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Grade 9 Physics

Grade 9 Physics on Temari has 37 revision cards, arranged by the chapters of the Ethiopian national curriculum. Every card says when the rule applies, what each symbol in it stands for, and the mistake students most often make with it. They are free to read and need no account.

37
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7
Chapters
19
Formulas
11
Reference tables
Grade 9 Physics
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6 September 2026
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01

Physics and Human Society

BranchSubject of Study
MechanicsMotion of objects with or without forces
AcousticsSound, its production, transmission, and effects
OpticsBehavior and properties of light
ThermodynamicsHeat, thermal energy, and heat transfer
ElectromagnetismElectric and magnetic fields and forces
Nuclear physicsStructure, properties, and reactions of atomic nuclei
AstrophysicsAstronomical objects and celestial phenomena

When you use it

Use this to classify physical phenomena into their correct subfields of physics.

Watch out

Do not confuse mechanics with thermodynamics. Mechanics deals with motion and forces, whereas thermodynamics deals strictly with heat and temperature transfer.

Drafted from Grade 9 Physics, pages 2-11, then checked twice before it went up

When you use it

Use this to distinguish historical eras and conceptual shifts in physics development.

Watch out

Classical physics covers discoveries from the Renaissance up to the end of the 19th century. Developments starting at the beginning of the 20th century belong to modern physics.

Drafted from Grade 9 Physics, pages 2-11, then checked twice before it went up

ScientistKey Contribution
Galileo GalileiTelescopic astronomy and the scientific method
Isaac NewtonLaws of motion and universal gravitation
Michael FaradayElectromagnetic induction and electrolysis
James Prescott JouleMechanical equivalent of heat and conservation of energy
Marie CurieRadioactivity, polonium, and radium
Albert EinsteinTheory of relativity and quantum theory

When you use it

Use this to identify major historical scientists and the fundamental principles they discovered.

Watch out

James Prescott Joule linked heat to mechanical work. Faraday is the contributor for electromagnetic induction, not Joule.

Drafted from Grade 9 Physics, pages 2-11, then checked twice before it went up

02

Physical Quantities

PrefixSymbolFactor
teraT101210^{12}
gigaG10910^9
megaM10610^6
kilok10310^3
centic10210^{-2}
millim10310^{-3}
microμ\mu10610^{-6}
nanon10910^{-9}
picop101210^{-12}

When you use it

Use when converting very large or very small measurements into standard powers of 10.

Watch out

Micro uses the Greek letter μ\mu for 10610^{-6}, while milli uses m for 10310^{-3}. Do not confuse the symbols.

Drafted from Grade 9 Physics, pages 12-35, then checked twice before it went up

When you use it

Use to classify physical quantities based on whether direction is required along with magnitude.

Watch out

Distance and speed are scalars, but displacement and velocity are vectors. Mass is a scalar, whereas force is a vector.

Drafted from Grade 9 Physics, pages 12-35, then checked twice before it went up

Physical quantitySymbolSI UnitUnit Symbol
Lengthllmeterm
Massmmkilogramkg
Timettseconds
TemperatureTTkelvinK
CurrentIIampereA
Amount of substancennmolemol
Luminous intensityIvI_vcandelacd

When you use it

Use this reference to identify the seven base physical quantities and their standard SI units.

Watch out

Speed, force, and density are derived quantities. Only these seven cannot be defined in terms of other quantities.

Drafted from Grade 9 Physics, pages 12-35, then checked twice before it went up

When you use it

Use when identifying valid mathematical operations on interval and ratio measurement scales.

Watch out

Celsius and Fahrenheit are interval scales without a true zero, so values cannot be multiplied or divided. Only the Kelvin scale is a ratio scale with an absolute zero.

Drafted from Grade 9 Physics, pages 12-35, then checked twice before it went up

03

Motion in a Straight Line

aav=vfvitfti=ΔvΔt\vec{a}_{av} = \frac{\vec{v}_f - \vec{v}_i}{t_f - t_i} = \frac{\Delta \vec{v}}{\Delta t}
aav\vec{a}_{av}
average accelerationms2m\,s^{-2}
vf\vec{v}_f
final velocityms1m\,s^{-1}
vi\vec{v}_i
initial velocityms1m\,s^{-1}
Δv\Delta \vec{v}
change in velocityms1m\,s^{-1}
Δt\Delta t
time intervalss

When you use it

Use to calculate the rate of change of velocity over a given time interval.

Watch out

When an object slows down, final velocity is less than initial velocity, resulting in negative acceleration (deceleration).

Drafted from Grade 9 Physics, pages 36-59, then checked twice before it went up

vav=stotttotv_{av} = \frac{s_{tot}}{t_{tot}}
vavv_{av}
average speedms1m\,s^{-1}
stots_{tot}
total distancemm
ttott_{tot}
total timess

When you use it

Use to calculate the rate at which total distance is covered over the total time taken.

Watch out

Always convert non SI units before calculating. Multiply km/h by 10/36 to convert to m/s.

Drafted from Grade 9 Physics, pages 36-59, then checked twice before it went up

vav=ΔSΔt=SfSitfti\vec{v}_{av} = \frac{\Delta \vec{S}}{\Delta t} = \frac{\vec{S}_f - \vec{S}_i}{t_f - t_i}
vav\vec{v}_{av}
average velocityms1m\,s^{-1}
ΔS\Delta \vec{S}
displacementmm
Sf\vec{S}_f
final positionmm
Si\vec{S}_i
initial positionmm
Δt\Delta t
time intervalss
tft_f
final timess
tit_i
initial timess

When you use it

Use to calculate the rate of change of position in a specific direction over a time interval.

Watch out

Displacement depends on initial and final positions only. It is not the total distance travelled along the path.

Drafted from Grade 9 Physics, pages 36-59, then checked twice before it went up

GraphSlopeArea Under Curve
StS-tvelocityNo physical meaning
vtv-taccelerationdistance or displacement

When you use it

Use when finding velocity, acceleration, or distance from position-time and velocity-time graphs.

Watch out

The slope of a v-t graph gives acceleration, while the area under it gives distance or displacement. Do not mix slope and area.

Drafted from Grade 9 Physics, pages 36-59, then checked twice before it went up

When you use it

Reach for this when an object completes a trip and returns to its starting point.

Watch out

When an object returns to its starting point, net displacement is zero and average velocity is zero, but total distance and average speed are greater than zero.

Drafted from Grade 9 Physics, pages 36-59, then checked twice before it went up

04

Force, Work, Energy and Power

Ep=mghE_p = m g h
EpE_p
gravitational potential energyJ\text{J}
mm
masskg\text{kg}
gg
acceleration due to gravityms2\text{m}\,\text{s}^{-2}
hh
heightm\text{m}

When you use it

Use to find the stored energy of an object raised to a height above the ground.

Watch out

Height h is the vertical distance above the reference point, not the path length along a slope.

Drafted from Grade 9 Physics, pages 60-81, then checked twice before it went up

Ek=12mv2E_k = \frac{1}{2} m v^2
EkE_k
kinetic energyJ\text{J}
mm
masskg\text{kg}
vv
speedms1\text{m}\,\text{s}^{-1}

When you use it

Use to calculate the energy possessed by an object due to its motion.

Watch out

Square only the speed v, not the mass. Doubling the speed quadruples the kinetic energy.

Drafted from Grade 9 Physics, pages 60-81, then checked twice before it went up

F=maF = m a
FF
net forceN\text{N}
mm
masskg\text{kg}
aa
accelerationms2\text{m}\,\text{s}^{-2}

When you use it

Use when calculating acceleration, net force, or mass of an accelerating body.

Watch out

Mass must always be converted to kg before calculating. Unbalanced force produces acceleration, not constant velocity.

Drafted from Grade 9 Physics, pages 60-81, then checked twice before it went up

P=WtP = \frac{W}{t}
PP
powerW\text{W}
WW
work done or energy transferredJ\text{J}
tt
time takens\text{s}

When you use it

Use to calculate the rate at which work is done or energy is transferred.

Watch out

Time t must be converted to seconds before dividing. One watt is one joule per second.

Drafted from Grade 9 Physics, pages 60-81, then checked twice before it went up

W=FSW = F_{\parallel} S
WW
workJ\text{J}
FF_{\parallel}
force in direction of displacementN\text{N}
SS
displacementm\text{m}

When you use it

Use when a constant force moves an object through a displacement parallel to the force.

Watch out

Carrying an object horizontally does no work against gravity because force and displacement are perpendicular.

Drafted from Grade 9 Physics, pages 60-81, then checked twice before it went up

05

Simple Machines

η=MAVR=Work outputWork input\eta = \frac{\text{MA}}{\text{VR}} = \frac{\text{Work output}}{\text{Work input}}
η\eta
Efficiency of the machinedimensionless\text{dimensionless}
MA\text{MA}
Mechanical Advantage, ratio of Load to Effortdimensionless\text{dimensionless}
VR\text{VR}
Velocity Ratio, distance moved by Effort over distance moved by Loaddimensionless\text{dimensionless}
Work output\text{Work output}
Useful work done by the machine on the LoadJ\text{J}
Work input\text{Work input}
Work put into the machine by the EffortJ\text{J}

When you use it

Use when finding the efficiency of any simple machine or relating output work and input work to mechanical advantage and velocity ratio.

Watch out

Mechanical Advantage, Velocity Ratio, and Efficiency are ratios and have no units. Efficiency is always less than 1 (or less than 100 percent) in real machines.

Drafted from Grade 9 Physics, pages 82-113, then checked twice before it went up

When you use it

Use when evaluating true or false statements and conceptual questions about whether machines create energy or decrease total work.

Watch out

Machines never multiply work or energy. A machine can multiply force or multiply speed and distance, but never both at the same time. Due to friction, work output is always less than work input, so AMA is always less than IMA.

Drafted from Grade 9 Physics, pages 82-113, then checked twice before it went up

ClassMiddle ComponentIMA CharacteristicExamples
1st ClassFulcrumIMA>1\text{IMA} > 1, IMA=1\text{IMA} = 1, or IMA<1\text{IMA} < 1Seesaw, scissors, crowbar
2nd ClassLoadIMA>1\text{IMA} > 1Wheelbarrow, nutcracker, bottle opener
3rd ClassEffortIMA<1\text{IMA} < 1Tweezers, broom, fishing pole, tongs

When you use it

Use to identify the class of a lever based on which point lies in the middle: Fulcrum, Load, or Effort.

Watch out

Remember the middle component order: 1st class has Fulcrum in the middle, 2nd class has Load in the middle, and 3rd class has Effort in the middle.

Drafted from Grade 9 Physics, pages 82-113, then checked twice before it went up

Simple MachineVelocity Ratio (VR) FormulaSymbols
Inclined PlaneVR=lh\text{VR} = \frac{l}{h}l=slope length,  h=heightl = \text{slope length},\; h = \text{height}
WedgeVR=lt\text{VR} = \frac{l}{t}l=penetration length,  t=thicknessl = \text{penetration length},\; t = \text{thickness}
ScrewIMA=2πrp=πdp\text{IMA} = \frac{2\pi r}{p} = \frac{\pi d}{p}r=radius,  d=diameter,  p=pitchr = \text{radius},\; d = \text{diameter},\; p = \text{pitch}
Wheel and AxleVR=Rr\text{VR} = \frac{R}{r}R=wheel radius,  r=axle radiusR = \text{wheel radius},\; r = \text{axle radius}
Pulley SystemVR=N\text{VR} = NN=number of rope strands supporting loadN = \text{number of rope strands supporting load}

When you use it

Use to calculate the theoretical Velocity Ratio or Ideal Mechanical Advantage directly from the physical dimensions of the machine.

Watch out

For a screw, pitch is the distance between consecutive threads. For wheel and axle, ensure the effort radius is divided by the load radius.

Drafted from Grade 9 Physics, pages 82-113, then checked twice before it went up

06

Mechanical Oscillation and Sound

When you use it

Apply when solving problems where sound travels to an obstacle and reflects back to the observer or source.

Watch out

The measured time t is for the round trip. The one way distance to the obstacle is d = v times t / 2. Forgetting to divide by 2 gives double the actual distance.

Drafted from Grade 9 Physics, pages 114-139, then checked twice before it went up

T=2πmkT = 2\pi \sqrt{\frac{m}{k}}
TT
Periodss
mm
Masskgkg
kk
Spring constantNm1N\,m^{-1}

When you use it

Use this formula to calculate the period of oscillation for a mass attached to a horizontal or vertical spring.

Watch out

Mass must be in kilograms and spring constant k in N/m. The period depends only on mass and spring constant, not on displacement amplitude.

Drafted from Grade 9 Physics, pages 114-139, then checked twice before it went up

T=2πLgT = 2\pi \sqrt{\frac{L}{g}}
TT
Periodss
LL
Length of pendulummm
gg
Acceleration due to gravityms2m\,s^{-2}

When you use it

Use this formula to find the period of a simple pendulum or to calculate local gravitational acceleration from pendulum length and period.

Watch out

The mass of the bob and the amplitude do not affect the period. Length must be converted from centimeters to meters.

Drafted from Grade 9 Physics, pages 114-139, then checked twice before it went up

v=3311+Tc273v = 331 \sqrt{1 + \frac{T_c}{273}}
vv
Speed of soundms1m\,s^{-1}
TcT_c
Air temperatureC^\circ\text{C}

When you use it

Use this formula to find the speed of sound in air at any given Celsius temperature.

Watch out

Insert the temperature directly in degrees Celsius, not Kelvin. The speed of sound at 0 degrees Celsius is 331 m/s.

Drafted from Grade 9 Physics, pages 114-139, then checked twice before it went up

v=fλv = f \lambda
vv
Wave speedms1m\,s^{-1}
ff
FrequencyHzHz
λ\lambda
Wavelengthmm

When you use it

Use this formula to relate the propagation speed of any periodic wave to its frequency and wavelength.

Watch out

Wavelength must be in meters. If given the period T instead of frequency, use f = 1/T.

Drafted from Grade 9 Physics, pages 114-139, then checked twice before it went up

What to compareTransverse waveLongitudinal wave
How the particles moveAt right angles to the direction the wave travels.Back and forth along the same line the wave travels.
What the diagram showsA sine curve of crests and troughs, with the travel arrow drawn along the horizontal axis.A band of vertical lines that are alternately crowded and spread out, labelled C R C R C, with the travel arrow drawn along the band.
The parts you labelCrests at the top of the curve and troughs at the bottom.Compressions, marked C, where the particles are crowded and the pressure is high; rarefactions, marked R, where they are spread apart and the pressure is low.
ExamplesWater waves, where the surface moves up and down while the wave travels across it. Light.Sound in air, sent out as a vibrating object pushes and pulls the air beside it.
What actually travelsThe energy goes forward. Each particle only swings about its own resting place.The energy goes forward. Each particle only swings about its own resting place.

When you use it

Use when a question asks which kind a given wave is, or asks you to label a wave diagram. Compare two directions: the way the particles of the medium vibrate and the way the wave itself travels. At right angles means transverse, along the same line means longitudinal.

Watch out

Students memorise the picture instead of the motion, so they see sound drawn as a smooth curve on an oscilloscope and answer that sound is transverse. That curve is a graph of displacement or pressure against distance or time. It is not a picture of what the air is doing. In air the particles move back and forth along the very line the sound is travelling, so sound stays longitudinal however it is graphed. Judge by the direction the particles vibrate and never by the shape of the drawing.

What to compareMechanical waveElectromagnetic wave
A medium to travel throughNeeded. It must have a solid, a liquid or a gas.Not needed. It carries itself across empty space, which is how starlight reaches us, and it can still pass through glass or water.
What moves it alongEach particle of the medium pushes and pulls the next one.An oscillating electric field and magnetic field that keep regenerating each other.
SpeedThe medium sets it. Sound in air at room temperature is about 340 m/s.Every one of them travels at about 300 000 000 m/s in a vacuum.
Transverse or longitudinalEither. A wave on a string is transverse and sound in air is longitudinal.Always transverse.
ExamplesSound, water waves, a wave on a stretched string, seismic waves.Light, radio waves, X-rays. Radio, television and mobile signals all travel this way.
In medical imagingUltrasound scanning, which is sound above 20 kHz.X-ray imaging.
The test that settles itRing an alarm clock inside a jar and pump the air out. The sound fades to nothing.The light from that same clock still reaches your eye.

When you use it

Use when a question asks which waves can cross a vacuum, or gives you a list of waves to sort into two groups. One thing decides every case: a mechanical wave needs matter to travel through and an electromagnetic wave does not.

Watch out

Students see X-ray and ultrasound printed together under medical imaging and file both as electromagnetic. Ultrasound is sound. It is a mechanical wave that needs tissue to travel through, and that is exactly why the technician squeezes gel between the probe and the skin: a thin layer of air would reflect the sound back and the scan would show nothing. X-rays need no medium at all. The exam question that catches this is always the same one, asking which of the listed waves can travel through a vacuum. Light, radio and X-rays can. Sound, ultrasound, water waves and seismic waves cannot.

node to node=λ2,  node to antinode=λ4\text{node to node} = \dfrac{\lambda}{2}, \; \text{node to antinode} = \dfrac{\lambda}{4}
λ\lambda
the wavelength of each of the two travelling waves that build the patternm\mathrm{m}
AA
the amplitude of one of those two waves on its ownm\mathrm{m}
2A2A
the amplitude at an antinode, twice that of a single wavem\mathrm{m}

When you use it

Use for a string, a rope or an air column vibrating in a fixed pattern, where a node stays still at all times and an antinode swings twice as far as either wave alone. Node to node is half a wavelength and node to antinode is a quarter, which is what turns a measured length into a wavelength.

Watch out

Students take the distance between two neighbouring nodes to be one full wavelength. It is half of one. That single slip breaks every string and pipe question: a string of length L vibrating in its fundamental holds one loop, so L is half a wavelength, the wavelength is twice L, and the frequency comes out as the wave speed divided by twice L. Read the wavelength as L instead and the answer is double the true frequency every time. Count loops rather than nodes, because each loop between two nodes is half a wave. One more thing to be exact about: an antinode has the largest amplitude of swing, and its displacement still passes through zero twice every cycle, at the instants when the whole medium is momentarily straight.

Ares=A1+A2 or Ares=A1A2A_{res} = A_{1} + A_{2} \text{ or } A_{res} = |A_{1} - A_{2}|
A1A_{1}
the amplitude of the first wavem\mathrm{m}
A2A_{2}
the amplitude of the second wavem\mathrm{m}
AresA_{res}
the resultant amplitude where the two overlap: the sum when they arrive in phase, the difference when they arrive half a cycle apartm\mathrm{m}

When you use it

Use when two waves overlap at a point and a question asks how loud, how bright or how tall the result is. Add the amplitudes when the waves arrive in phase, which means a path difference of a whole number of wavelengths, and subtract them when the waves arrive half a cycle apart, which means a path difference of an odd number of half wavelengths.

Watch out

Students read destructive as the waves being destroyed and expect silence or darkness whenever two waves meet out of step. Two things have to be true before the result is zero: the waves must arrive exactly half a cycle apart, which is an odd number of half wavelengths of path difference rather than merely out of step, and their amplitudes must be equal. A 3 cm wave meeting a 2 cm wave in antiphase leaves a 1 cm wave. Nothing is lost either. The energy taken from the quiet points reappears at the loud ones, and both waves come out of the meeting exactly as they went in.

EA2f2E \propto A^{2} f^{2}
EE
the energy the wave carries. It travels forward while the particles of the medium only swing about their resting placesJ\mathrm{J}
AA
the displacement amplitude: how far each particle swings from its resting placem\mathrm{m}
ff
the frequency of the wave, the number of complete oscillations each secondHz\mathrm{Hz}

When you use it

Use when a question changes the amplitude or the frequency of a sound, a wave on a string or a water wave and asks what happens to the energy it carries. Both quantities are squared, so doubling either one on its own gives four times the energy and doubling both gives sixteen times.

Watch out

Students read the proportion as a straight multiplication and say that doubling the amplitude doubles the energy. It quadruples, because the amplitude is squared, and doubling the amplitude and the frequency together gives sixteen times the energy rather than four. The second trap is hearing higher frequency as louder: a higher frequency sound is higher in pitch, and loudness is what the amplitude controls. Note also that the relation carries no constant, so it compares two waves of the same kind in the same medium and never gives an energy in joules. It belongs to mechanical waves alone and does not carry over to light, whose brightness is set by amplitude while frequency changes the colour.

07

Temperature and Thermometry

ScaleIce PointSteam PointDivisions
Celsius0C0^\circ\text{C}100C100^\circ\text{C}100100
Fahrenheit32F32^\circ\text{F}212F212^\circ\text{F}180180
Kelvin273.15 K273.15\text{ K}373.15 K373.15\text{ K}100100

When you use it

Reference the standard calibration fixed points and division counts across standard scales.

Watch out

A temperature difference of 1 degree Celsius is equal to 1 Kelvin, but it is not equal to 1 degree Fahrenheit.

Drafted from Grade 9 Physics, page 140 onwards, then checked twice before it went up

ΔL=αL0ΔT\Delta L = \alpha L_0 \Delta T
ΔL\Delta L
change in lengthm\text{m}
α\alpha
coefficient of linear expansion(C)1(^\circ\text{C})^{-1}
L0L_0
initial lengthm\text{m}
ΔT\Delta T
change in temperatureC^\circ\text{C}

When you use it

Calculate the expansion or contraction in length of a solid rod when its temperature changes.

Watch out

Do not confuse the change in length with the final length. The final length is the initial length plus the change in length.

Drafted from Grade 9 Physics, page 140 onwards, then checked twice before it went up

TC=59(TF32)=TK273.15T_C = \frac{5}{9}(T_F - 32) = T_K - 273.15
TCT_C
temperature in CelsiusC^\circ\text{C}
TFT_F
temperature in FahrenheitF^\circ\text{F}
TKT_K
temperature in KelvinK\text{K}

When you use it

Convert temperature readings between Celsius, Fahrenheit, and Kelvin scales.

Watch out

Subtract 32 before multiplying by 5/9 when converting Fahrenheit to Celsius. Do not use degree signs with Kelvin.

Drafted from Grade 9 Physics, page 140 onwards, then checked twice before it went up

When you use it

Use when determining whether a hole or inner diameter expands or contracts during heating.

Watch out

A hole in an object does not shrink when heated. It expands at the exact same rate as if it were filled with solid material.

Drafted from Grade 9 Physics, page 140 onwards, then checked twice before it went up

ThermometerThermometric PropertyMeasuring Range
Mercury thermometerLength of mercury column30C to 300C-30^\circ\text{C}\text{ to }300^\circ\text{C}
Alcohol thermometerExpansion of alcohol volume115C to 78.15C-115^\circ\text{C}\text{ to }78.15^\circ\text{C}
Resistance thermometerElectrical resistance of platinum270C to 700C-270^\circ\text{C}\text{ to }700^\circ\text{C}
ThermocoupleVoltage between two junctions270C to 2300C-270^\circ\text{C}\text{ to }2300^\circ\text{C}

When you use it

Select appropriate thermometer types and identify their physical thermometric properties.

Watch out

Alcohol thermometers are chosen for very cold environments because alcohol freezes at a much lower temperature than mercury.

Drafted from Grade 9 Physics, page 140 onwards, then checked twice before it went up

Q=mcΔT and Q=mLQ = mc\,\Delta T \text{ and } Q = mL
QQ
the heat energy transferred because of a temperature difference. A body does not contain heat; it contains internal energy, and heat is that energy while it is movingJ\mathrm{J}
mm
the mass of the substance being heated, cooled or changedkg\mathrm{kg}
cc
the specific heat capacity of the material: the energy that raises 1 kg of it by 1 K. For water it is about 4200 J per kilogram per kelvinJkg1K1\mathrm{J\,kg^{-1}\,K^{-1}}
ΔT\Delta T
the change in temperature. A Celsius interval and a kelvin interval are the same size, so the number is the same either wayK\mathrm{K}
LL
the specific latent heat: fusion for melting and freezing, vaporisation for boiling and condensing. For water these are about 334 000 and about 2 260 000 joules per kilogramJkg1\mathrm{J\,kg^{-1}}
CC
the heat capacity of one whole body, which is its mass times c. A big block has a larger C than a small block of the same materialJK1\mathrm{J\,K^{-1}}

When you use it

Use whenever a question heats, cools, melts, freezes or boils something and asks for the energy. While the thermometer is still moving, the energy is mass times specific heat capacity times temperature change; while it holds steady at a melting or boiling point, it is mass times specific latent heat.

Watch out

Students reach for the temperature form on a melting or boiling step. Asked for the energy that turns 0.5 kg of ice at 0 °C into water at 0 °C, they look for a temperature change, find none, and either write zero or invent one. Melting has no temperature change at all: it is mass times the latent heat of fusion, which comes to 167 000 J. On a heating curve, use the temperature form on the sloping parts and the latent heat form on the flat parts, then add the steps. The other slip is swapping C for c. Capital C belongs to one particular object and is measured in J/K; small c belongs to the material and is measured in J/(kg K), and small c is the one printed in the data table.

The same subject in other years

An exam paper keeps asking for what the year below taught. Those cards are here too.

Questions students ask

What do the Grade 9 Physics cards cover?
37 cards across 7 chapters of the national textbook: Physics and Human Society, Physical Quantities, Motion in a Straight Line, Force, Work, Energy and Power, Simple Machines, Mechanical Oscillation and Sound and Temperature and Thermometry. You can take any chapter one card at a time on the page itself.
Is there a national exam in Grade 9?
No. Ethiopia sets national exams in Grade 6, Grade 8 and Grade 12 only. These cards are for your school's own exams, and for the national exam that comes a few years later.
Where do these cards come from?
They are drafted from Grade 9 Physics, the Ministry of Education textbook for this grade. A second pass that cannot see the chapter then re-derives every formula, constant and table row, and anything it cannot confirm is held back instead of published.
Is this free?
Yes. Every card here is free to read and the printable sheet is free to download. Neither needs an account.
When was this last checked?
6 September 2026. Cards arrive chapter by chapter, and the line under each one says when that card was last read through.

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