IB Physics HLTopic 1 — Motion, Forces & EnergyPaper 1 & 2Work, Energy & Power~10 min read
Principle of Conservation of Energy
Energy is the thing that never goes missing. Push a swing, switch on a kettle, drop a ball — whatever happens, the energy you started with is all still there afterwards. It might have moved somewhere else or changed into a different form, but the total never budges. That single idea — the principle of conservation of energy — is one of the most powerful tools in physics, because it lets you follow energy from start to finish without worrying about every detail in between.
📘 What you need to know
Energy cannot be created or destroyed — it can only be transferred from one form to another
The total energy in a closed system stays constant, even as it changes between forms
A system is just the object (or group of objects) we choose to focus on
The main forms are kinetic, gravitational potential, elastic potential, chemical, nuclear and internal (thermal) energy
Kinetic, gravitational and elastic potential energy together are called mechanical energy
No transfer is 100% efficient — some energy is always dissipated (usually as heat) and counted as wasted
Total energy in = useful energy out + wasted energy
What conservation of energy actually says
The principle of conservation of energy can be stated in one line:
The principle of conservation of energy
Energy cannot be created or destroyed; it can only be transferred from one form to another
So the total amount of energy always stays the same. What changes is how that energy is shared out between the different forms. When nothing is happening — a system in equilibrium — the energy just sits there. The moment something changes, energy gets transferred, and that transfer is what makes things happen.
Think of energy like money in a sealed bank. You can move it between accounts — savings, current, cash in your pocket — but the total never changes unless money comes in or leaves. In a closed system nothing comes in or leaves, so the total is fixed. Conservation of energy is just “the books always balance.”
The forms energy comes in
Energy is a single quantity, but it shows up wearing different costumes. Here are the ones you’ll meet most:
Kinetic — the energy of anything that’s moving.
Gravitational potential — energy something gains when it’s lifted up, and loses when it falls.
Elastic potential — energy stored in a stretched or squashed spring (sometimes called strain energy).
Chemical — energy locked inside a chemical substance, like fuel or a battery.
Nuclear — energy held within the nucleus of an atom.
Internal (thermal) — energy something has because of its temperature.
The first three — kinetic, gravitational potential and elastic potential — are grouped together as mechanical energy, because they’re the ones that swap back and forth in moving mechanical systems like springs, pendulums and falling objects.
Chemical (fuel in a car)
transfers to →
Kinetic (car moving)
then some →
Thermal (brakes, air)
Energy transfers and dissipation
Every time energy is transferred from one form to another, some of it leaks away into the surroundings — nearly always as thermal energy that spreads out and can’t easily be used again. We say that energy has been dissipated, and because it’s no longer useful, we call it wasted energy.
Take a kettle. It turns electrical energy into thermal energy in the heating element, and most of that usefully heats the water. But some warms the plastic casing, and some drifts off into the surrounding air. The transfer that heats the water is the useful one; the rest is wasted. Which is which always depends on what you actually want the system to do.
Because energy is conserved, the useful and wasted parts must add up to everything you put in:
Energy accounting
Total energy in = Useful energy out + Wasted energy
The energy going in splits into a useful part (wide green arrow) and a wasted part (thin blue arrow). Add the two together and you get back exactly what went in — nothing is lost.
WE 1
A lamp is supplied with 60 J of electrical energy. Of this, 45 J is transferred to the surroundings as thermal energy. How much useful light energy does the lamp produce?
Step 1 — energy is conserved
Total in = useful out + wasted
Step 2 — rearrange for the useful part
useful = total in − wasted
Step 3 — substituteuseful = 60 − 45Useful light energy = 15 JThe 45 J isn’t destroyed — it’s just spread into the surroundings, where it’s no longer useful.
Where the energy goes: useful vs wasted
In a mechanical system, the energy that gets transferred is the same as the work done — the two are just different names for the same thing. Some everyday examples of energy flowing between forms:
A falling object in a vacuum transfers gravitational potential energy into kinetic energy.
A mass on a horizontal spring swaps elastic potential energy for kinetic energy.
A battery turns chemical energy into electrical energy.
A car engine turns chemical energy from fuel into kinetic energy of the car.
A person on a trampoline cycles between elastic potential, kinetic and gravitational potential energy.
Often there’s also work done against resistive forces like friction. That work doesn’t vanish — it shows up as thermal energy. So when something slides up a rough slope, for instance, the books still balance:
Including friction
Loss in kinetic energy = Gain in gravitational potential energy + Work done against friction
Conservation of mechanical energy
Here’s the trick that makes this idea so useful. If we can ignore friction and drag, then no mechanical energy leaks away as heat, so the mechanical energy alone is conserved. That means whatever one form loses, another form gains — exactly. For a falling object or a swinging pendulum:
When drag is negligible
Loss in gravitational potential energy = Gain in kinetic energy
A swinging pendulum trades gravitational potential energy for kinetic energy and back again. Ignoring air resistance, the total mechanical energy stays the same at every point of the swing.
WE 2
A 2.0 kg ball is dropped from a height of 5.0 m. Ignoring air resistance, use conservation of energy to find its speed just before it hits the ground. (Take g = 9.81 m s−2.)
Step 1 — all the GPE lost becomes KE
mgΔh = ½mv²
Step 2 — the mass cancels, rearrange for v
v = √(2gΔh)
Step 3 — substitutev = √(2 × 9.81 × 5.0) = √98.1v = 9.9 m s⁻¹Notice we never needed the mass — it cancels. Every object falls to the same speed from the same height (when drag is ignored).
🛠️ Using conservation of energy in a problem
Decide on your system and pick a “zero” level for gravitational potential energy (usually the ground or lowest point).
List the energy at the start and the energy at the end — which forms are present at each stage?
Set start energy equal to end energy, since the total is conserved.
Account for any wasted energy (friction, drag) as an extra term if the question mentions it.
Rearrange and solve for whatever you’re after — a speed, a height, or an amount of energy.
WE 3
An electric drill is supplied with 500 J of electrical energy. It does 350 J of useful work on a screw, and the rest is dissipated as thermal energy in the motor. How much energy is wasted?
Step 1 — the books must balance
Total in = useful out + wasted
Step 2 — rearrange for wasted
wasted = total in − useful out
Step 3 — substitutewasted = 500 − 350Wasted energy = 150 JThat 150 J is why a drill gets warm after use — the “lost” energy has simply become heat.
💡 Top tips
Energy is never lost. If a question says energy is “lost”, it means dissipated to the surroundings — usually as heat — not destroyed.
Choose your zero. Any height can be your gravitational potential energy zero, as long as you’re consistent. Only changes in height matter.
Mass often cancels. In pure GPE-to-KE problems the mass drops out, so you don’t always need it.
“Useful” depends on the job. The same thermal energy is useful in a kettle but wasted in a light bulb.
Quick recap: Energy can’t be created or destroyed, only transferred between forms, so the total in a closed system is constant. Kinetic, gravitational and elastic potential energy make up mechanical energy. No transfer is perfectly efficient — some energy is always dissipated (usually as heat) and counted as wasted — so total energy in = useful energy out + wasted energy.
⚠ Common mistakes
Saying energy is “used up” or “lost” — it’s only ever transferred or dissipated, never destroyed
Forgetting the wasted energy term when a system isn’t 100% efficient
Treating heat as separate from energy accounting — dissipated thermal energy still counts in the total
Mixing up useful and wasted — which is which depends entirely on what the system is meant to do
Including the mass when it cancels out, or panicking when a question doesn’t give it
This principle is the backbone of the whole “Work, Energy & Power” section. Next we’ll see how Sankey diagrams turn this “total in = useful out + wasted” idea into a picture, where the width of each arrow shows exactly how much energy flows to each place. Once you can read one of those, efficiency will make instant sense.
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Book a free meeting and let’s work through the tricky bits together.