O Level Physics Topical Revision Notes

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) 101210^{12}
    • Giga (G) 10910^{9}
    • Mega (M) 10610^{6}
    • Kilo (k) 10310^{3}
    • Deci (d) 10110^{-1}
    • Centi (c) 10210^{-2}
    • Milli (m) 10310^{-3}
    • Micro (µ) 10610^{-6}
    • Nano (n) 10910^{-9}
    • Pico (p) 101210^{-12}
    • The syllabus highlights the bolded ones (the ones listed above).
    • Example: Converting 5 km to meters: 5 km=5×103 m5 \text{ km} = 5 \times 10^3 \text{ m}. Converting 200 mA to Amperes: 200 mA=200×103 A=0.2 A200 \text{ mA} = 200 \times 10^{-3} \text{ A} = 0.2 \text{ A}.
  • Orders of magnitude and estimation
    • Used to compare sizes from atomic scales to astronomical scales.
    • Examples:
    • Diameter of an atom: 1010 m10^{-10} \text{ m}
    • Thickness of human hair: 105 m10^{-5} \text{ m}
    • Height of a human: 100 m10^0 \text{ m} (or ~1 meter)
    • Diameter of Earth: 107 m10^7 \text{ m}
    • Distance to the Sun: 1011 m10^{11} \text{ 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/s2^2 upwards, force = 20 N at 3030^\circ from horizontal).
  • Addition of vectors (graphical and analytical)
    • Resultant R of two perpendicular vectors F1 and F2:
    • Magnitude: R=F<em>12+F</em>22R = \sqrt{F<em>1^2 + F</em>2^2}
    • Direction: tanθ=F<em>1F</em>2\tan\theta = \frac{F<em>1}{F</em>2} (angle above the horizontal, for example)
    • Example: A force F<em>1=3 NF<em>1 = 3\text{ N} acting East and a force F</em>2=4 NF</em>2 = 4\text{ N} acting North.
    • The resultant magnitude R=32+42=9+16=25=5 NR = \sqrt{3^2 + 4^2} = \sqrt{9 + 16} = \sqrt{25} = 5\text{ N}.
    • The direction θ=tan1(43)53.1\theta = \tan^{-1}\left(\frac{4}{3}\right) \approx 53.1^\circ 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\pm 0.1\text{ cm}). Used for lengths from a few cm to several meters.
    • Micrometers (typically ±0.01 mm\pm 0.01\text{ mm}) and vernier calipers (typically ±0.01 cm\pm 0.01\text{ 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\pm 0.01\text{ cm}.
    • Jaws: external jaws measure external dimensions; internal jaws measure internal dimensions; tail measures depth.
    • 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 mm3.5 \text{ mm} + 0.25 \text{ mm} = 3.75 \text{ 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=2πlgT = 2\pi \sqrt{\frac{l}{g}}
    • Note: This formula is for small angles of oscillation (<10^\circ).
    • Example: A pendulum with length l=0.99 ml = 0.99\text{ m} on Earth (g9.81 m s2g \approx 9.81\text{ m s}^{-2}) will have a period T=2π0.999.812.00 sT = 2\pi \sqrt{\frac{0.99}{9.81}} \approx 2.00\text{ 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=distance travelledt\text{speed} = \frac{\text{distance travelled}}{t}
    • Average speed: vavg=Total distance travelledTotal time takenv_{\text{avg}} = \frac{\text{Total distance travelled}}{\text{Total time taken}}
    • Velocity: rate of change of displacement; average velocity: vavg=ΔxΔtv_{\text{avg}} = \frac{\Delta x}{\Delta t} (where Δx\Delta x is displacement and Δt\Delta t is time interval).
    • Example: A car travels 100 km in 2 hours. Its average speed is 100 km/2 h=50 km/h100\text{ km} / 2\text{ h} = 50\text{ km/h}.
  • Acceleration
    • Acceleration: a=ΔvΔta = \frac{\Delta v}{\Delta t} (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 (2010) m/s5 s=2 m s2\frac{(20 - 10)\text{ m/s}}{5\text{ s}} = 2\text{ 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 = 12(u+v)t\frac{1}{2}(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 s2\approx 10\text{ m s}^{-2} (approximate value used in the notes, more precisely 9.81 m s29.81\text{ 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 East200\text{ 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: 12×10 s×20 m/s=100 m\frac{1}{2} \times 10\text{ s} \times 20\text{ m/s} = 100\text{ 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\mathbf{F}_{\text{net}} = m\mathbf{a}
    • Example: A 10 kg block is pushed by a 20 N force. Its acceleration is a=F/m=20 N/10 kg=2 m s2a = F/m = 20\text{ N} / 10\text{ kg} = 2\text{ 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 \rightarrow 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\neq 0 \rightarrow 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 s2=5 kgm = 50\text{ N} / 10\text{ m s}^{-2} = 5\text{ kg}) is on a rough surface. A horizontal applied force F1=12 NF_1 = 12\text{ N} pulls it, and friction f=2 Nf = 2\text{ N} opposes it.
    • The horizontal resultant force = F1f=12 N2 N=10 NF_1 - f = 12\text{ N} - 2\text{ N} = 10\text{ N}.
    • The acceleration a=Fnet/m=10 N/5 kg=2 m s2a = F_{\text{net}}/m = 10\text{ N} / 5\text{ kg} = 2\text{ 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=Fmg = \frac{F}{m} (near the Earth’s surface 9.8 N kg1\approx 9.8\text{ N kg}^{-1}, often approximated as 10 N kg110\text{ N kg}^{-1} for calculations).
    • Example: On the Moon, g1.6 N kg1g \approx 1.6\text{ N kg}^{-1}, so an object weighs less there.
  • Weight (W)
    • Gravitational force on a body: W=mgW = 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 kg1=686 N70\text{ kg} \times 9.8\text{ N kg}^{-1} = 686\text{ N} on Earth, but only 70 kg×1.6 N kg1=112 N70\text{ kg} \times 1.6\text{ N kg}^{-1} = 112\text{ N} on the Moon.
  • Density (ρ\rho)
    • Defined as mass per unit volume: ρ=mV\rho = \frac{m}{V}; SI unit: kg m3^{-3}. (Also commonly g cm3^{-3}).
    • Example: A block of material has a mass of 500 g and a volume of 200 cm3^3. Its density is 500 g/200 cm3=2.5 g cm3500\text{ g} / 200\text{ cm}^3 = 2.5\text{ 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\rho<em>{\text{wood}} < \rho</em>{\text{water}}). An object sinks if more dense (e.g., a rock in water, since ρ<em>rock>ρ</em>water\rho<em>{\text{rock}} > \rho</em>{\text{water}}).
Topic 5: Turning Effect of Forces
  • Moment of a force (torque)
    • Turning effect about a pivot: Moment=F×d\text{Moment} = F \times 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 m10\text{ N} \times 0.5\text{ m} = 5\text{ 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 m10\text{ N} \times 0.5\text{ m} clockwise = 10 N×0.5 m10\text{ N} \times 0.5\text{ 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 m2^{-2}.
    • Example: A 100 N force applied over an area of 0.1 m20.1\text{ m}^2 creates a pressure of 100 N/0.1 m2=1000 Pa100\text{ N} / 0.1\text{ m}^2 = 1000\text{ Pa}.
  • Liquid pressure and hydrostatics
    • Pressure at depth in a liquid: P=P<em>0+ρghP = P<em>0 + \rho gh, where P</em>0P</em>0 is atmospheric pressure, ρ\rho is liquid density, gg is gravitational field strength, and hh 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 m3\rho = 1000\text{ kg m}^{-3}, g=10 N kg1g = 10\text{ N kg}^{-1}) is P=P<em>0+(1000×10×5)=P</em>0+50000 PaP = P<em>0 + (1000 \times 10 \times 5) = P</em>0 + 50000\text{ Pa}.
  • Transmission of pressure in hydraulic systems
    • Incompressible fluid in a container transmits pressure in all directions (Pascal's Principle).
    • Basic hydraulic relation: F<em>1A</em>1=F<em>2A</em>2\frac{F<em>1}{A</em>1} = \frac{F<em>2}{A</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 NF<em>1 = 10\text{ N} is applied to a piston with area A</em>1=0.01 m2A</em>1 = 0.01\text{ m}^2, the pressure is 1000 Pa1000\text{ Pa}. If this pressure acts on a larger piston with area A<em>2=1 m2A<em>2 = 1\text{ m}^2, the output force F</em>2=P×A2=1000 Pa×1 m2=1000 NF</em>2 = P \times A_2 = 1000\text{ Pa} \times 1\text{ m}^2 = 1000\text{ 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\approx 1.01 \times 10^5\text{ Pa}).
  • Manometer
    • Instrument to measure gas pressure differences; uses height difference h and density ρ\rho of the manometer liquid: P<em>1=P</em>0+ρghP<em>1 = P</em>0 + \rho gh (if the gas pressure P<em>1P<em>1 is greater than atmospheric pressure P</em>0P</em>0 and pushes the liquid column down on its side).
    • Example: If a gas creates a height difference of 10 cm (0.1 m0.1\text{ m}) in a mercury manometer (ρHg=13600 kg m3\rho_{\text{Hg}} = 13600\text{ kg m}^{-3}), the gauge pressure is ρgh=13600×10×0.1=13600 Pa\rho gh = 13600 \times 10 \times 0.1 = 13600\text{ 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=12mv2K_E = \frac{1}{2} m v^2
    • Example: A 2 kg object moving at 5 m/s has KE=12×2×52=25 JK_E = \frac{1}{2} \times 2 \times 5^2 = 25\text{ J}.
    • GPE (reference at Earth’s surface): U=mghU = m g h
    • Example: A 2 kg object raised 3 m above the ground (g=10 N kg1g = 10\text{ N kg}^{-1}) has U=2×10×3=60 JU = 2 \times 10 \times 3 = 60\text{ J}.
  • Work and power
    • Work done by a force: W=FsW = F s (displacement in the direction of the force). If the force is not parallel to displacement, W=FscosθW = Fs \cos\theta.
    • Power: P=WtP = \frac{W}{t}; SI unit: W = J s1^{-1}.
    • Example: A 50 N force pushes a box 10 m in 5 seconds. Work done = 50 N×10 m=500 J50\text{ N} \times 10\text{ m} = 500\text{ J}. Power = 500 J/5 s=100 W500\text{ J} / 5\text{ s} = 100\text{ W}.
  • Efficiency
    • Efficiency of energy conversion: η=useful output energytotal input energy×100%\eta = \frac{\text{useful output energy}}{\text{total input energy}} \times 100\%. Also, η=useful output powertotal input power×100%\eta = \frac{\text{useful output power}}{\text{total input power}} \times 100\%.
    • Example: A light bulb uses 100 J of electrical energy and produces 5 J of light energy. Its efficiency is 5 J100 J×100%=5%\frac{5\text{ J}}{100\text{ J}} \times 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 \propto T) (Gay-Lussac's Law).
    • For a fixed mass of gas at constant pressure, increasing temperature increases volume (V \propto T) (Charles's Law).
    • For a fixed mass of gas at constant temperature, increasing volume decreases pressure (P \propto 1/V) (Boyle's Law).
    • These lead to the relation P<em>1V</em>1=P<em>2V</em>2P<em>1V</em>1 = P<em>2V</em>2 when T is constant, etc. (Combined Gas Law: P<em>1V</em>1T<em>1=P</em>2V<em>2T</em>2\frac{P<em>1V</em>1}{T<em>1} = \frac{P</em>2V<em>2}{T</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\theta<em>K = \theta</em>{{^{\circ}\text{C}}} + 273.15. Absolute zero (0 K or 273.15C-273.15^{\circ}\text{C}) is the lowest possible temperature.
    • Example: 20C20^{\circ}\text{C} is equivalent to 20+273.15=293.15 K20 + 273.15 = 293.15\text{ 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 0C0^{\circ}\text{C}, steam point 100C100^{\circ}\text{C} at standard atmospheric pressure) are used for calibration.
  • Temperature calibration
    • Ice point (0C0^{\circ}\text{C}) and steam point (100C100^{\circ}\text{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 1C1^{\circ}\text{C} (or 1 K): CC with units J C1^{\circ}\text{C}^{-1} or J K1^{-1}.
    • Specific heat capacity: energy required to raise the temperature of 1 kg of substance by 1C1^{\circ}\text{C} (or 1 K): cc with units J kg1C1^{-1} {^{\circ}\text{C}^{-1}} or J kg1 K1^{-1}\text{ K}^{-1}.
    • Formulas:
    • Q=CΔθQ = C \Delta \theta
    • Q=mcΔθQ = m c \Delta \theta
    • Example: To raise the temperature of 2 kg of water (cwater=4200 J kg1C1c_{\text{water}} = 4200\text{ J kg}^{-1} {^{\circ}\text{C}^{-1}}) by 10C10^{\circ}\text{C} requires Q=2×4200×10=84000 JQ = 2 \times 4200 \times 10 = 84000\text{ 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>fQ = m L<em>f (L</em>fL</em>f is specific latent heat of fusion).
    • Latent heat of vaporisation (boiling/condensation): Q=mL<em>vQ = m L<em>v (L</em>vL</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 0C0^{\circ}\text{C} (Lf=3.34×105 J kg1)L_f = 3.34 \times 10^5\text{ J kg}^{-1})) requires Q=1×3.34×105=334000 JQ = 1 \times 3.34 \times 10^5 = 334000\text{ J}. The temperature remains 0C0^{\circ}\text{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\lambda): distance between two consecutive identical points on a wave.
    • Period (T): time for one complete oscillation (T=1/fT = 1/f).
    • Amplitude (a): maximum displacement of a particle from its rest position.
    • Relationship: v=fλv = f \lambda
    • 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 v330 m/sv \approx 330\text{ m/s}) has a wavelength λ=v/f=330/100=3.3 m\lambda = v/f = 330/100 = 3.3\text{ 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 3030^\circ to the normal, it will reflect at 3030^\circ to the normal.
  • Refraction
    • Snell’s Law: n<em>1sini=n</em>2sinrn<em>1 \sin i = n</em>2 \sin r where n is the refractive index of the medium.
    • Refractive index definition: n=cvn = \frac{c}{v} where c is the speed of light in vacuum (3×108 m s1\approx 3 \times 10^8\text{ 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=1.33n<em>{\text{water}} = 1.33) from air (n</em>air=1n</em>{\text{air}} = 1) with an angle of incidence of 4545^\circ. (1)sin45=(1.33)sinr    sinr=(sin45)/1.330.5317    r32.1(1) \sin 45^\circ = (1.33) \sin r \implies \sin r = (\sin 45^\circ) / 1.33 \approx 0.5317 \implies r \approx 32.1^\circ.
  • 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: c3×108 m s1c \approx 3 \times 10^8 \text{ 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\sim 10^3\text{ m}-101 m10^{-1}\text{ m}). Uses: broadcasting, communication, radar.
    • Microwaves: (101 m\sim 10^{-1}\text{ m}-103 m10^{-3}\text{ m}). Uses: cooking (microwave ovens), satellite communication, mobile phones.
    • Infrared (IR): (103 m\sim 10^{-3}\text{ m}-7×107 m7 \times 10^{-7}\text{ m}). Uses: remote controls, thermal imaging, optical fibres (heat), night vision, heating.
    • Visible light: (7×107 m\sim 7 \times 10^{-7}\text{ m}-(red) to 4×107 m4 \times 10^{-7}\text{ m}(violet)). Uses: human vision, optical fibres, lasers, photography.
    • Ultraviolet (UV): (4×107 m\sim 4 \times 10^{-7}\text{ m}-108 m10^{-8}\text{ m}). Uses: sterilisation, sunbeds, fluorescent lamps, detecting forged currency.
    • X-rays: (108 m\sim 10^{-8}\text{ m}-1012 m10^{-12}\text{ m}). Uses: medical imaging (radiography), security scans, crystallography.
    • Gamma rays (γ\gamma): 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 330340 m/s\approx 330-340\text{ m/s}, in water 1500 m/s\approx 1500\text{ m/s}, in steel 5000 m/s\approx 5000\text{ 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=fλv = f \lambda); 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/timev = \text{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=vΔt22d = v \Delta t \implies d = \frac{v \Delta t}{2}
    • 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 md = (340 \times 4) / 2 = 680\text{ 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=NeQ = N e where e is the elementary charge (e=1.6×1019 Ce = 1.6 \times 10^{-19} \text{ 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=ItQ = I t, 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 CQ = 2\text{ A} \times 10\text{ s} = 20\text{ 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=QVW = 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=WQV = \frac{W}{Q} 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=VIR = \frac{V}{I} (Unit: Ohm, Ω\Omega).
    • Ohm’s Law: a linear conductor at constant temperature obeys V \propto 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=6ΩR = 12\text{ V} / 2\text{ A} = 6 \Omega.
  • 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+V = V<em>1 + V</em>2 + \cdots (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.
  • Resistance in series and parallel
    • Series: Effective Resistance R<em>eff=R</em>1+R2+R<em>{\text{eff}} = R</em>1 + R_2 + \cdots
    • Example: Two resistors, 3Ω3 \Omega and 5Ω5 \Omega, in series have Reff=3+5=8ΩR_{\text{eff}} = 3 + 5 = 8 \Omega.
    • Parallel: 1/R<em>eff=1/R</em>1+1/R2+1/R<em>{\text{eff}} = 1/R</em>1 + 1/R_2 + \cdots
    • Example: Two resistors, 3Ω3 \Omega and 6Ω6 \Omega, in parallel have 1/R<em>eff=1/3+1/6=2/6+1/6=3/6=1/2    R</em>eff=2Ω1/R<em>{\text{eff}} = 1/3 + 1/6 = 2/6 + 1/6 = 3/6 = 1/2 \implies R</em>{\text{eff}} = 2 \Omega.
  • Circuit symbols
    • Familiar symbols: fuse, lamp (bulb), battery (DC source), switch, voltmeter (connected in parallel), ammeter (connected in series), thermistor, LDR, resistor, variable resistor.
  • Potential divider concept
    • 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; VPWV_{PW} (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>2R</em>1+R2)V<em>{\text{out}} = V</em>{\text{in}} \left(\frac{R<em>2}{R</em>1 + R_2}\right).
    • Example: A 12 V supply across two series resistors, R<em>1=200ΩR<em>1 = 200 \Omega and R</em>2=100ΩR</em>2 = 100 \Omega. The voltage across R<em>2R<em>2 is V</em>R2=12 V(100200+100)=12 V×13=4 VV</em>{R2} = 12\text{ V} \left(\frac{100}{200 + 100}\right) = 12\text{ V} \times \frac{1}{3} = 4\text{ 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>2R<em>2 in a potential divider, the output voltage (V</em>R2V</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=VItW = VI t (electrical energy converted).
    • Power: P=VIP = VI (rate of energy conversion); alternative forms: P=I2RP = I^2 R; P=V2/RP = V^2 / R.
    • Example: A 240 V heater draws 10 A of current. Its power is P=240×10=2400 WP = 240 \times 10 = 2400\text{ W}. In 1 hour ($3600\text{ s}$), it uses W=2400×3600=8.64×106 JW = 2400 \times 3600 = 8.64 \times 10^6\text{ J}.
  • Cost of electricity
    • Cost = energy used (kWh) ×\times price per kWh; 1 kWh = 3.6×106 J3.6 \times 10^6\text{ J}.
    • Example: If electricity costs 0.20perkWh,andanapplianceuses2.4kWh,thecostis0.20 per kWh, and an appliance uses 2.4 kWh, the cost is2.4 \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, I2^2R 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).
    • Coil/Solenoid: Magnetic field similar