Topic 1: Physical Quantities, Units and Measurement
Physical quantities consist of two parts: numerical magnitude and a unit.
Formally: a physical quantity = magnitude + unit. For example, a length of 5 meters consists of the magnitude 5 and the unit meter.
Classification of quantities
Basic (fundamental) quantities and SI base units:
length → unit: metre (m)
mass → kilogram (kg)
time → second (s)
thermodynamic temperature → kelvin (K)
amount of substance → mole (mol)
current → ampere (A)
Derived quantities – defined in terms of base quantities via equations; their SI units are derived from the base units.
For example, speed is derived from length/time, with the unit m/s.
Prefixes and orders of magnitude (SI prefixes)
Common prefixes and symbols (factor):
Tera (T) 1012
Giga (G) 109
Mega (M) 106
Kilo (k) 103
Deci (d) 10−1
Centi (c) 10−2
Milli (m) 10−3
Micro (µ) 10−6
Nano (n) 10−9
Pico (p) 10−12
The syllabus highlights the bolded ones (the ones listed above).
Example: Converting 5 km to meters: 5 km=5×103 m. Converting 200 mA to Amperes: 200 mA=200×10−3 A=0.2 A.
Orders of magnitude and estimation
Used to compare sizes from atomic scales to astronomical scales.
Examples:
Diameter of an atom: 10−10 m
Thickness of human hair: 10−5 m
Height of a human: 100 m (or ~1 meter)
Diameter of Earth: 107 m
Distance to the Sun: 1011 m
Scalars vs. vectors
Scalar: magnitude only (e.g., mass = 5 kg, distance = 10 m, time = 2 s, speed = 5 m/s, work = 10 J, energy = 50 J).
Vector: magnitude and direction (e.g., weight = 50 N downwards, displacement = 10 m East, velocity = 5 m/s North, acceleration = 2 m/s2 upwards, force = 20 N at 30∘ from horizontal).
Addition of vectors (graphical and analytical)
Resultant R of two perpendicular vectors F1 and F2:
Magnitude: R=F<em>12+F</em>22
Direction: tanθ=F</em>2F<em>1 (angle above the horizontal, for example)
Example: A force F<em>1=3 N acting East and a force F</em>2=4 N acting North.
The resultant magnitude R=32+42=9+16=25=5 N.
The direction θ=tan−1(34)≈53.1∘ North of East.
Graphical method: parallel–parallelogram rule, scale drawing, then measure the resultant.
Measurement of length and time
Instruments and accuracy:
Measuring tape, rule (±0.1 cm). Used for lengths from a few cm to several meters.
Micrometers (typically ±0.01 mm) and vernier calipers (typically ±0.01 cm).
Micrometers measure very small dimensions like the thickness of a wire or a sheet of paper.
Vernier calipers measure external/internal diameters or depths of objects.
Time: stopwatches; accuracy depends on the instrument and procedure. Digital stopwatches can read to 0.01 s.
Parallax errors and accuracy concepts
Parallax error arises from incorrect eye position or non-contact with the scale; correct positioning (eye level, perpendicular to scale) minimizes parallax.
Accuracy refers to how close a measurement is to the true value.
Vernier calipers
Used to measure external diameter, thickness, etc., with precision ±0.01 cm.
Zero error and correction procedures are important.
Positive Zero Error: When jaws are closed, the vernier zero mark is to the right of the main scale zero mark. Example: Vernier zero is at 0.04 cm. The reading will be (measured value - 0.04 cm).
Negative Zero Error: When jaws are closed, the vernier zero mark is to the left of the main scale zero mark. Example: Vernier zero is at -0.02 cm. The reading will be (measured value - (-0.02 cm) = measured value + 0.02 cm).
Micrometer screw gauge
Measures very small lengths with precision; reading = main scale + circular (thimble) scale; zero error checks required.
Example reading: If the main scale reads 3.5 mm and the thimble scale aligns with 25 (meaning 0.25 mm), the reading is 3.5 mm+0.25 mm=3.75 mm. Apply zero correction if necessary.
Period of oscillation of a simple pendulum
Definitions:
One oscillation: one complete to-and-fro movement from A to B to C and back to A.
Period T: time for one complete oscillation.
Amplitude: maximum displacement from rest position.
Period formula (near-earth gravity):
T=2πgl
Note: This formula is for small angles of oscillation (<10^\circ).
Example: A pendulum with length l=0.99 m on Earth (g≈9.81 m s−2) will have a period T=2π9.810.99≈2.00 s.
Topic 2: Kinematics
Scalars and vectors: Distance vs. displacement; Speed vs. velocity.
Distance: scalar; total path length covered. E.g., walking 5m North then 3m South, distance = 8m.
Displacement: vector; straight-line distance from start to end, with direction. E.g., for the above, displacement = 2m North.
Speed: scalar; rate of change of distance. E.g., 10 m/s.
Velocity: vector; rate of change of displacement. E.g., 10 m/s East.
Key definitions and equations
Speed: speed=tdistance travelled
Average speed: vavg=Total time takenTotal distance travelled
Velocity: rate of change of displacement; average velocity: vavg=ΔtΔx (where Δx is displacement and Δt is time interval).
Example: A car travels 100 km in 2 hours. Its average speed is 100 km/2 h=50 km/h.
Acceleration
Acceleration: a=ΔtΔv (rate of change of velocity).
Acceleration is a vector quantity (magnitude and direction). Positive for increasing velocity in a given direction, negative for decreasing velocity (deceleration) or increasing velocity in the opposite direction.
Example: A car increases its speed from 10 m/s to 20 m/s in 5 seconds. Its acceleration is 5 s(20−10) m/s=2 m s−2.
Graphical analysis of motion
Distance–time graph:
gradient = speed. A straight line indicates constant speed; a curved line indicates changing speed (acceleration).
Speed–time graph:
gradient = acceleration. A horizontal line means constant speed (zero acceleration).
area under the graph = displacement.
Example: A speed-time graph with a trapezoidal shape (initial speed u, final speed v, time t) has area = 21(u+v)t, which is the displacement.
Special results and concepts
Free-fall near the Earth's surface: acceleration due to gravity (g) is constant ≈10 m s−2 (approximate value used in the notes, more precisely 9.81 m s−2).
Terminal velocity: when air resistance equals weight, net force is zero and acceleration becomes zero; velocity becomes constant. This occurs for falling objects in a fluid (e.g., skydiver).
Examples from the notes
Example 2.1 (car path O to D): Imagine a car travels along a semi-circular path from point O to point D. If the path length is 314 m, this is the distance. If the straight-line distance from O to D is 200 m directly East, this is the car's displacement (200 m East).
Example 2.4–2.6: These examples involve calculating displacement from velocity-time graphs. For instance, if a car accelerates uniformly from rest to 20 m/s in 10 s, the displacement is the area of the triangle: 21×10 s×20 m/s=100 m. If it then brakes to a stop, the negative gradient (deceleration) would be calculated, and the area under that part of the graph (a triangle or trapezium) would be the displacement during braking.
Topic 3: Dynamics
Force and motion
A force is a push or pull, measured in newtons (N).
Contact force (normal force) upwards balances weight in contact with a surface. E.g., a book on a table experiences an upward normal force from the table.
Free body diagrams are used to represent forces on an object. All forces acting on the object are drawn as arrows from its center of mass.
Newton’s Laws
First Law (equilibrium): A body at rest or moving with constant velocity experiences no resultant force.
Example: A book lying still on a table, or a satellite moving at constant velocity in space far from gravitational influences.
Second Law: Resultant force equals mass times acceleration:
Fnet=ma
Example: A 10 kg block is pushed by a 20 N force. Its acceleration is a=F/m=20 N/10 kg=2 m s−2.
Third Law: For every action, there is an equal and opposite reaction.
Example: When you push against a wall (action force), the wall pushes back on you with an equal and opposite force (reaction force).
Balanced vs. unbalanced forces
Balanced: net force = 0 N → no change in motion (object remains at rest or moves with constant velocity).
Example: A car cruising at a steady speed on a flat road, where engine thrust equals air resistance and friction.
Unbalanced: net force =0→ acceleration occurs (velocity changes).
Example: A car accelerating from rest, where engine thrust is greater than resistive forces.
Friction
Friction opposes motion between surfaces in contact. It depends on the nature of the surfaces and the normal force.
Advantages: enables walking, braking in vehicles, holding objects, starting a car (tires grip the road).
Disadvantages: causes wear and energy loss (e.g., heat in engine parts); requires more energy to move objects on rough surfaces.
Ways to overcome friction: lubricants (e.g., oil in engines), ball bearings (in wheels), smoother surfaces (polishing).
Dynamics examples
Example 3.2: Pulling a block: A 50 N weight (mass m=50 N/10 m s−2=5 kg) is on a rough surface. A horizontal applied force F1=12 N pulls it, and friction f=2 N opposes it.
The horizontal resultant force = F1−f=12 N−2 N=10 N.
The acceleration a=Fnet/m=10 N/5 kg=2 m s−2.
Example 3.3: Circular motion: An object moving in a circle at constant speed experiences centripetal acceleration toward the center of the circle. This acceleration is caused by a resultant force (centripetal force) also directed toward the center. This force is often provided by tension in a string, gravity, or friction.
Example 3.4: Skydiver: A skydiver initially has weight Q greater than air resistance P, so they accelerate downwards. As their speed increases, P increases until eventually P = Q. At this point, the net force is zero, and the skydiver reaches terminal velocity.
Topic 4: Mass, Weight and Density
Mass
A measure of the amount of substance in a body; SI unit: kg; scalar quantity; depends on size and constituent atoms.
Mass is an intrinsic property of an object and does not change with location.
Inertia
The resistance of a body to changes in its state of rest or motion; proportional to mass. A more massive object has greater inertia and is harder to accelerate or decelerate.
Gravitational field strength (g)
Defined as gravitational force per unit mass: g=mF (near the Earth’s surface ≈9.8 N kg−1, often approximated as 10 N kg−1 for calculations).
Example: On the Moon, g≈1.6 N kg−1, so an object weighs less there.
Weight (W)
Gravitational force on a body: W=mg.
Compared to mass: mass is intrinsic; weight depends on location (gravitational field). E.g., a person with a mass of 70 kg has a weight of 70 kg×9.8 N kg−1=686 N on Earth, but only 70 kg×1.6 N kg−1=112 N on the Moon.
Density (ρ)
Defined as mass per unit volume: ρ=Vm; SI unit: kg m−3. (Also commonly g cm−3).
Example: A block of material has a mass of 500 g and a volume of 200 cm3. Its density is 500 g/200 cm3=2.5 g cm−3.
Buoyancy: an object floats if its density is less than the surrounding liquid (e.g., wood in water, since ρ<em>wood<ρ</em>water). An object sinks if more dense (e.g., a rock in water, since ρ<em>rock>ρ</em>water).
Topic 5: Turning Effect of Forces
Moment of a force (torque)
Turning effect about a pivot: Moment=F×d where d is the perpendicular distance from pivot to line of action of the force.
SI unit of moment: N m.
Example: A 10 N force applied at the end of a 0.5 m spanner, perpendicular to the spanner, creates a moment of 10 N×0.5 m=5 N m.
Equilibrium and the Principle of Moments
For an object in equilibrium (at rest or constant angular velocity):
The sum of clockwise moments about any point equals the sum of anticlockwise moments about that point: sum of moments = 0.
Example: A uniform plank of length 2 m and weight 20 N is pivoted at its center. If a 10 N weight is placed 0.5 m from the pivot on one side, a 10 N force needs to be applied 0.5 m from the pivot on the other side to keep it balanced (10 N×0.5 m clockwise = 10 N×0.5 m anticlockwise).
Centre of Gravity (C.G.)
The point where the whole weight appears to act.
The C.G. can lie outside the object, depending on shape.
Example: For a ring or a hollow cylinder, the C.G. is in the empty space at the center. For an L-shaped object, the C.G. is typically outside the material itself.
Its position influences stability.
Stability
Stability is the ability of an object to return to its original position after a small displacement.
Stability criteria depend on base area, height of the centre of gravity, and contact area with the surface.
Ways to improve stability
Lower the center of gravity. (e.g., racing cars have very low C.G.).
Increase the base area. (e.g., the wide base of a pyramid makes it very stable).
Topic 6: Pressure
Pressure definition
Pressure = Force / Area; units: Pascal (Pa) = N m−2.
Example: A 100 N force applied over an area of 0.1 m2 creates a pressure of 100 N/0.1 m2=1000 Pa.
Liquid pressure and hydrostatics
Pressure at depth in a liquid: P=P<em>0+ρgh, where P</em>0 is atmospheric pressure, ρ is liquid density, g is gravitational field strength, and h is fluid depth.
In a liquid at rest, pressure is the same along any horizontal line (same depth). This is why water finds its own level.
Example: The pressure at a depth of 5 m in water (ρ=1000 kg m−3, g=10 N kg−1) is P=P<em>0+(1000×10×5)=P</em>0+50000 Pa.
Transmission of pressure in hydraulic systems
Incompressible fluid in a container transmits pressure in all directions (Pascal's Principle).
Basic hydraulic relation: A</em>1F<em>1=A</em>2F<em>2 when pistons areas are A1 and A2 and F1, F2 are the respective forces.
This principle allows lifting heavy loads using hydraulic systems (e.g., car jacks, hydraulic brakes).
Example: If F<em>1=10 N is applied to a piston with area A</em>1=0.01 m2, the pressure is 1000 Pa. If this pressure acts on a larger piston with area A<em>2=1 m2, the output force F</em>2=P×A2=1000 Pa×1 m2=1000 N, allowing a small force to generate a large force.
Atmospheric pressure
Pressure exerted by the weight of air: measured with mercury barometer.
At sea level, standard atmosphere corresponds to 760 mm Hg (≈1.01×105 Pa).
Manometer
Instrument to measure gas pressure differences; uses height difference h and density ρ of the manometer liquid: P<em>1=P</em>0+ρgh (if the gas pressure P<em>1 is greater than atmospheric pressure P</em>0 and pushes the liquid column down on its side).
Example: If a gas creates a height difference of 10 cm (0.1 m) in a mercury manometer (ρHg=13600 kg m−3), the gauge pressure is ρgh=13600×10×0.1=13600 Pa.
Topic 7: Energy, Work and Power
Forms of energy
Kinetic energy (KE), elastic potential energy, gravitational potential energy (GPE), chemical potential energy, thermal energy, electrical energy, nuclear energy, etc.
Conservation of energy
The total energy in a closed system remains constant; energy converts between forms without net loss.
Example: A falling object converts GPE to KE; a pendulum converts GPE to KE and back.
Kinetic energy and potential energy
KE: KE=21mv2
Example: A 2 kg object moving at 5 m/s has KE=21×2×52=25 J.
GPE (reference at Earth’s surface): U=mgh
Example: A 2 kg object raised 3 m above the ground (g=10 N kg−1) has U=2×10×3=60 J.
Work and power
Work done by a force: W=Fs (displacement in the direction of the force). If the force is not parallel to displacement, W=Fscosθ.
Power: P=tW; SI unit: W = J s−1.
Example: A 50 N force pushes a box 10 m in 5 seconds. Work done = 50 N×10 m=500 J. Power = 500 J/5 s=100 W.
Efficiency
Efficiency of energy conversion: η=total input energyuseful output energy×100%. Also, η=total input poweruseful output power×100%.
Example: A light bulb uses 100 J of electrical energy and produces 5 J of light energy. Its efficiency is 100 J5 J×100%=5%.
Topic 8: Kinetic Model of Matter
States of matter (qualitative comparison)
Solids: definite volume and shape; particles vibrate about fixed positions; densest (generally); strong inter-molecular forces.
Liquids: definite volume, take shape of container; particles can flow past each other; moderate forces; less dense than solids (generally).
Gases: no definite volume or shape; particles far apart; negligible intermolecular forces; compressible; move freely and randomly; least dense.
Brownian motion
Random, irregular motion of microscopic particles suspended in fluids due to collisions with fast-moving, invisible fluid molecules.
Example: Smoke particles observed under a microscope moving erratically due to collisions with air molecules.
Gas pressure and molecular model
Gas pressure arises from molecules colliding with container walls; increasing number of molecules, their speeds (related to temperature), or molecular mass increases pressure.
Gas relationships (qualitative gas laws)
For a fixed amount of gas at constant volume, increasing temperature increases pressure (P ∝ T) (Gay-Lussac's Law).
For a fixed mass of gas at constant pressure, increasing temperature increases volume (V ∝ T) (Charles's Law).
For a fixed mass of gas at constant temperature, increasing volume decreases pressure (P ∝ 1/V) (Boyle's Law).
These lead to the relation P<em>1V</em>1=P<em>2V</em>2 when T is constant, etc. (Combined Gas Law: T<em>1P<em>1V</em>1=T</em>2P</em>2V<em>2).
Example (Boyle's Law): A gas at 1 atm has a volume of 10 L. If its volume is compressed to 5 L at constant temperature, its new pressure will be 2 atm ($1 \times 10 = P2 \times 5 \implies P2 = 2$).
Topic 9: Transfer of Thermal Energy
Three modes of heat transfer
Conduction: through direct contact; particles transfer energy by vibrating against neighbors. Metals are good conductors due to free electrons; liquids/gases are poor conductors.
Example: A metal spoon quickly gets hot when placed in hot soup.
Convection: in fluids (liquids and gases); warmer, less dense regions rise and cooler, denser regions sink, setting up currents.
Example: Boiling water in a pot (hot water rises, cool water sinks); sea breezes and land breezes created by differential heating of land and sea.
Radiation: transfer of energy by electromagnetic waves (infrared); does not require a medium and can travel through a vacuum; rate affected by colour/texture/area.
Example: Feeling the heat from a distant campfire; the Sun's energy reaching Earth.
Applications
Greenhouses trap solar radiation; cooking utensils made of good conductors; insulating flasks minimize heat transfer.
Vacuum flask
Optimally reduces heat transfer by all three modes:
Vacuum between double walls: eliminates conduction and convection.
Silvered/reflective inner surfaces: minimize heat transfer by radiation.
Stopper (cork/plastic): reduces heat loss by conduction and convection through the opening.
Topic 10: Temperature
Temperature and scales
Temperature measured in Kelvin (K); relation to Celsius: θ<em>K=θ</em>∘C+273.15. Absolute zero (0 K or −273.15∘C) is the lowest possible temperature.
Example:20∘C is equivalent to 20+273.15=293.15 K.
Measurement and thermometric properties
Thermometric properties used for temperature scales include:
Volume changes of liquids, e.g., mercury/alcohol. These expand uniformly with temperature.
EMF between different metals (thermocouples). The voltage produced depends on the temperature difference.
Resistance of metals (e.g., platinum resistance thermometers). Resistance typically increases with temperature.
Common thermometers and ranges
Mercury/alcohol thermometers (common for everyday use; alcohol used for lower temperatures);
Thermocouples (wide range, fast response, e.g., for furnaces or engines);
Fixed points (ice point 0∘C, steam point 100∘C at standard atmospheric pressure) are used for calibration.
Temperature calibration
Ice point (0∘C) and steam point (100∘C) serve as fixed points; the range between these points is subdivided into 100 equal divisions for the Celsius scale.
Thermocouples
Two junctions of dissimilar metals at different temperatures; voltages produced depend on temperature difference.
Advantages: wide range, robustness, small size, fast response, measurement at a point.
Example: Used to measure very high temperatures in industrial ovens where liquid-in-glass thermometers would melt.
Topic 11: Thermal Properties of Matter
Internal energy
Sum of kinetic and potential energies of molecules within a substance; increases with temperature rise.
For an ideal gas, internal energy is purely kinetic.
Heat capacity and specific heat capacity
Heat capacity: the energy required to raise the temperature of the substance by 1∘C (or 1 K): C with units J ∘C−1 or J K−1.
Specific heat capacity: energy required to raise the temperature of 1 kg of substance by 1∘C (or 1 K): c with units J kg−1∘C−1 or J kg−1 K−1.
Formulas:
Q=CΔθ
Q=mcΔθ
Example: To raise the temperature of 2 kg of water (cwater=4200 J kg−1∘C−1) by 10∘C requires Q=2×4200×10=84000 J.
Latent heat and phase changes
Latent heat is the energy absorbed or released during a phase change (e.g., melting, boiling) without a change in temperature.
Latent heat of fusion (melting/solidification): Q=mL<em>f (L</em>f is specific latent heat of fusion).
Latent heat of vaporisation (boiling/condensation): Q=mL<em>v (L</em>v is specific latent heat of vaporisation).
Melting/solidification and boiling/condensation occur at constant temperature (plateaus on heating/cooling curves) while energy is absorbed or released to break/form intermolecular bonds.
Example: To melt 1 kg of ice at 0∘C (Lf=3.34×105 J kg−1)) requires Q=1×3.34×105=334000 J. The temperature remains 0∘C during this process.
Types of internal energy by state
Solid: mainly vibrational kinetic + potential energy (due to fixed positions in a lattice).
Liquid: translational kinetic + potential energy (particles can move past each other).
Gas: mainly translational kinetic energy (particles are far apart, so potential energy due to intermolecular forces is negligible).
Cooling curves
Illustrate temperature vs. time during cooling/heating, showing plateaus during phase changes. For a pure substance, the phase change occurs at a sharp, constant temperature. For a mixture, the phase change occurs over a range of temperatures.
Topic 12: General Wave Properties
Wave motion and energy transfer
Waves involve oscillations that transfer energy without transferring matter.
Mechanical waves require a medium (e.g., sound waves, water waves); electromagnetic waves do not require a medium and can travel in vacuum (e.g., light waves).
Transverse waves (e.g., light) have oscillations perpendicular to wave propagation. Longitudinal waves (e.g., sound) have oscillations parallel to wave propagation.
Key quantities
Speed (v): how fast the wave travels through the medium.
Frequency (f): number of oscillations per second (Hz).
Wavelength (λ): distance between two consecutive identical points on a wave.
Period (T): time for one complete oscillation (T=1/f).
Amplitude (a): maximum displacement of a particle from its rest position.
Relationship: v=fλ
Data is often represented as wavefronts (plane or circular) and as sine curves for displacement vs. time or vs. distance.
Example: A sound wave with frequency 100 Hz in air (where v≈330 m/s) has a wavelength λ=v/f=330/100=3.3 m.
Wavefronts
A wavefront is a locus of points in phase; circular (near a point source) and plane (far from the source).
Topic 13: Light
Reflection
Law: angle of incidence i equals angle of reflection r, with the incident ray, reflected ray, and normal all in the same plane.
Normal: imaginary line perpendicular to the reflecting surface at the point of incidence.
Example: If a light ray hits a plane mirror at an angle of 30∘ to the normal, it will reflect at 30∘ to the normal.
Refraction
Snell’s Law: n<em>1sini=n</em>2sinr where n is the refractive index of the medium.
Refractive index definition: n=vc where c is the speed of light in vacuum (≈3×108 m s−1) and v is the speed in the medium.
Critical angle and total internal reflection: when light travels from a denser to a less dense medium, if the angle of incidence exceeds the critical angle (i > c), refraction ceases and total internal reflection occurs.
Example: Light entering water (n<em>water=1.33) from air (n</em>air=1) with an angle of incidence of 45∘. (1)sin45∘=(1.33)sinr⟹sinr=(sin45∘)/1.33≈0.5317⟹r≈32.1∘.
Lenses and ray diagrams
Thin lenses: converging (convex, thicker in middle, focuses parallel rays to a focal point) and diverging (concave, thinner in middle, spreads parallel rays as if from a focal point).
Focal length f, optical centre C, principal axis, ray diagrams show how rays refract.
Real images (can be projected on a screen) and virtual images (cannot be projected, seen through the lens), magnification, and applications (e.g., telescope, camera, projector, magnifying glass).
Example: A converging lens can form a real, inverted image when the object is placed beyond the focal point, or a virtual, upright, magnified image (like a magnifying glass) when the object is within the focal point.
Optical fibres
Utilize total internal reflection to transmit light with advantages: high data capacity, low interference, secure transmission, and flexibility.
Topic 14: Electromagnetic Spectrum
Electromagnetic waves (EM waves)
All EM waves are transverse and travel at the speed of light in vacuum: c≈3×108 m s−1.
Propagation does not require a medium; can travel in vacuum.
Spectrum components (order of magnitude of wavelength and basic uses)
Organized by decreasing wavelength (increasing frequency/energy):
Radio waves: Longest wavelength (∼103 m-10−1 m). Uses: broadcasting, communication, radar.
Microwaves: (∼10−1 m-10−3 m). Uses: cooking (microwave ovens), satellite communication, mobile phones.
Infrared (IR): (∼10−3 m-7×10−7 m). Uses: remote controls, thermal imaging, optical fibres (heat), night vision, heating.
Visible light: (∼7×10−7 m-(red) to 4×10−7 m(violet)). Uses: human vision, optical fibres, lasers, photography.
X-rays: (∼10−8 m-10−12 m). Uses: medical imaging (radiography), security scans, crystallography.
Gamma rays (γ): Shortest wavelength (\sim <10^{-12}\text{ m}). Uses: sterilisation of medical equipment/food, cancer treatment (radiotherapy).
Effects and hazards of EM radiation
Heating (IR, microwaves) and ionisation effects (UV, X-rays, gamma rays).
Higher frequency waves tend to be more energetic and potentially hazardous (e.g., ionising radiation can cause cell damage and cancer).
Topic 15: Sound
Production and nature
Sound is produced by vibrating sources (e.g., vocal cords, guitar strings, speakers).
Longitudinal waves that require a medium for propagation (cannot travel in a vacuum).
Medium and speed of sound
Speed of sound depends on the medium and its temperature/density:
Solids > Liquids > Gases (sound travels fastest in solids, slowest in gases).
Example: Speed of sound in air ≈330−340 m/s, in water ≈1500 m/s, in steel ≈5000 m/s.
Amplitude and frequency
Loudness is related to amplitude (larger amplitude means louder sound).
Pitch is related to frequency (higher frequency means higher pitch).
(v=fλ); for a constant speed, higher frequency means shorter wavelength and higher pitch.
Determining the speed of sound in air
A basic method uses a timing apparatus and a known distance (e.g., firing a starting pistol at one end of a field, and a timer at the other end measures the time delay between seeing the flash and hearing the sound, then v=distance/time).
Echoes
Sound waves reflecting off a surface. Distance measurement using echoes: time delay corresponds to twice the distance to the reflecting surface.
2d=vΔt⟹d=2vΔt
Example: If an echo from a cliff is heard 4 seconds after a shout, and the speed of sound in air is 340 m/s, the distance to the cliff is d=(340×4)/2=680 m.
Ultrasound
Frequencies above 20 kHz (beyond human hearing range).
Uses include prenatal scanning (imaging unborn babies), detecting flaws in materials (e.g., cracks in metal pipes), medical therapeutic uses, sonar (imaging underwater objects).
Topic 16: Static Electricity
Electric charges
Charges are either positive (+) or negative (-); like charges repel, unlike charges attract.
Charge magnitude is measured in coulombs (C).
The total charge Q relates to number of electrons N via: Q=Ne where e is the elementary charge (e=1.6×10−19 C for a single electron).
Charge transfer and rubbing
Rubbing (charging by friction) transfers electrons from one material to another, resulting in both objects becoming oppositely charged; nuclei do not move.
Insulators (e.g., plastic, glass) tend to retain charges on surfaces where they are generated.
Conductors (e.g., metals) allow charge redistribution across their surface.
Example: Rubbing a plastic rod with a cloth transfers electrons from the cloth to the rod, making the rod negatively charged and the cloth positively charged.
Electric field
An electric field is a region in which a unit positive charge experiences a force. It is a force field.
Field is a vector quantity; electric field lines indicate the direction of force on a positive test charge. Field lines originate from positive charges and terminate on negative charges.
Electric field patterns
Field patterns around isolated point charges (radial, outwards from positive, inwards to negative).
Field patterns between two point charges (like charges repel, field lines push away; opposite charges attract, field lines connect).
Uniform fields exist between parallel charged plates (parallel, equally spaced field lines).
Hazards and applications
Hazards: lightning (large-scale static discharge), electric shocks from charged objects.
Applications: induction charging (charging without contact), photocopying processes (toner particles attracted to charged drum), electrostatic spray painting (charged paint particles are attracted to the object being painted).
Topic 17: Current of Electricity
Conventional current vs electron flow
Conventional current: positive charge flow direction (from positive terminal to negative terminal, historical convention).
Electron flow: actual charge carriers are electrons moving opposite to the conventional current (from negative terminal to positive terminal).
Charge, current and time
Charge: Q=It, with current I (in Amperes, A) and time t (in seconds, s).
Example: A current of 2 A flows for 10 s. The total charge passed is Q=2 A×10 s=20 C.
Electromotive force (e.m.f., emf)
The work done by a source (e.g., battery) to move unit charge around a complete circuit: W=QV
V is emf (in volts, V). Unit: J/C.
For a series of sources, total emf adds; for parallel, it depends on configuration.
Potential difference (p.d.)
PD across a component is the work done to move unit charge across that component: V=QW or simply the potential drop across the component in a circuit.
It is the energy converted from electrical to other forms (heat, light) per unit charge.
Resistance and Ohm’s Law
Resistance: R=IV (Unit: Ohm, Ω).
Ohm’s Law: a linear conductor at constant temperature obeys V ∝ I (current is directly proportional to potential difference); plot of I–V is a straight line for ohmic conductors.
Non-ohmic: filament lamp has increasing resistance with increasing current due to temperature rise (it gets hotter, resistance increases, so I-V graph curves).
Example: A resistor with 12 V across it draws 2 A of current. Its resistance is R=12 V/2 A=6Ω.
Components: diodes and LDR
Diode: semiconductor device that allows current to flow in one direction only (forward bias) and blocks it in the reverse direction (rectification); nonlinear I–V characteristic.
LDR (Light-Dependent Resistor / photoresistor): resistance decreases with increasing light intensity; used in automatic lighting circuits (e.g., street lights, night lights).
Topic 18: D.C. Circuits
Basic circuit rules
Current in a series circuit is the same at all points.
The sum of the potential differences in a series circuit equals the emf of the source: V=V<em>1+V</em>2+⋯ (Kirchhoff's Voltage Law).
In parallel circuits, the current splits (total current is sum of branch currents); the potential difference across each branch is the same.
A uniform wire (or series of resistors) connected to a voltage source can act as a variable resistor to provide a fraction of the supply voltage; VPW (voltage across part of the wire/resistor) depends on the position along the resistor.
The output voltage is given by V<em>out=V</em>in(R</em>1+R2R<em>2).
Example: A 12 V supply across two series resistors, R<em>1=200Ω and R</em>2=100Ω. The voltage across R<em>2 is V</em>R2=12 V(200+100100)=12 V×31=4 V.
Thermistors and LDRs as inputs
Temperature-dependent (thermistors) or light-dependent (LDRs) resistance changes used in potential dividers for sensing.
Example: In a temperature sensor, a thermistor's resistance decreases with increasing temperature. If placed as R<em>2 in a potential divider, the output voltage (V</em>R2) would decrease as temperature rises, triggering a fan or alarm.
Topic 19: Practical Electricity
Heating effects of electricity
Electrical energy can be converted to heat in resistors (heating elements).
Common materials: Nichrome due to high resistivity and high melting point. Used in toaster elements, electric kettles, hair dryers.
Energy and power relations for appliances
Work/energy: W=VIt (electrical energy converted).
Power: P=VI (rate of energy conversion); alternative forms: P=I2R; P=V2/R.
Example: A 240 V heater draws 10 A of current. Its power is P=240×10=2400 W. In 1 hour ($3600\text{ s}$), it uses W=2400×3600=8.64×106 J.
Cost of electricity
Cost = energy used (kWh) × price per kWh; 1 kWh = 3.6×106 J.
Example: If electricity costs 0.20perkWh,andanapplianceuses2.4kWh,thecostis2.4 \times 0.20 = $0.48$.
Hazards and safety
Damp conditions increase conductivity and risk of shock.
Damaged insulation exposes live wires.
Overheating cables can cause fires (due to too much current, I2R heating).
Multiple plug outlets can overload circuits, leading to overheating.
Fuses and circuit breakers protect circuits; earthing provides safety for metal casings.
Live, neutral, and earth wires: live is dangerous (carries fluctuating voltage); neutral is at/near earth potential (completes circuit); earth provides a low-resistance path to ground for fault currents, preventing electrocution.
Electrical wiring and safety devices
Switches are always placed on the live wire to break the circuit fully when turned off.
Fuses are rated for expected current; they melt and break the circuit if current exceeds safe limits.
Double insulation (plastic casing) provides protection without needing an earth wire for appliances.
Earthing connects metal casings of appliances to the ground, so if the live wire touches the casing, current flows to earth and blows the fuse.
Topic 20: Magnetism
Properties of magnets
Two poles (North and South); magnets do not exist as monopoles (if cut, new poles form).
Like poles repel; unlike poles attract.
Magnetic dipoles can be represented by arrows indicating orientation.
Induced magnetism
A magnetic material (e.g., iron, steel) becomes magnetised when placed in a magnetic field; domains (regions of aligned atomic magnets) within the material align to produce induced magnetisation.
Example: A paper clip becomes temporarily magnetic when held near a strong magnet and can then pick up other paper clips.
Magnetisation using electricity
A steel bar can be magnetised by placing it in a solenoid connected to a DC source (electromagnetism); the direction of current determines the pole orientation (use right-hand grip rule).
Magnetic materials and magnets
Common magnetic materials: iron, steel, nickel, cobalt (ferromagnetic materials).
Temporary (soft) magnets (e.g., soft iron): easily magnetised and demagnetised. Used in electromagnets, relays.
Permanent magnets (e.g., steel, alnico): hard to magnetise but retain magnetism strongly. Used in compasses, speakers, motors.
Electromagnets vs permanent magnets
Electromagnet: coil of wire with soft iron core; magnetism is temporary and requires current to sustain (can be turned on/off).
Permanent magnets: magnetism persists without current; used in compasses, motors, dynamos, door catches, speakers.
Magnetic field and field lines
Magnetic field lines show the direction of the magnetic force (from N to S outside the magnet, S to N inside); strength is indicated by line density (closer lines mean stronger field).
Field patterns and effects
Field patterns between bar magnets show attraction/repulsion interactions depending on pole orientation.
Example: Two North poles facing each other will have field lines pushing away from each other, illustrating repulsion.
Topic 21: Electromagnetism
Magnetic fields around currents
A current-carrying wire produces a magnetic field; the pattern depends on the geometry of the conductor.
Straight Wire: Concentric circles around the wire. Direction using Right-Hand Grip Rule (thumb in current direction, fingers show field direction).