope: atoms of the same element with a different
number of neutrons but the same number of protons
13.3 Nuclear Processes
ο‚· During a nuclear process, nucleon number, proton
number and mass-energy are conserved
Radioactive process are random and spontaneous
ο‚· Random: impossible to predict and each nucleus has the
same probability of decaying per unit time
ο‚· Spontaneous: not affected by external factors such as
the presence of other nuclei, temperature and pressure
ο‚· Evidence on a graph:
o Random; graph will have fluctuations in count rate
o Spontaneous; graph has same shape even at different
temperatures, pressure etc.
𝐸1 𝐿1
=
𝐸2 𝐿2
10
1
=
𝐸2 0.4
𝐸2 = 4𝑉
PAGE 14 OF 16
CIE AS-LEVEL PHYSICS//9702
,
ο‚· Quark Models:
13.4 Radiations
𝜢particle
Identity
Symbol
Charge
Relative
Mass
Speed
Helium
nucleus
4
2𝐻𝑒
𝜷-particle
𝜷−
Neutron
2 Up & 1 Down
2 2 1
+ + − = +1
3 3 3
1 Up & 2 Down
2 1 1
+ − − =0
3 3 3
Electromagnetic
𝛾
−1
+1
0
1
0
1840
Fast
V of Light
(3 × 108 ms-1)
(108 ms-1)
Varying
Few mm of
Few cm of
aluminum
lead
4
Slow
(106 ms-1)
Discrete
Energy
Stopped
Paper
by
Ionizing
High
Low
power
Effect of Deflected
Deflected greater
Magnetic
slightly
Effect of Attracted
Attracted to
Electric
to -ve
+ve
-ve
Very Low
ο‚· 𝜢-decay: loses a helium proton
ο‚· 𝜷− -decay: neutron turns into a proton and an electron &
electron antineutrino are emitted
ο‚· 𝜷+ -decay: proton turns into a neutron and a positron &
electron neutrino are emitted
ο‚· 𝜸-decay: a nucleus changes from a higher energy state
to a lower energy state through the emission of
electromagnetic radiation (photons)
13.6 Fundamental Particles
ο‚· Fundamental Particle: a particle that cannot be split up
into anything smaller
ο‚· Electron is a fundamental particle but protons and
neutrons are not
ο‚· Protons and neutrons are made up of different
combinations of smaller particles called quarks
ο‚· Table of Quarks:
Symbol
𝑒
𝑑
𝑠
ο‚· All particles have their corresponding antiparticle
ο‚· A particle and its antiparticle are essentially the same
except for their charge
ο‚· Table of Antiquarks:
Undeflected
13.5 Types of Decays
Quark
Up
Down
Strange
Proton
𝜷+
Fast-moving
electron/positron
0
0
−1𝑒
+1𝑒
+2
𝜸-ray
Antiquark
Symbol
Charge
Anti-Up
𝑒̅
−2/3
Anti-Down
+1/3
𝑑̅
Anti-Strange
𝑠̅
−1/3
ο‚· These antiquarks combine to similarly form respective
antiprotons and antineutrons
13.7 Quark Nature of 𝜷-decay
ο‚· Conventional model of 𝛽-decay:
o 𝜷−-decay:
𝑛 → 𝑝 + 𝛽 − + 𝑣̅
+
o 𝜷 -decay:
𝑝 → 𝑛 + 𝛽+ + 𝑣
ο‚· Quark model of 𝛽-decay:
o 𝜷−-decay:
o 𝜷+-decay:
Charge
+2/3
−1/3
+1/3
ο‚· Quarks undergo change to another quark in what is
called a ‘weak interaction’
PAGE 15 OF 16
CIE AS-LEVEL PHYSICS//9702
,
13.8 Particle Families
Electron
Positron
Electron Family
Electron Neutrino
Electron
Antineutrino
Leptons
ο‚· There are other families under Leptons
ο‚· Leptons are a part of elementary particles
Baryons
Hadrons
Protons
Neutrons
ο‚· There are other families under Hadrons too
ο‚· Hadrons are a part of composite particles
PAGE 16 OF 16
Download