Measurement
Base quantities and their units;
mass (kg), length (m), time (s), current (A), temperature (K), amount of
substance (mol):
Base
Quantities
|
SI
Units
|
|
Name
|
Symbol
|
|
Length
|
metre
|
M
|
Mass
|
kilogram
|
kg
|
Time
|
second
|
S
|
Amount of substance
|
mole
|
mol
|
Temperature
|
Kelvin
|
K
|
Current
|
ampere
|
A
|
Luminous intensity
|
candela
|
cd
|
Derived units as products or
quotients of the base units:
Derived
|
Quantities
Equation
|
Derived
Units
|
Area (A)
|
A = L2
|
m2
|
Volume (V)
|
V = L3
|
m3
|
Density (ρ)
|
ρ = m / V
|
kg m-3
|
Velocity (v)
|
v = L / t
|
ms-1
|
Acceleration (a)
|
a = Δv / t
|
ms-1 / s = ms-2
|
Momentum (p)
|
p = m x v
|
(kg)(ms-1) = kg m s-1
|
Derived
Quantities
|
Equation
|
Derived
Unit
|
Derived
Units
|
|
Special
Name
|
Symbol
|
|||
Force (F)
|
F = Δp / t
|
Newton
|
N
|
[(kg m s-1) / s = kg m
s-2
|
Pressure (p)
|
p = F / A
|
Pascal
|
Pa
|
(kg m s-2) / m2
= kg m-1 s-2
|
Energy (E)
|
E = F x d
|
joule
|
J
|
(kg m s-2)(m) = kg m2
s-2
|
Power (P)
|
P = E / t
|
watt
|
W
|
(kg m2 s-2)
/ s = kg m2 s-3
|
Frequency (f)
|
f = 1 / t
|
hertz
|
Hz
|
1 / s = s-1
|
Charge (Q)
|
Q = I x t
|
coulomb
|
C
|
A s
|
Potential Difference (V)
|
V = E / Q
|
volt
|
V
|
(kg m2 s-2)
/ A s = kg m2 s-3 A-1
|
Resistance (R)
|
R = V / I
|
ohm
|
Ω
|
(kg m2 s-3 A-1)
/ A = kg m2 s-3 A-2
|
Prefixes and their symbols to
indicate decimal sub-multiples or multiples of both base and derived units:
Multiplying
Factor
|
Prefix
|
Symbol
|
10-12
|
pico
|
P
|
10-9
|
nano
|
N
|
10-6
|
micro
|
Μ
|
10-3
|
milli
|
M
|
10-2
|
centi
|
C
|
10-1
|
decid
|
D
|
103
|
kilo
|
K
|
106
|
mega
|
M
|
109
|
giga
|
G
|
1012
|
tera
|
T
|
Estimates
of physical quantities:
When making an estimate, it is only
reasonable to give the figure to 1 or at most 2 significant figures since an
estimate is not very precise.
Physical
Quantity
|
Reasonable
Estimate
|
Mass of 3 cans (330 ml) of Coke
|
1 kg
|
Mass of a medium-sized car
|
1000 kg
|
Length of a football field
|
100 m
|
Reaction time of a young
man
|
0.2 s
|
- Occasionally, students are asked to estimate the area under a graph. The usual method of counting squares within the enclosed area is used. (eg. Topic 3 (Dynamics), N94P2Q1c)
- Often, when making an estimate, a formula and a simple calculation may be involved.
EXAMPLE
Estimate the average running speed
of a typical 17-year-old‟s 2.4-km run.
velocity = distance / time = 2400 /
(12.5 x 60) = 3.2 ≈3 ms-1
Which estimate is realistic?
|
Option
|
Explanation
|
|
A
|
The kinetic energy of a bus
travelling on an expressway is 30000J
|
A bus of mass m travelling on an
expressway will travel between 50 to 80 kmh-1, which is 13.8 to
22.2 ms-1. Thus, its KE will be approximately ½ m(182) = 162m.
Thus, for its KE to be 30000J: 162m = 30000. Thus, m = 185kg, which is an
absurd weight for a bus; ie. This is not a realistic estimate.
|
|
B
|
The power of a domestic light is
300W.
|
A single light bulb in the house
usually runs at about 20W to 60W. Thus, a domestic light is unlikely to run
at more than 200W; this estimate is rather high.
|
|
C
|
The temperature of a hot oven is
300 K.
|
300K = 27 0C. Not very hot.
|
|
D
|
The volume of air in a car tyre is
0.03 m3.
|
![]() |
Estimating the width of a tyre, t,
is 15 cm or 0.15 m, and estimating R to be 40 cm and r to be 30
cm,
volume of air in a car tyre is
= π(R2 – r2)t = π(0.42 – 0.32)(0.15) = 0.033 m3 ≈ 0.03 m3 (to one sig. fig.) |
Distinction
between systematic errors (including zero errors) and random errors and between
precision and accuracy:
Random error: is the type of error
which causes readings to scatter about the true value.
Systematic error: is the type of
error which causes readings to deviate in one direction from the true value.
Precision: refers to the degree
of agreement (scatter, spread) of repeated measurements of the same
quantity. {NB: regardless of whether or not they are correct.}
Accuracy: refers to the degree of
agreement between the result of a measurement and the true value of the
quantity.
|
→ → R Error Higher → → →
→ → → Less Precise → → → |
|
↓
↓ ↓
S
Error
Higher
Less
Accurate
↓
↓ ↓ |
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Assess the uncertainty in a derived
quantity by simple addition of actual, fractional or percentage uncertainties
(a rigorous statistical treatment is not required).
For a quantity x = (2.0 ± 0.1) mm,
Actual/ Absolute uncertainty, Δ x =
± 0.1 mm
Fractional uncertainty, Δxx = 0.05
Percentage uncertainty, Δxx ´ 100% = 5 %
If p = (2x + y) / 3 or p = (2x - y)
/ 3 , Δp = (2Δx + Δy) / 3
If r = 2xy3 or r = 2x / y3
, Δr / r = Δx / x + 3Δy / y
Actual error must be recorded
to only 1 significant figure, &
The number of decimal places a calculated quantity should have is determined by its actual error.
The number of decimal places a calculated quantity should have is determined by its actual error.
For eg, suppose g has been initially
calculated to be 9.80645 ms-2 & Δg has been initially calculated
to be 0.04848 ms-2. The final value of Δg must be recorded as 0.05
ms-2 {1 sf }, and the appropriate recording of g is (9.81 ± 0.05) ms-2.
Distinction
between scalar and vector quantities:
|
Scalar
|
Vector
|
Definition
|
A scalar quantity
has a magnitude only. It is completely described by a certain number
and a unit.
|
A vector quantity
has both magnitude and direction. It can be described by an arrow
whose length represents the magnitude of the vector and the arrow-head
represents the direction of the vector.
|
Examples
|
Distance, speed, mass, time,
temperature, work done, kinetic energy, pressure, power, electric
charge etc.
Common Error: Students tend to associate kinetic energy and pressure with vectors because of the vector components involved. However, such considerations have no bearings on whether the quantity is a vector or scalar. |
Displacement, velocity, moments
(or torque), momentum, force, electric field etc.
|
Representation
of vector as two perpendicular components:
In the diagram below, XY represents
a flat kite of weight 4.0 N. At a certain instant, XY is inclined at 30° to the
horizontal and the wind exerts a steady force of 6.0 N at right angles to XY so
that the kite flies freely.

By
accurate scale drawing
|
By
calculations using sine and cosine rules, or Pythagoras‟ theorem
|
Draw a scale diagram to find the
magnitude and direction of the resultant force acting on the kite.
![]()
R = 3.2 N (≡ 3.2 cm)
at θ = 112° to the 4 N vector. |
![]()
Using cosine rule, a2 =
b2 + c2 – 2bc cos A
R2 = 42 + 62 -2(4)(6)(cos 30°) R = 3.23 N
Using sine rule: a / sin A = b /
sin B
6 / sin α = 3.23 / sin 30° α = 68° or 112° = 112° to the 4 N vector |
Kinematics
Displacement, speed, velocity and acceleration:
Distance: Total length covered irrespective of the direction of motion.Displacement: Distance moved in a certain direction.
Speed: Distance travelled per unit time.
Velocity: is defined as the rate of change of displacement, or, displacement per unit time
{NOT: displacement over time, nor, displacement per second, nor, rate of change of displacement per unit time}
Acceleration: is defined as the rate of change of velocity.
Using graphs to find displacement, velocity and acceleration:
- The area under a velocity-time graph is the change in displacement.
- The gradient of a displacement-time graph is the {instantaneous} velocity.
- The gradient of a velocity-time graph is the acceleration.
The 'SUVAT' Equations of Motion
The most important word for this chapter is SUVAT, which stands for:- S (displacement),
- U (initial velocity),
- V (final velocity),
- A (acceleration) and
- T (time)
Below is a list of the equations you MUST memorise, even if they are in the formula book, memorise them anyway, to ensure you can implement them quickly.
1.
|
v = u +at
|
derived from definition of acceleration: a = (v – u) / t
|
2.
|
s = ½ (u + v) t
|
derived from the area under the v-t graph
|
3.
|
v2 = u2 + 2as
|
derived from equations (1) and (2)
|
4.
|
s = ut + ½at2
|
derived from equations (1) and (2)
|
Motion of bodies falling in a uniform gravitational field with air resistance:
Consider a body moving in a uniform gravitational field under 2 different conditions:Without Air Resistance:

With Air Resistance:

At the highest point, the body is momentarily at rest; air resistance becomes zero and hence the only force acting on it is the weight. The acceleration is thus 9.81 ms-2 at this point.
As a body falls, air resistance opposes its weight. The downward acceleration is thus less than 9.81 ms-2. As air resistance increases with speed, it eventually equals its weight (but in opposite direction). From then there will be no resultant force acting on the body and it will fall with a constant speed, called the terminal velocity.
Equations for the horizontal and vertical motion:
|
x direction
(horizontal – axis)
|
y direction
(vertical – axis)
|
s (displacement)
|
sx = ux
t
sx = ux t + ½ax t2 |
sy = uy
t + ½ ay t2
(Note: If projectile ends at same level as the start, then sy = 0) |
u (initial
velocity)
|
ux
|
uy
|
v (final
velocity)
|
vx = ux
+ axt
(Note: At max height, vx = 0) |
vy = uy
+ at
vy2 = uy2 + 2asy |
a (acceleration)
|
ax
(Note: Exists when a force in x direction present) |
ay
(Note: If object is falling, then ay = -g) |
t (time)
|
t
|
T
|
θ: direction of tangential velocity {NOT: tan θ = sy / sx }
Dynamics
Newton's
laws of motion:
Newton's First Law
Every body continues in a state of rest or uniform motion in a straight line unless a net (external) force acts on it.
Every body continues in a state of rest or uniform motion in a straight line unless a net (external) force acts on it.
Newton's Second Law
The rate of change of momentum of a body is directly proportional to the net force acting on the body, and the momentum change takes place in the direction of the net force.
The rate of change of momentum of a body is directly proportional to the net force acting on the body, and the momentum change takes place in the direction of the net force.
Newton's Third Law
When object X exerts a force on object Y, object Y exerts a force of the same type that is equal in magnitude and opposite in direction on object X.
When object X exerts a force on object Y, object Y exerts a force of the same type that is equal in magnitude and opposite in direction on object X.
The two forces ALWAYS act on different
objects and they form an action-reaction pair.
Linear
momentum and its conservation:
Mass: is a measure of the amount of
matter in a body, & is the property of a body which resists change in
motion.
Weight: is the force of
gravitational attraction (exerted by the Earth) on a body.
Linear momentum: of a body is
defined as the product of its mass and velocity ie p = m v
Impulse of a force (I): is defined
as the product of the force and the time Δt during which it acts
ie
I = F x Δt {for force which is const over the duration Δt}
For a variable force, the
impulse I = Area under the F-t graph { ∫Fdt; may need to “count squares”}
Impulse is equal in magnitude
to the change in momentum of the body acted on by the force.
Hence the change in momentum of the body is equal in mag to the area under a (net) force-time graph.
{Incorrect to define impulse as change in momentum}
Hence the change in momentum of the body is equal in mag to the area under a (net) force-time graph.
{Incorrect to define impulse as change in momentum}
Force: is defined as the rate of
change of momentum, ie F = [ m (v - u) ] / t = ma or F = v dm / dt
The {one} Newton: is defined as the force needed to accelerate a mass of 1 kg by 1 m s-2.
The {one} Newton: is defined as the force needed to accelerate a mass of 1 kg by 1 m s-2.
Principle of Conservation of Linear
Momentum: When objects of a system interact, their total momentum before and
after interaction are equal if no net (external) force acts on the
system.
- The total momentum of an isolated system is constant
- m1 u1 + m2 u2 = m1 v1 + m2 v2 if net F = 0 {for all collisions }
NB: Total momentum DURING
the interaction/collision is also conserved.
(Perfectly) elastic collision: Both
momentum & kinetic energy of the system are conserved.
Inelastic collision: Only momentum
is conserved, total kinetic energy is not conserved.
Perfectly inelastic collision: Only
momentum is conserved, and the particles stick together after collision. (i.e.
move with the same velocity.)
For all elastic
collisions, u1 – u2 = v2 – v1
ie. relative speed of approach =
relative speed of separation
or, ½ m1u12
+ ½ m2u22 = ½ m1v12
+ ½ m2v22
In inelastic collisions, total
energy is conserved but Kinetic Energy may be converted into other forms of
energy such as sound and heat energy.
Forces
Hooke's
Law:
Within the limit of proportionality,
the extension produced in a material is directly proportional to the force/load
applied
F
= kx
Force constant k = force per unit extension (F/x)
Force constant k = force per unit extension (F/x)
Elastic potential energy/strain
energy = Area under the F-x graph {May
need to “count the squares”}
For a material that obeys Hooke‟s
law,
Elastic
Potential Energy, E = ½ F x = ½ k x2
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.
A region of space in which a mass experiences an (attractive) force due to the presence of another mass.
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.
A region of space where a charge experiences an (attractive or repulsive) force due to the presence of another charge.
Hydrostatic
Pressure p = ρgh
{or,
pressure difference between 2 points separated by a vertical distance of
h }
Upthrust: An upward force exerted by
a fluid on a submerged or floating object; arises because of the difference
in pressure between the upper and lower surfaces of the object.
Archimedes' Principle: Upthrust =
weight of the fluid displaced by submerged object.
ie
Upthrust = Volsubmerged x ρfluid x g
Frictional Forces:
- The contact force between two surfaces = (friction2 + normal reaction2)½
- The component along the surface of the contact force is called friction
- Friction between 2 surfaces always opposes relative motion {or attempted motion}, and
- Its value varies up to a maximum value {called the static friction}
Viscous Forces:
- A force that opposes the motion of an object in a fluid
- Only exists when there is (relative) motion
- Magnitude of viscous force increases with the speed of the object
Centre of Gravity of an object is
defined as that pt through which the entire weight of the object may be
considered to act.
A couple is a pair of forces which
tends to produce rotation only.
Moment of a Force: The product of
the force and the perpendicular distance of its line of action to the pivot
Torque of a Couple: The produce of
one of the forces of the couple and the perpendicular distance between the
lines of action of the forces. (WARNING: NOT an action-reaction pair as
they act on the same body.)
Conditions for Equilibrium (of an
extended object):
- The resultant force acting on it in any direction equals zero
- The resultant moment about any point is zero
If a mass is acted upon by 3
forces only and remains in equilibrium, then
- The lines of action of the 3 forces must pass through a common point
- When a vector diagram of the three forces is drawn, the forces will form a closed triangle (vector triangle), with the 3 vectors pointing in the same orientation around the triangle.
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.
Work, Energy and Power
Work Done by a force is defined as
the product of the force and displacement (of its point of application) in
the direction of the force
W
= F s cos θ
Negative work is said to be done by F if x or its compo. is anti-parallel
to F
If a variable force F produces a displacement in the direction of F, the work done is determined from the area under F-x graph. {May need to find area by “counting the squares”. }
If a variable force F produces a displacement in the direction of F, the work done is determined from the area under F-x graph. {May need to find area by “counting the squares”. }
By Principle of Conservation of
Energy,
Work
Done on a system = KE gain + GPE gain + Work done against friction}
Consider a rigid object of mass m
that is initially at rest. To accelerate it uniformly to a speed v, a constant
net force F is exerted on it, parallel to its motion over a displacement s.
Since F is constant, acceleration is
constant,
Therefore, using the equation:
v2
= u2 +2as,
as = 12 (v2 - u2)
as = 12 (v2 - u2)
Since kinetic energy is equal to the
work done on the mass to bring it from rest to a speed v,
The kinetic energy, EK
|
= Work done by the force F
= Fs = mas = ½ m (v2 - u2) |
Gravitational potential energy: this
arises in a system of masses where there are attractive gravitational
forces between them. The gravitational potential energy of an object is the
energy it possesses by virtue of its position in a gravitational field.
Elastic potential energy: this
arises in a system of atoms where there are either attractive or repulsive
short-range inter-atomic forces between them.
Electric potential energy: this
arises in a system of charges where there are either attractive or repulsive
electric forces between them.
The potential energy, U, of a body
in a force field {whether gravitational or electric field} is related to the
force F it experiences by:
F = - dU / dx.
F = - dU / dx.
Consider an object of mass m being
lifted vertically by a force F, without acceleration, from a certain height h1
to a height h2. Since the object moves up at a constant speed, F is
equal to mg.
The change in
potential energy of the mass
|
= Work done by the force F
= F s = F h = m g h |
Efficiency: The ratio of (useful)
output energy of a machine to the input energy.
ie
=
|
Useful
Output Energy
|
x100%
=
|
Useful
Output Power
|
x100%
|
Input
Energy
|
Input
Power
|
Power {instantaneous} is defined as
the work done per unit time.
P
=
|
Total
Work Done
|
=
|
W
|
Total
Time
|
t
|
Since work done W = F x s,
P
=
|
F
x s
|
=
|
Fv
|
t
|
- for object moving at const speed: F = Total resistive force {equilibrium condition}
- for object beginning to accelerate: F = Total resistive force + ma
Wave Motion
Displacement (y): Position of an
oscillating particle from its equilibrium position.
Amplitude (y0 or A): The
maximum magnitude of the displacement of an oscillating particle from its
equilibrium position.
Period (T): Time taken for a
particle to undergo one complete cycle of oscillation.
Frequency (f): Number of
oscillations performed by a particle per unit time.
Wavelength (λ): For a progressive
wave, it is the distance between any two successive particles
that are in phase, e.g. it is the distance between 2 consecutive
crests or 2 troughs.
Wave speed (v): The speed at which
the waveform travels in the direction of the propagation of the wave.
Wave front: A line or surface
joining points which are at the same state of oscillation, i.e. in phase, e.g.
a line joining crest to crest in a wave.
Ray: The path taken by the wave.
This is used to indicate the direction of wave propagation. Rays are always at
right angles to the wave fronts (i.e. wave fronts are always perpendicular to
the direction of propagation).
From the definition of speed, Speed
= Distance / Time
A wave travels a distance of one wavelength, λ, in a time interval of one period, T.
The frequency, f, of a wave is equal to 1 / T
Therefore, speed, v = λ / T = (1 / T)λ = fλ
A wave travels a distance of one wavelength, λ, in a time interval of one period, T.
The frequency, f, of a wave is equal to 1 / T
Therefore, speed, v = λ / T = (1 / T)λ = fλ
v
= fλ
Example 1:
A wave travelling in the positive x direction is showed in the figure. Find the amplitude, wavelength, period, and speed of the wave if it has a frequency of 8.0 Hz.
Amplitude (A) = 0.15 m
Wavelength (λ) = 0.40 m
Period (T) = 1f = 18.0 ≈ 0.125 s
Speed (v) =fλ = 8.0 x 0.40 = 3.20
m s-1
A wave which results in a net
transfer of energy from one place to another is known as a progressive wave.
|
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Intensity {of a wave}: is defined as
the rate of energy flow per unit time {power} per unit cross-sectional area
perpendicular to the direction of wave propagation.
Intensity
= Power / Area = Energy / (Time x Area)
For a point source (which
would emit spherical wavefronts),
Intensity = (½mω2xo2)
/ (t x 4πr2) where x0: amplitude & r: distance from
the point source.
Therefore, I ∝ xo2 / r2 (Pt Source)
Therefore, I ∝ xo2 / r2 (Pt Source)
For all wave sources, I ∝ (Amplitude)2
Transverse
wave:
A wave in which the oscillations
of the wave particles {NOT: movement} are perpendicular to
the direction of the propagation of the wave.

Longitudinal
wave:
A wave in which the oscillations
of the wave particles are parallel to the direction of the
propagation of the wave.

Polarisation is said to occur when
oscillations are in one direction in a plane, {NOT just “in one
direction”} normal to the direction of propagation.
{Only transverse waves can
be polarized; longitudinal waves can’t.}
Example 2:
The following stationary wave pattern is obtained using a C.R.O. whose screen is graduated in centimetre squares. Given that the time-base is adjusted such that 1 unit on the horizontal axis of the screen corresponds to a time of 1.0 ms, find the period and frequency of the wave.
Period, T = (4 units) x 1.0
= 4.0 ms = 4.0 x 10-3 s
f = 1 / T
= 14 x 10-3 = 250 Hz |
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Superposition
Principle of Superposition: When two
or more waves of the same type meet at a point, the resultant displacement
of the waves is equal to the vector sum of their individual
displacements at that point.
Stretched
String
A horizontal rope with one end fixed
and another attached to a vertical oscillator. Stationary waves will be
produced by the direct and reflected waves in the string.

Or we can have the string stopped at
one end with a pulley as shown below.

Microwaves
A microwave emitter placed a
distance away from a metal plate that reflects the emitted wave. By moving a
detector along the path of the wave, the nodes and antinodes could be detected.

Air
column
A tuning fork held at the mouth of a
open tube projects a sound wave into the column of air in the tube. The length
of the tube can be changed by varying the water level. At certain lengths of
the tube, the air column resonates with the tuning fork. This is due to the
formation of stationary waves by the incident and reflected sound
waves at the water surface.

Stationary (Standing) Wave) is one
- whose waveform/wave profile does not advance {move},
- where there is no net transport of energy, and
- where the positions of antinodes and nodes do not change (with time).
A stationary wave is formed when two
progressive waves of the same frequency, amplitude
and speed, travelling in opposite directions are
superposed. {Assume boundary conditions are met}
|
Stationary
Waves
|
Stationary
Waves Progressive Waves
|
Amplitude
|
Varies from maximum at the
anti-nodes to zero at the nodes.
|
Same for all particles in the wave
(provided no energy is lost).
|
Wavelength
|
Twice the distance between a pair
of adjacent nodes or anti-nodes.
|
The distance between two
consecutive points on a wave, that are in phase.
|
Phase
|
Particles in the same segment/
between 2 adjacent nodes, are in phase. Particles in adjacent segments are in
anti-phase.
|
All particles within one
wavelength have different phases.
|
Wave
Profile
|
The wave profile does not advance.
|
The wave profile advances.
|
Energy
|
No energy is transported by the
wave.
|
Energy is transported in the
direction of the wave.
|
Node is a region of destructive
superposition where the waves always meet out of phase by π radians.
Hence displacement here is permanently zero {or minimum}.
Antinode is a region of constructive
superposition where the waves always meet in phase. Hence a
particle here vibrates with maximum amplitude {but it is NOT a pt
with a permanent large displacement!}
Dist
between 2 successive nodes / antinodes = λ / 2
Max pressure change occurs at the nodes {NOT the antinodes} because
every node changes fr being a pt of compression to become a pt of rarefaction
{half a period later}
Diffraction: refers to the spreading
{or bending} of waves when they pass through an opening {gap}, or round an
obstacle (into the “shadow” region). {Illustrate with diag}
For significant diffraction to occur, the size of the gap ≈ λ of the wave
For significant diffraction to occur, the size of the gap ≈ λ of the wave
For a diffraction grating, d sin θ =
n λ ,
d = dist between successive slits {grating spacing} = reciprocal of number of lines per metre
d = dist between successive slits {grating spacing} = reciprocal of number of lines per metre
When a “white light” passes
through a diffraction grating, for each order of diffraction, a longer wavelength
{red} diffracts more than a shorter wavelength {violet} {as sin θ ∝ λ}.
Diffraction refers to the spreading of waves as they pass through a
narrow slit or near an obstacle.
For diffraction to occur, the size
of the gap should approximately be equal to the wavelength of the wave.


Coherent waves: Waves having a constant
phase difference {not: zero phase difference / in phase}
Interference may be described as the
superposition of waves from 2 coherent sources.
For an observable / well-defined
interference pattern, the waves must be coherent, have about
the same amplitude, be unpolarised or polarised
in the same direction, & be of the same type.
Two-source
interference using:
1.
Water Waves

Interference patterns could be
observed when two dippers are attached to the vibrator of the ripple tank. The
ripples produce constructive and destructive interference. The dippers are
coherent sources because they are fixed to the same vibrator.
2.
Microwaves

Microwave emitted from a transmitter
through 2 slits on a metal plate would also produce interference patterns. By
moving a detector on the opposite side of the metal plate, a series of rise and
fall in amplitude of the wave would be registered.
3.
Light Waves (Young‟s double slit experiment)

Since light is emitted from a bulb
randomly, the way to obtain two coherent light sources is by splitting light
from a single slit.
The 2 beams from the double slit
would then interfere with each other, creating a pattern of alternate bright
and dark fringes (or high and low intensities) at regular intervals, which is
also known as our interference pattern.

Condition
for Constructive Interference at a pt P:
Phase difference of the 2 waves at P = 0 {or 2π, 4π, etc}
Thus, with 2 in-phase
sources, * implies path difference = nλ; with 2 antiphase
sources: path difference = (n + ½)λ
Condition
for Destructive Interference at a pt P:
Phase difference of the 2 waves at P = π { or 3π, 5π, etc }
With 2 in-phase sources, + implies path difference = (n+ ½ λ), with 2 antiphase sources: path difference = n λ
With 2 in-phase sources, + implies path difference = (n+ ½ λ), with 2 antiphase sources: path difference = n λ
Fringe separation x = λD / a,
if a<<D {applies only to Young's Double Slit interference of light, ie, NOT for microwaves, sound waves, water waves}
if a<<D {applies only to Young's Double Slit interference of light, ie, NOT for microwaves, sound waves, water waves}
Phase difference Δφ betw the 2 waves
at any pt X {betw the central & 1st maxima) is (approx) proportional to the
dist of X from the central maxima.
Using 2 sources of equal amplitude x0,
the resultant amplitude of a bright fringe would be doubled {2x0},
& the resultant intensity increases by 4 times {not 2 times}. { IResultant
∝ (2 x0)2 }
Electric Fields
Electric field strength / intensity
at a point is defined as the force per unit positive charge
acting at that point {a vector; Unit: N C-1 or V m-1}
E
= F / q → F = qE
- The electric force on a positive charge in an electric field is in the direction of E, while
- The electric force on a negative charge is opposite to the direction of E.
- Hence a +ve charge placed in an electric field will accelerate in the direction of E and gain KE {& simultaneously lose EPE}, while a negative charge caused to move (projected) in the direction of E will decelerate, ie lose KE, { & gain EPE}.
Representation
of electric fields by field lines
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Coulomb's
law:
The (mutual) electric force F acting
between 2 point charges Q1 and Q2 separated by a
distance r is given by:
F
= Q1Q2 / 4πεor2 where ε0:
permittivity of free space
or,
the (mutual) electric force between two point charges is proportional to the
product of their charges & inversely proportional to the square of their
separation.
Example
1:
Two positive charges, each 4.18 μC,
and a negative charge, -6.36 μC, are fixed at the vertices of an equilateral
triangle of side 13.0 cm. Find the electrostatic force on the negative charge.
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F = Q1Q2 /
4πεor2
= (8.99 x 109) [(4.18 x
10-6)(6.36 x 10-6) / (13.0 x 10-2)2]
= 14.1 N
(Note: negative sign for -6.36 μC
has been ignored in the calculation)
FR = 2 x Fcos300
= 24.4 N, vertically upwards
|
Electric
field strength due to a Point Charge Q
: E = Q / 4πεor2
{NB: Do NOT substitute a negative Q with its negative sign in calculations!}
{NB: Do NOT substitute a negative Q with its negative sign in calculations!}
Example
2:
In the figure below, determine the
point (other than at infinity) at which the total electric field strength is
zero.

From the diagram, it can be observed
that the point where E is zero lies on a straight line where the charges lie,
to the left of
the -2.5 μC charge.
the -2.5 μC charge.
Let this point be a distance r from
the left charge.
Since the total electric field
strength is zero,
E6μ = E-2μ
[6μ / (1 + r)2] / 4πεor2
= [2.5μ / r2] / 4πεor2 (Note: negative sign
for -2.5 μC has been ignored here)
6 / (1 + r)2 = 2.5 / r2
√(6r) = 2.5 (1 + r)
r = 1.82 m
The point lies on a straight line
where the charges lie, 1.82 m to the left of the -2.5 μC charge.
Uniform
electric field between 2 Charged Parallel Plates: E = Vd,
d: perpendicular dist between the plates,
V: potential difference between plates
d: perpendicular dist between the plates,
V: potential difference between plates
Path of charge moving at 90° to
electric field: parabolic.
Beyond the pt where it exits the field, the path is a straight line, at a tangent to the parabola at exit.
Beyond the pt where it exits the field, the path is a straight line, at a tangent to the parabola at exit.
Example
3:
An electron (m = 9.11 x 10-31
kg; q = -1.6 x 10-19 C) moving with a speed of 1.5 x 107
ms-1, enters a region between 2 parallel plates, which are 20 mm
apart and 60 mm long. The top plate is at a potential of 80 V relative to the
lower plate. Determine the angle through which the electron has been deflected
as a result of passing through the plates.

Time taken for the electron to
travel 60 mm horizontally = Distance / Speed = 60 x 10-3 / 1.5 x 107
= 4 x 10-9 s
E = V / d = 80 / 20 x 10-3 = 4000 V m-1
a = F / m = eE / m = (1.6 x 10-19)(4000) / (9.1 x 10-31) = 7.0 x 1014 ms-2
vy = uy + at = 0 + (7.0 x 1014)( 4 x 10-9) = 2.8 x 106 ms-1
tan θ = vy / vx = 2.8 x 106 / 1.5 x 107 = 0.187
Therefore θ = 10.6°
E = V / d = 80 / 20 x 10-3 = 4000 V m-1
a = F / m = eE / m = (1.6 x 10-19)(4000) / (9.1 x 10-31) = 7.0 x 1014 ms-2
vy = uy + at = 0 + (7.0 x 1014)( 4 x 10-9) = 2.8 x 106 ms-1
tan θ = vy / vx = 2.8 x 106 / 1.5 x 107 = 0.187
Therefore θ = 10.6°
Effect
of a uniform electric field on the motion of charged particles
- Equipotential surface: a surface where the electric potential is constant
- Potential gradient = 0, ie E along surface = 0 }
- Hence no work is done when a charge is moved along this surface.{ W=QV, V=0 }
- Electric field lines must meet this surface at right angles.
- {If the field lines are not at 90° to it, it would imply that there is a non-zero component of E along the surface. This would contradict the fact that E along an equipotential = 0. }
Electric potential at a point: is
defined as the work done in moving a unit positive
charge from infinity to that point, { a scalar; unit: V } ie V = W / Q
The electric potential at infinity
is defined as zero. At any other point, it may be positive or negative
depending on the sign of Q that sets up the field. {Contrast gravitational
potential.}
Relation between E and V: E = - dV /
dr
i.e. The electric field strength at
a pt is numerically equal to the potential gradient at that pt.
NB: Electric field lines point in
direction of decreasing potential {ie from high to low pot}.
Electric potential energy U of a
charge Q at a pt where the potential is V: U = QV
Work done W on a charge Q in moving it across a pd ΔV: W = Q ΔV
Work done W on a charge Q in moving it across a pd ΔV: W = Q ΔV
Electric Potential due to a point
charge Q : V = Q / 4πεo
Current of Electricity
Electric current is the rate of flow
of charge. {NOT: charged particles}
Electric charge Q passing a point is
defined as the product of the (steady) current at that point and the time for
which the current flows,
Q
= I t
One coulomb is defined as the charge
flowing per second pass a point at which the current is one
ampere.
Example 1:
An ion beam of singly-charged Na+ and K+ ions is passing through vacuum. If the beam current is 20 μ A, calculate the total number of ions passing any fixed point in the beam per second. (The charge on each ion is 1.6 x 10-19 C.)
An ion beam of singly-charged Na+ and K+ ions is passing through vacuum. If the beam current is 20 μ A, calculate the total number of ions passing any fixed point in the beam per second. (The charge on each ion is 1.6 x 10-19 C.)
Current, I = Q / t = Ne / t
where N is the no. of ions and e is the charge on one ion.
No. of ions per second = N / t = I /
e = (20 x 10-6) / (1.6 x 10-19) = 1.25 x 10-14
Potential difference is defined as
the energy transferred from electrical energy to other forms of energy
when unit charge passes through an electrical device,
V
= W / Q
P. D. = Energy Transferred / Charge
= Power / Current or, is the ratio of the power supplied to the device to the
current flowing,
V
= P / I
The volt: is defined as the
potential difference between 2 pts in a circuit in which one joule of energy
is converted from electrical to non-electrical energy when one coulomb
passes from 1 pt to the other, ie 1 volt = One joule per coulomb
Difference between Potential and
Potential Difference (PD):
The potential at a point of the circuit is due to the amount of charge present along with the energy of the charges. Thus, the potential along circuit drops from the positive terminal to negative terminal, and potential differs from points to points.
The potential at a point of the circuit is due to the amount of charge present along with the energy of the charges. Thus, the potential along circuit drops from the positive terminal to negative terminal, and potential differs from points to points.
Potential Difference refers to the
difference in potential between any given two points.
For example, if the potential of point A is 1 V and the potential at point B is 5 V, the PD across AB, or VAB , is 4 V. In addition, when there is no energy loss between two points of the circuit, the potential of these points is same and thus the PD across is 0 V.
For example, if the potential of point A is 1 V and the potential at point B is 5 V, the PD across AB, or VAB , is 4 V. In addition, when there is no energy loss between two points of the circuit, the potential of these points is same and thus the PD across is 0 V.
Example 2:
A current of 5 mA passes through a bulb for 1 minute. The potential difference across the bulb is 4 V. Calculate:
A current of 5 mA passes through a bulb for 1 minute. The potential difference across the bulb is 4 V. Calculate:
(a) The amount of charge passing
through the bulb in 1 minute.
Charge Q = I t = 5 x 10-3
x 60 = 0.3 C
(b) The work done to operate the
bulb for 1 minute.
Potential difference across the bulb
= W / Q
4 = W / 0.3
Work done to operate the bulb for 1 minute = 0.3 x 4 = 1.2 J
4 = W / 0.3
Work done to operate the bulb for 1 minute = 0.3 x 4 = 1.2 J
Electrical
Power, P = V I = I2 / R = V2 / R
{Brightness of a lamp is
determined by the power dissipated, NOT: by V, or I or R alone}
Example 3:
A high-voltage transmission line with a resistance of 0.4 Ω km-1 carries a current of 500 A. The line is at a potential of 1200 kV at the power station and carries the current to a city located 160 km from the power station. Calculate
A high-voltage transmission line with a resistance of 0.4 Ω km-1 carries a current of 500 A. The line is at a potential of 1200 kV at the power station and carries the current to a city located 160 km from the power station. Calculate
(a) the power loss in the line.
The power loss in the line P = I2
R = 5002 x 0.4 x 160 = 16 MW
(b) the fraction of the transmitted
power that is lost.
The total power transmitted = I V =
500 x 1200 x 103 = 600 MW
The fraction of power loss = 16 / 600 = 0.267
The fraction of power loss = 16 / 600 = 0.267
Resistance is defined as the ratio
of the potential difference across a component to the current flowing through
it ,
R
= VI
{It is NOT defined
as the gradient of a V-I graph; however for an ohmic conductor,
its resistance equals the gradient of its V-I graph as this graph
is a straight line which passes through the origin}
The Ohm: is the resistance of a
resistor if there is a current of 1 A flowing through it when the pd across it
is 1 V, ie,
1 Ω = One volt per ampere
1 Ω = One volt per ampere
Example 4:
In the circuit below, the voltmeter reading is 8.00 V and the ammeter reading is 2.00 A. Calculate the resistance of R.
In the circuit below, the voltmeter reading is 8.00 V and the ammeter reading is 2.00 A. Calculate the resistance of R.
Resistance
of R = V / I = 8 / 2 = 4.0 Ω
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Temperature
characteristics of thermistors:
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The resistance (i.e. the ratio V /
I) is constant because metallic conductors at constant temperature obey Ohm's
Law.
|
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As V increases, the temperature
increases, resulting in an increase in the amplitude of vibration of ions and
the collision frequency of electrons with the lattice ions. Hence the
resistance of the filament increases with V.
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A thermistor is made from
semi-conductors. As V increases, temperature increases. This releases more
charge carriers (electrons and holes) from the lattice, thus reducing the
resistance of the thermistor. Hence, resistance decreases as temperature
increases.
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In forward bias, a diode has low
resistance.
In reverse bias, the diode has high resistance until the breakdown voltage is reached. |
Ohm's law: The current in a
component is proportional to the potential difference across it provided
physical conditions (eg temp) stay constant.
R
= ρL / A {for a conductor of length l, uniform x-sect area A and resistivity ρ}
Resistivity is defined as the
resistance of a material of unit cross-sectional area and unit length.
{From R = ρl / A , ρ = RA / L}
Example 5:
Calculate the resistance of a nichrome wire of length 500 mm and diameter 1.0 mm, given that the resistivity of nichrome is
1.1 x 10-6 Ω m.
Calculate the resistance of a nichrome wire of length 500 mm and diameter 1.0 mm, given that the resistivity of nichrome is
1.1 x 10-6 Ω m.
Resistance, R = ρl / A = [(1.1 x 10-6)(500
x 10-3)] / π(1 x 10-3 / 2)2 = 0.70 Ω
Electromotive force (Emf) is defined
as the energy transferred / converted from non-electrical forms of energy
into electrical energy when unit charge is moved round a complete
circuit. ie EMF = Energy Transferred per unit charge
E
= WQ
EMF refers to the electrical energy
generated from non-electrical energy forms, whereas PD refers to electrical
energy being changed into non-electrical energy. For example,
EMF
Sources
|
Energy
Change
|
PD
across
|
Energy
Change
|
Chemical Cell
|
Chem → Elec
|
Bulb
|
Elec → Light
|
Generator
|
Mech → Elec
|
Fan
|
Elec → Mech
|
Thermocouple
|
Thermal → Elec
|
Door Bell
|
Elec → Sound
|
Solar Cell
|
Solar → Elec
|
Heating element
|
Elec → Thermal
|
Effects
of the internal resistance of a source of EMF:
Internal resistance is the
resistance to current flow within the power source. It reduces the potential
difference (not EMF) across the terminal of the power supply when it is
delivering a current.
Consider the circuit below:

The voltage across the resistor, V =
IR,
The voltage lost to internal resistance = Ir
Thus, the EMF of the cell, E = IR + Ir = V + Ir
Therefore If I = 0A or if r = 0Ω, V = E
The voltage lost to internal resistance = Ir
Thus, the EMF of the cell, E = IR + Ir = V + Ir
Therefore If I = 0A or if r = 0Ω, V = E
Nuclear Physics
Experimental evidence for a small charged nucleus in an
atom:
Results of an experiment where a beam of alpha particles is fired at a thin
gold foil, where n= no of alpha particles incident per unit time.

A very small proportion was deflected by more than 90°, some of these approaching 180°
From these 2 observations it can be deduced that: the nucleus occupies only a small proportion of the available space (ie the atom is mostly empty space) & that it is positively charged since the positively-charged alpha particles are repelled/deflected.
Nucleon: A particle within the nucleus; can be either a proton or a neutron
Nuclide: An atom with a particular number of protons and a particular number of neutrons
Proton number Z {old name: atomic number}: No. of protons in an atom
Nucleon number N {mass number}: Sum of number of protons and neutrons in an atom
Isotopes: are atoms with the same proton number, but different nucleon number {or different no of neutrons}
Mass defect and Nuclear Binding Energy::
Energy & Mass are Equivalent: E = mc2 → ΔE =
(Δm)c2
Nuclear Binding Energy:
- Energy that must be supplied to completely separate the nucleus into its individual nucleons/particles.
- The energy released {not lost} when a nucleus is formed from its constituent nucleons.
Mass Defect: The difference in mass between a nucleus and the total mass of its individual nucleons
Zmp + (A -
Z)mn - Mass of Nucleus
Thus, Binding Energy. = Mass Defect x c2In both nuclear fusion and fission, products have higher B.E. per nucleon {due to shape of BE per nucleon-nucleon graph}, energy is released {not lost} and hence products are more stable.
Energy released = Total B.E. after reaction (products) -
Total B.E. before reaction (reactants)
Nuclear fission: The disintegration of a heavy nucleus into 2 lighter
nuclei. Typically, the fission fragments have approximately the same mass
and neutrons are emitted.Fig below shows the variation of BE per nucleon plotted against the nucleon no.

Principle of Conservation of Energy-Mass:
Total energy-mass
before reaction = Total energy - mass after reaction
Σ (mc2 + ½ mv2)reactants = Σ (mc2 + ½ mv2)products + hf {if γ - photon emitted}
Energy released in nuclear reaction= Δmc2 = (Total
rest mass before reaction – Total rest mass after reaction) x c2Σ (mc2 + ½ mv2)reactants = Σ (mc2 + ½ mv2)products + hf {if γ - photon emitted}
Radioactive decay:
Radioactivity is the spontaneous and random decay of an unstable nucleus, with the emission of an alpha or beta particle, and is usually accompanied by the emission of a gamma ray photon.Spontaneous: The emission is not affected by factors outside the nucleus
Random: It cannot be predicted when the next emission will occur {Evidence in fluctuation in count-rate}
Decay law: dN/dt = -λN, where N= No. of undecayed {active} nuclei at that instant;
N = N0e-λt
; A = A0e-λt ; C = C0e-λt
Background radiation refers to radiation from sources other than the
source of interest.
True count rate =
Measured count rate – Background count rate
Nature of α, β & γ:
|
Alpha Particles
|
Beta particles
|
Gamma Particles
|
Notation
|
α
|
β
|
Γ
|
Charge
|
+ 2e
|
- e
|
No charge
|
Mass
|
4u
|
1/1840 u
|
Massless
|
Nature
|
Particle {He nucleus}
|
Particle {electron emitted from nucleus}
|
Electromagnetic Radiation
|
Speed
|
Monoenergetic
(i.e. one speed only) |
Continuous range
(up to approximately 98% of light) |
100% speed of light
|
Activity is defined as the rate at which the nuclei are disintegrating; A = dN/dt = λN
A0 = λ N0
Number of undecayed nuclei ∝ Mass of
sample
Number of nuclei in sample = (Sample Mass / Mass of 1
mol) x NAwhere, Mass of 1 mol of nuclide= Nucleon No {or relative atomic mass} expressed in grams {NOT: in kg!!}
{Thus for eg, mass of 1 mole of U-235 = 235 g = 235 x 10-3kg, NOT: 235 kg}
Application of PCM to radioactive decay:
It is useful to remember that when a stationary nucleus emits a single particle, by PCM, after the decay,the
ratio of their KE = ratio of their speeds = reciprocal of the ratio of their masses
Half-life is defined as the average time taken for half the number {not: mass or amount} of undecayed nuclei in the sample to disintegrate,
or, the average time taken for the activity to be halved.
t½ = (ln2)
/ λ
Example:Antimony-124 has a half-life of 60 days. If a sample of antimony-124 has an initial activity of 6.5 x 106Bq, what will its activity be after 1 year (365 days)?
Using A = A0e-λt & t½ = (ln2) / λ
A = 9.6 x 104Bq
Biological effect of radiation:
Radiation damage to biological organisms is often categorized as: somatic
and genetic.Somatic damage refers to any part of the body except the reproductive organs.
Somatic damage harms that particular organism directly. Some somatic effects include radiation sickness (nausea, fatigue, and loss of body hair) and burns, reddening of the skin, ulceration, cataracts in the eye, skin cancer, leukaemia, reduction of white blood cells, death, etc.
Genetic damage refers to damage to reproductive organs.
Genetic effects cause mutations in the reproductive cells and so affect future generations – hence, their effects are indirect. (Such mutations may contribute to the formation of a cancer.)
Alternatively,
- Ionising radiation may damage living tissues and cells directly.
- It may also occur indirectly through chemical changes in the surrounding medium, which is mainly water. For example, the ionization of water molecules produces OH free radicals which may react to produce H2O2, the powerful oxidizing agent hydrogen peroxide, which can then attack the molecules which form the chromosomes in the nucleus of each cell.
Good luck