1.1The Molecular Structure of Water, Its Unique Properties and Water Sustainability1.2The Atmosphere: Layers, the Greenhouse Effect and Ozone Depletion1.3Renewable Energy Sources, Green Hydrogen and Climate Adaptation1.4The Greenhouse Effect, the Carbon Footprint and Sustainable Solutions1.5Ecological Balance in Earth Systems, Biogeochemical Cycles and Food Webs1.1Why study motion?1.2Definition of motion1.3Types of motion1.4Why we need velocity1.5Speed and velocity1.6Converting units1.7Worked examples1.8Uniform and non-uniform (variable) velocity1.9Instantaneous and average velocity1.10Worked examples1.11How to draw it1.12Reading the displacement–time graph1.13Worked examples1.14Definition1.15A motion diagram: the car that gains 5 m/s every second1.16Types of acceleration1.17Worked examples1.18Reading the graph1.19Analysing a multi-stage graph1.20Extension — displacement from the v–t graph1.21Motion (dot) diagrams1.22More worked examples1.23Short answers to typical discussion questions1.24Summary1.25Introduction1.26What is force?1.27Resultant force1.28Observation and the old belief1.29Statement of the law1.30Consequences of the first law1.31Inertia1.32Momentum1.33Statement1.34Another statement of the law1.35Definition of the newton1.36Thinking exercise1.37Worked examples1.38Life applications of the second law (force, time and change of momentum)1.39The first law as a special case of the second1.40Observations1.41Statement1.42Properties of action and reaction1.43Applications1.44Worked examples1.45Short answers to typical discussion questions1.46Summary1.47Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula| Comparison aspect | Main idea | Example | Keywords |
|---|---|---|---|
| Translational motion |
| — | startingpointExamplesstraight |
| Periodic motion |
| a swinging pendulum or a vibrating tuning-fork prong | repeatsitselfequalintervals |
| Motion | Type |
|---|---|
| Pendulum of a clock | periodic (vibrational) |
| A projectile | translational |
| A train going from Cairo to Aswan | translational |
| Prong of a sounding tuning fork | periodic (vibrational) |
| The Earth’s revolution around the Sun | periodic (circular) |
| Point | Speed | Velocity |
|---|---|---|
| Definition | distance covered per unit time | displacement per unit time |
| Type of quantity | scalar (magnitude only) | vector (magnitude and direction) |
| Sign | always positive |
|
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Example 1. | A cyclist covers 450 m in 90 s along a straight road. Find the velocity in m/s and in km/h | cyclistcoversalongstraight |
| v = Δd/Δt = 450/90 = 5 m/s; in km/h | 5 × 3.6 = 18 km/h | |
| Example 2. | A train moves at a velocity of 72 km/h. How far does it go in 25 min if the velocity is uniform? | trainmovesvelocitydoes |
| • |
| 1500 |
| (Or in km/h | 72 × 25/60 = 30 km.) | |
| Example 3. | An athlete runs 6000 m in 40 min along a straight track. The average velocity is 6000/(40 × 60) = 2.5 m/s = 9 km/h. If he keeps this average velocity he covers 2.5 × 3600 = 9000 m in one hour | athleteruns6000along |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Uniform velocity |
| objectcoversequaldisplacements |
| Non-uniform (variable) velocity |
| objectcoversunequaldisplacements |
| Shape of the graph | Meaning |
|---|---|
| Straight line sloping upward | uniform velocity (positive) |
| Steeper straight line | greater velocity |
| Horizontal line | displacement does not change → the object is at rest (velocity = 0) |
| Straight line sloping downward | uniform velocity in the negative direction (moving back) |
| Curve |
|
| Slope of a tangent at a point | instantaneous velocity at that moment |
| Slope of the chord joining two points | average velocity between those two moments |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Example 1. |
| straightlinedisplacementtime |
| Example 2. |
| curvedgraphobjectaverage |
| Example 3 (graph in words). |
| walkermovesoriginrising |
| time (s) | 0 | 1 | 2 | 3 | 4 |
|---|---|---|---|---|---|
| velocity (m/s) | 0 | 5 | 10 | 15 | 20 |
| Shape of the v–t graph | Meaning |
|---|---|
| Horizontal line (above the axis) | constant velocity → a = 0 (uniform velocity) |
| Horizontal line on the time axis (v = 0) | at rest |
| Straight line sloping upward | uniform positive acceleration |
| Straight line sloping downward | uniform negative acceleration (deceleration) |
| Steeper line | larger magnitude of acceleration |
| Curved line | non-uniform acceleration |
| Stage | AB | BC | CD |
|---|---|---|---|
| Initial velocity vᵢ | 0 | 25 m/s | 25 m/s |
| Final velocity vf | 25 m/s | 25 m/s | 0 |
| Change Δv | +25 m/s | 0 | −25 m/s |
| Duration | 10 s | 10 s | 10 s |
| Acceleration a = Δv/t | +2.5 m/s2 | 0 | −2.5 m/s2 |
| Description | speeding up uniformly | constant velocity | slowing down uniformly to rest (braking) |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| AB | ½ × 10 × 25 = 125 m | |
| BC | 10 × 25 = 250 m | |
| CD | ½ × 10 × 25 = 125 m | |
| • |
| Totaldistanceaveragevelocity |
| • |
| constantaccelerationfollowingresults |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Example 1. |
| graphlinepassesthrough |
| Example 2. | A train slows from 30 m/s to 10 m/s in 20 s. a = (10 − 30)/20 = −1 m/s2. Its v–t line slopes downward with slope −1 | trainslowslineslopes |
| Example 3 (both quantities negative). |
| cartmovesleftvelocity |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| • |
| ballrollsfloorslows |
| If an object’s acceleration is zero, is its velocity zero? |
| meansconstantExampletravelling |
| Why does the average velocity differ from the instantaneous velocity? |
| overalldisplacementtotaltime |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| If ΣF = 0, then a = 0 |
| velocitydoeschangewhether |
| • |
| forceneededstartstationary |
| No force is needed to keep an object moving at constant velocity | (only to cancel friction/air resistance). A car moving steadily on a straight road has an engine force that exactly balances the resistances: ΣF = 0 | cancelfrictionresistancesteadily |
| Example 1. |
| movessteadyalongstraight |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| • | It is a vector (same direction as the velocity) | vectorsamedirectionvelocity |
| Unit | kg·m/s | |
| Dimensional formula | MLT−1 | |
| • | A body with larger momentum needs a larger force or a longer time to be stopped | bodylargermomentumneeds |
| Example 1. | A truck of mass 8000 kg moves at 15 m/s: p = 8000 × 15 = 1.2 × 105 kg·m/s. A cyclist and cycle of total mass 90 kg at 6 m/s: p = 540 kg·m/s. The truck’s momentum is more than 200 times larger | truckmass8000moves |
| Example 2. |
| ballmovesrightAfter |
| Example 3. | What speed gives a 1200 kg car the same momentum as the truck in Example 1? v = p/m = 1.2 × 105/1200 = 100 m/s (360 km/h) | Whatspeedgives1200 |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Example 1 — F = ma. | A car of mass 1200 kg accelerates uniformly at 2.5 m/s2. The resultant force = 1200 × 2.5 = 3000 N | mass1200acceleratesuniformly |
| Example 2 — mass. | A resultant force of 45 N gives a body an acceleration of 1.5 m/s2. m = F/a = 45/1.5 = 30 kg | resultantforcegivesbody |
| Example 3 — net force with friction. |
| cratepushedwhileopposes |
| Example 4 — from the change of momentum. |
| forceactsbodychanging |
| Example 5 — velocity after a time. |
| trolleyrestpulledforce |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Newton’s third law |
| objectexertsforcesecond |
| Mathematical form | F₁ = − F₂ |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| There is no single force |
| universeactionreactionappear |
| • |
| equalmagnitudeoppositedirection |
| They have the same nature |
| actiongravitationalforcereaction |
| They do not cancel each other | because they act on two different bodies. (Forces cancel only if they act on the same body.) | becausedifferentbodiesForces |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Rocket propulsion |
| burninglargemassexpelled |
| Recoil of a gun |
| pushesbulletforwardbackward |
| Swimming/walking |
| swimmerpusheswaterback |
| Space | an astronaut who throws an object in one direction moves in the opposite direction. This suggests how a spacecraft can change its direction outside the atmosphere: by ejecting gas in the direction opposite to the desired change | astronautthrowsobjectdirection |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| • |
| trainsuddenlymovesforward |
| Why is the first law a special case of the second? |
| constantvelocity |
| What happens when an astronaut throws an object? |
| movesoppositedirectionthird |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Force |
| externalinfluencechangestries |
| First law |
| restconstantvelocityinertia |
| • | Momentum p = mv (kg·m/s) | Momentum |
| Second law |
| longertimeimpactgives |
| Third law |
| equaloppositesamenature |
| • |
| margin18pxbordersolid |
| Graph Type | Curve Shape | Physical Meaning | Physical Slope Value |
|---|---|---|---|
| Distance – Time (d – t) | Straight line passing through origin | Uniform Constant Speed | Slope = Velocity (v) |
| Distance – Time (d – t) | Horizontal line parallel to time axis | Body at complete rest | Slope = 0 (v = 0) |
| Speed – Time (v – t) | Straight line passing through origin | Uniform Positive Acceleration | Slope = Acceleration (+a) |
| Speed – Time (v – t) | Horizontal line parallel to time axis | Uniform Constant Speed | Slope = 0 (Zero acceleration) |
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