Electrical Power
Flick on a phone charger and it stays cool for hours. Flick on an electric kettle and it roars
through nearly two litres of boiling water in barely a minute. Both are just "electricity" — so
why is one a gentle trickle and the other a firehose? The difference is power:
how fast each device turns electrical energy into something useful.
The power of an electrical device is the energy it transfers every
second. A big number means energy is being shifted quickly — a bright lamp, a fierce
heater, a fast motor. A small number means a slow dribble — a night-light, a clock, a charging
phone. In this lesson we'll pin that idea down to two short formulas you can carry into any
exam, and see exactly why the kettle is a monster and the charger a mouse.
Power is volts times amps
Two things decide how much energy an electrical device shifts each second. The
potential difference
V (in volts) is the energy handed to each unit of charge as
it passes through. The current I (in amps) is
how much charge flows past every second. Multiply "energy per charge" by "charge per
second" and you get "energy per second" — which is exactly power:
P = V\,I \qquad\text{(watts} = \text{volts} \times \text{amps)}.
Power comes out in watts (symbol \text{W}), and one
watt is one joule of energy transferred per second. So a device rated
1500\ \text{W} is pouring out
1500 joules every single second it runs.
There is a second, equally useful form. Because
Ohm's law tells us
V = I\,R, we can swap V for
I\,R in P = V\,I:
P = V\,I = (I\,R)\,I = I^2 R.
This P = I^2 R version is the one you reach for whenever you care about
the heat made in a resistor or a wire — because a wire's resistance
R is fixed, so the heat it wastes depends on the square of the
current running through it. That single squared term explains most of this lesson.
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Power is energy transferred per second:
P = V\,I (watts = volts × amps).
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Using V = I\,R, the same power can be written
P = I^2 R (and, substituting I = V/R,
P = \dfrac{V^2}{R}).
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The energy transferred in a time t is
E = P\,t = V\,I\,t, in joules when
t is in seconds.
Worked examples
Example 1 — a kettle's power from its volts and amps. A kettle runs on the mains
at 230\ \text{V} and draws a current of
10\ \text{A}. What is its power?
P = V\,I = 230\ \text{V} \times 10\ \text{A} = 2300\ \text{W} = 2.3\ \text{kW}.
Just as advertised on the box — a couple of kilowatts, which is why it boils so fast.
Example 2 — a light bulb. A car headlight bulb runs on a
12\ \text{V} battery and draws
5\ \text{A}. Its power is
P = V\,I = 12 \times 5 = 60\ \text{W}.
A bright bulb — sixty joules of light and heat every second.
Example 3 — heat made in a resistor, using
P = I^2 R. A current of
3\ \text{A} flows through a heating element of resistance
8\ \Omega. How much power does it turn into heat?
P = I^2 R = 3^2 \times 8 = 9 \times 8 = 72\ \text{W}.
Notice the current is squared first: doubling the current to
6\ \text{A} would give
6^2 \times 8 = 288\ \text{W} — four times the heat, not
twice.
Example 4 — energy used over time. That
2300\ \text{W} kettle from Example 1 boils for
80\ \text{s}. How much energy does it transfer? Use
E = P\,t:
E = P\,t = 2300\ \text{W} \times 80\ \text{s} = 184\,000\ \text{J} = 184\ \text{kJ}.
The units keep you right: watts (joules per second) times seconds gives joules back. If your
units don't cancel to joules, a rearrangement has slipped.
See it: build your own appliance
Below is an appliance fed through a cable. Set its voltage
V and the current I it
draws, and the top bar shows the useful power P = V\,I it delivers.
The lower bar is the power wasted as heat in the cable, which has a small fixed
resistance — and that waste follows I^2 R. Watch what happens:
- turn either control up and the useful power grows — power is
volts times amps;
- but the cable-heat bar reacts to the current alone, and grows far faster,
because it depends on I^2. Double the current and it quadruples.
Why power cables are thick and made of copper
Every wire has a little resistance, so every wire wastes some power as heat —
P_{\text{waste}} = I^2 R. Engineers can't change the current a house or
a city needs, but they can change R. A thick
cable of a good conductor like copper has a very
low resistance,
so I^2 R is small and hardly any energy leaks away as heat.
This is also the secret behind the tall pylons that march across the countryside carrying
electricity at hundreds of thousands of volts. For a fixed power
P = V\,I, pushing the voltage up lets the current
I come down for the same power delivered — and since waste is
I^2 R, a smaller current means dramatically less energy lost heating up
hundreds of kilometres of wire. High voltage, low current, thick copper: three ways to keep
I^2 R tiny.
Feel a phone charger after an hour and it's warm; the flex to your kettle stays cool even
though far more power is flowing through it. The heat you feel isn't the total power —
it's I^2 R wasted inside that part. The charger deliberately
drops the mains voltage down, and its little electronics have some resistance, so a bit of
I^2 R warms the plastic. The kettle's thick flex is built with such
low R that even a big current wastes almost nothing along it — all
the energy is saved for the element at the end, which is meant to get hot.
Power ratings and the energy bill
Every appliance carries a power rating stamped on its label — the power it draws
at normal mains voltage. It's a quick guide to how hungry a device is:
- a phone charger: about 5\ \text{W};
- an LED lamp: about 10\ \text{W};
- a laptop: roughly 50\ \text{W};
- a toaster: about 1000\ \text{W} = 1\ \text{kW};
- a kettle or an electric heater: about 2{-}3\ \text{kW}.
The rating also tells you the current the device needs, since
I = P/V — a 3\ \text{kW} appliance on
230\ \text{V} pulls about
13\ \text{A}, which is exactly why UK plugs top out at a
13\ \text{A} fuse.
Your electricity bill, though, is charged for energy, not power — and energy is
power multiplied by time, E = P\,t. To avoid gigantic numbers of
joules, energy companies measure in kilowatt-hours
(\text{kWh}): one kilowatt-hour is a
1\ \text{kW} device left on for one hour. So a
2\ \text{kW} heater running for 3 hours uses
E = P\,t = 2\ \text{kW} \times 3\ \text{h} = 6\ \text{kWh}.
At, say, 30\text{p} per unit, that's
6 \times 30\text{p} = \pounds1.80 of electricity — the same
E = P\,t idea, just in bill-friendly units.
It's tempting to think the most powerful gadget must cost the most to run — but the
bill is E = P\,t, so time matters just as much as power.
A mighty 2000\ \text{W} kettle used for
3 minutes uses 2000 \times 180 = 360\,000\ \text{J}.
A humble 60\ \text{W} bulb left on all night
(8 hours = 28\,800\ \text{s}) uses
60 \times 28\,800 \approx 1\,700\,000\ \text{J} — nearly
five times more. High power for a short burst can be cheaper than low power left
running for hours.
These three catch people out again and again — get them straight now:
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Power is V \times I, never
V \div I or V + I. You
multiply the volts by the amps. (V/I is resistance, a
completely different quantity.) A 12\ \text{V} device drawing
3\ \text{A} is 36\ \text{W}, not
4\ \text{W} and not 15\ \text{W}.
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Heat wasted in a wire grows with the square of the current. Because
P = I^2 R, doubling the current doesn't double the heat — it
quadruples it. This is why we fight to keep current low in long cables.
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A higher-power appliance transfers energy faster, not "more".
Power is a rate (joules per second). How much total energy — and how big the bill —
depends on the rate and how long it runs, through
E = P\,t.