Measuring very large and very small lengths, masses and times · Physics Class 11–12 | StemPy Lab
Course 1.1·Lesson 3 of 3
Measuring very large and very small lengths, masses and times
Lengths in nature run from about 10−15m (a nucleus) to 1026m
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A ruler will not do
A ruler is fine for a book. But how would you measure the height of a mountain, the distance to the Moon, or the size of an atom? You cannot lay a ruler on any of them.
So physicists measure most lengths indirectly: they measure something easy, like an angle or a volume, and calculate the length.
From the very small to the very large
A horizontal line that shows lengths as powers of ten, from 10 to the power minus 15 metre on the left to 10 to the power 25 metre on the right. Things are marked on it in order of size: a proton, an atom, a virus, a hair, a person, a mountain, the Earth, the Sun, the distance from the Earth to the Sun, the nearest star, the Milky Way galaxy and the observable universe.
Lengths in nature cover more than 40 powers of ten. A proton is about 10−15m across, an atom about 10−10m, you about 1m, the Earth about 107m, and the part of the universe we can see about 1026m. Masses and times have the same huge spread.
Large distances: parallax
Hold up a finger and look at it with your left eye, then with your right. It jumps against the background. That jump is parallax.
A triangle. Two observers, L on the left and R on the right, stand on a straight baseline of length b at the bottom. Lines from L and R meet at a tree at the top, and the angle between them at the tree is theta. The distance D from the baseline to the tree is marked on the right. Dashed extensions of the two lines go on to a line of far hills, and they meet it at two different points. The formula D equals b divided by theta is written, with theta in radians.
Two observers stand a known distance b apart: the baseline. Each looks at the same far object. The two lines of sight meet at the object at a small angle θ, the parallax angle. For a small angle, the arc of the baseline is almost straight, so
θ=Db⇒D=θb(θ in radians)
Try it with a tree.
You should find that a far tree gives a tiny angle, and a longer baseline gives a bigger angle that is easier to measure. That is why astronomers use the widest baseline they have: the Earth's orbit, 3×1011m across, measured six months apart.
Watch out.θ must be in radians. Change degrees with ×180π, and seconds of arc with ×36001×180π.
A worked example
Two friends stand 50m apart on a straight road. The lines of sight to a water tower meet at 1.2∘. How far is the tower?
Angle in radians.1.2∘=1.2×180πrad=0.02094rad.
Distance.D=0.02094rad50m≈2390m, about 2.4km.
Think first.1.2∘ is small but not tiny, so the tower should be about 50 times π×1.2180≈48 baselines away. Yes, about 2.4km.
Very small sizes: one molecule thick
A drop of oil spreads on water into a very thin film. Oleic acid spreads until the film is one molecule thick. So:
size of a molecule=thickness=area of filmvolume of oil
The drop must be tiny, so the oil is first mixed with alcohol, say 1 part in 500. The alcohol dissolves in the water and leaves only the oil. The answer comes out near 10−9m, a nanometre.
Masses
A kitchen scale weighs grams; a lorry scale weighs tonnes. For the very large and the very small we again calculate:
The mass of the Earth comes from gravity: how fast things fall and how the Moon moves.
The mass of an atom is measured in atomic mass units: 1u is 121 of the mass of a carbon-12 atom, 1u=1.66×10−27kg. A water molecule is about 18u.
Times
A pendulum or a quartz watch is good for everyday times. The most accurate clocks are atomic clocks, which count the vibrations of caesium atoms. They lose less than a second in millions of years. Very short times, like the life of an unstable particle, are found from how far the particle travels before it decays.
Practise with new numbers
Try it in Python
The program works out the distance of the water tower from the worked example.
Remember these
Most lengths are measured indirectly: measure something easy, then calculate.
Parallax: D=θb, with θ in radians. A longer baseline gives a bigger, easier angle.
An oil film one molecule thick: size = volume of oil ÷ area, about 10−9m.
1u=1.66×10−27kg; atomic clocks keep the second.
Check yourself
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
A distance gives a parallax of 0.01rad with a 3m baseline. How far is it?
Why must the oil be mixed with alcohol first?
A water molecule is about 18u. What is its mass in kilograms?
Why do astronomers measure a star's position six months apart?
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