Part III · Geometry Chapter 20 of 60
Area and volume
A workshop with scissors: we cut figures, rearrange the pieces and find out what area is. Any polygon can be re-cut into any other of the same area, but a disc and a cube won’t give in to scissors.
Builds on: 19 · The circle and the number π
You will learn
- derive the areas of a parallelogram, triangle and trapezium by re-cutting, and find areas on squared paper with Pick’s theorem
- understand why any two polygons of equal area can be re-cut into each other, while a disc and a square can’t
- find the volumes of a prism, pyramid, cylinder, cone and ball and the area of a sphere, and know where these formulas come from
The last chapter found the area of a disc by a trick: the disc was sliced into thin sectors, and they were put together into a shape almost indistinguishable from a rectangle with sides $\pi r$ and $r$. The trick worked, but it hides two questions. Why doesn’t area change when a figure is cut up and rearranged? And what is area anyway: a number we assign to a figure, or something that’s “contained” in it?
In this chapter a workshop is open. There are two tools: scissors that cut only in straight lines, and a table on which pieces can be slid, rotated and flipped, but not stretched or piled on top of one another. At first the workshop can handle any order: a parallelogram, a triangle, a trapezium, an arbitrary polygon, even a triangle that has to be turned into a square. Then two orders come in that it can’t fill, a disc and a cube, and it becomes clear what scissors are missing.
The workshop rules
The school definition, “area is how many little squares fit in a figure”, is fine for a rectangle. For a triangle the squares along the edges have to be cut, and for a disc they don’t fit at all. So mathematicians do something else: instead of explaining what area “really” is, they list its properties. Everything else is derived from them.
The area of a polygon is a number assigned to it by the four rules written below. The area of a disc and other figures with curved edges is defined through polygons that approximate the figure from inside and outside; how to do this carefully is told in the chapters on the integral and on measure.
- The area of any polygon is a non-negative number.
- Congruent polygons, that is, ones that can be made to coincide by a motion, have equal areas.
- If a polygon is made up of several polygons that don’t overlap, its area is the sum of their areas.
- The area of a square with side $1$ is $1$.
The fourth rule is an agreement about the unit: a centimetre, a metre or a square of an exercise book. But the famous “length times width” isn’t among the rules. It has to be proved.
The area of a rectangle with sides $a$ and $b$ is $ab$.
The plan: fill the rectangle with equal little squares, and where they don’t fit exactly, squeeze the area between two approximations.
The rules also give the workshop’s main property: if a figure is cut up and another is assembled from the pieces, the area doesn’t change. The pieces in the second figure are the same, only slid or rotated, so their areas are the same (rule 2), and each of the two figures has area equal to the sum of the areas of the pieces (rule 3). There are words for such pairs.
Two figures are equal in area if their areas are equal. Two polygons are equidecomposable if one can be cut into finitely many polygons and the other assembled from these pieces.
Equidecomposable polygons, as we’ve just seen, are equal in area. The workshop’s main question is the converse: if two figures are equal in area, can one always be re-cut into the other? For polygons the answer will be “yes”, and that’s not obvious at all. For a disc and a square it’s “no”, if you cut with scissors. And with volumes, scissors fail even for polyhedra.
Three re-cuts
The first orders are the figures whose areas are taught at school. Each formula can be derived with one or two cuts, and each time the figure turns into another whose area we already know.
The area of a parallelogram is a side times the height to that side.
The trick is to cut a triangle off the parallelogram and attach it on the other side.
The proof relied on luck: the point $H$ landed on the base. In a very slanted parallelogram the height falls outside, and the triangle we cut off no longer fits into place. A different cutting pattern comes to the rescue. Every horizontal line crosses the parallelogram in a segment of length exactly $a$. Cut the figure with vertical lines every $a$ units and slide the strips to the left by whole multiples of $a$. All the strips land in the same $a \times h$ rectangle, and the horizontal segments at each height join end to end, with no gaps and no overlaps. There are more pieces, but the method works for any slant.
A parallelogram has sides $5$ and $3$. What is its area?
The area is the base times the height, and the height depends on the angle between the sides. Squash the parallelogram flat and the height tends to zero; straighten it into a rectangle and the height grows to $3$. The area can be any number from $0$ to $15$, and exactly $15$ happens only for a rectangle.
The triangle. In chapter 17 the formula $S = \frac12 ah$ came from the fact that two identical triangles make a parallelogram. The workshop can do more: re-cut the triangle itself, without doubling it.
A triangle with base $a$ and height $h$ is equidecomposable with a parallelogram of base $a$ and height $\frac h2$. So $S = \frac12 ah$.
Cut the top off along the midline and rotate it about the midpoint of a side.
The trapezium. The same trick, a $180^\circ$ rotation about the midpoint of a side, turns it into a triangle.
The area of a trapezium with parallel sides $a$ and $b$ and height $h$ is $\frac{a + b}{2} \cdot h$.
Turn the trapezium into a triangle of the same height whose base is the sum of the trapezium’s parallel sides.
A plot of land is a trapezium: its parallel sides are $11$ m and $5$ m, and the distance between them is $6$ m. Find the area of the plot in square metres.
$S = \frac{11 + 5}{2} \cdot 6 = 8 \cdot 6 = 48$ m². Check by re-cutting: a triangle with base $11 + 5 = 16$ and height $6$ has area $\frac12 \cdot 16 \cdot 6 = 48$.
Squared paper
Draw on squared paper a polygon with its vertices at grid points. Its area can be found with no cutting at all, just by counting points: the grid points strictly inside and the grid points on the boundary (vertices count too). The formula was found in 1899 by the Austrian mathematician Georg Pick.
If all the vertices of a polygon without self-intersections or holes lie at the points of a square grid of side $1$, its area is $I + \frac B2 - 1$, where $I$ is the number of grid points inside and $B$ the number on the boundary.
Let’s show that the quantity $f = I + \frac B2 - 1$ behaves like area: it adds up under cutting and coincides with area for the simplest figures.
Why any polygon can be cut into triangles by diagonals
It’s enough to show that any polygon with more than three vertices has a diagonal lying entirely inside it: it cuts the polygon into two polygons with fewer vertices, and the process can be repeated. Take the leftmost vertex $V$ and its neighbours $U$ and $W$. The angle at $V$ is less than $180^\circ$: there’s nothing to the left of $V$. If triangle $UVW$ contains no other vertices of the polygon, the segment $UW$ is the diagonal we want. If it does, take the one farthest from the line $UW$; the segment from it to $V$ crosses no sides and will do too.
The formula collapses as soon as the conditions are broken. If a vertex isn’t at a grid point, the points no longer count what’s needed: try it in the widget. If the polygon has holes, one is added to the right side for each. And in space there’s no analogue at all: in 1957 the British mathematician John Reeve constructed tetrahedra with vertices at the points of a cubic lattice that have no lattice points inside or on the faces apart from the vertices, yet have arbitrarily large volume.
A triangle has vertices at the grid points $(0, 0)$, $(6, 0)$ and $(2, 4)$. How many grid points lie strictly inside it? Hint: the area is easy to find, and the grid points on the sides can be counted with greatest common divisors.
The area is $\frac12 \cdot 6 \cdot 4 = 12$. The side from $(0, 0)$ to $(6, 0)$ has $7$ grid points. The side from $(6, 0)$ to $(2, 4)$ goes with the shift $(-4, 4)$ and passes through $\gcd(4, 4) + 1 = 5$ grid points, and the side from $(2, 4)$ to $(0, 0)$ with the shift $(-2, -4)$ through $\gcd(2, 4) + 1 = 3$. We’ve counted each vertex twice, so $B = 7 + 5 + 3 - 3 = 12$. By Pick’s theorem $I = S - \frac B2 + 1 = 12 - 6 + 1 = 7$.
Any polygon into any other
So far the workshop has re-cut figures into ones whose area we already knew. The main question was broader: can any two polygons of equal area be re-cut into each other, say an L-shape into a regular pentagon of the same area? In the first third of the nineteenth century several people proved this independently. The theorem is named after two of them: the Hungarian mathematician Farkas Bolyai, father of János Bolyai, one of the creators of non-Euclidean geometry, and the German Paul Gerwien, who published a proof in 1833.
Any two polygons of equal area are equidecomposable.
The plan: learn to turn any polygon into a rectangular strip of width $1$. If we can do this for both polygons, the strips will come out identical, since the length of each equals the area, and all that’s left is to lay one cutting pattern over the other.
The proof gives a recipe, but a wasteful one: there are many pieces, and the less alike the figures, the more pieces. Finding the most economical dissections is a sport of its own, and its champion lived in England more than a hundred years ago.
The haberdasher and four pieces
Henry Dudeney (1857–1930) was perhaps the most inventive puzzle setter of his time. In 1902, in a newspaper column, he set the haberdasher’s problem: cut a piece of cloth shaped like an equilateral triangle into four parts that can be assembled into a square. In 1907 the problem went into his book The Canterbury Puzzles. The solution turned out more beautiful than anyone could have hoped: the four pieces can be hinged into a chain that folds now into the triangle, now into the square. Dudeney showed a mahogany model with brass hinges at a meeting of the Royal Society of London in 1905.
The cuts are found with compass and straightedge. A triangle with side $2$ has area $\sqrt3$, so the side of the square we need is $\sqrt{\sqrt3} = \sqrt[4]{3} \approx 1.316$. Such a segment is constructed as a geometric mean. Let $E$ be the midpoint of side $BC$; the median $AE$ has length $\sqrt3$. Extend it beyond $E$ by $EF = 1$ and draw a semicircle on $AF$ as diameter. The perpendicular to $AF$ at the point $E$ meets it at a point $H$, and $EH^2 = AE \cdot EF = \sqrt3$: triangle $AHF$ is right-angled because it stands on a diameter, and the altitude of a right triangle is the geometric mean of the pieces of the hypotenuse (this follows from the similarity of the two triangles the altitude divides it into). Then a circle of radius $EH$ centred at $E$ marks a point $J$ on side $AC$, the segment $JK = 1$ is laid off from it, and perpendiculars are dropped onto $EJ$ from $K$ and from the midpoint $D$ of side $AB$.
For more than a century nobody doubted that four pieces was the limit, but nobody could prove it either. Only in 2024 did Erik Demaine, Tonan Kamata and Ryuhei Uehara prove that a square can’t be made from an equilateral triangle in three pieces.
A disc that won’t be cut
The workshop has coped with polygons. Now the order it was really opened for: big question 2. A disc and a square of the same area: can the disc be cut into pieces and a square assembled from them? With scissors cutting in straight lines, no, and the reason can be seen with the naked eye.
A disc can’t be cut by straight cuts into finitely many pieces from which a square can be assembled.
The point is that every piece’s arcs bulge outwards, and for a bulging arc to have somewhere to go, its neighbour needs a hollow one.
It’s not only a matter of the cuts being straight: in 1963 the American mathematicians Lester Dubins, Morris Hirsch and Jack Karush proved that scissors cutting along any curves won’t help either. A square of the right area can’t be constructed with compass and straightedge either: that follows from the transcendence of $\pi$, proved by Lindemann in 1882 (chapter 6). And yet in 1990 the Hungarian mathematician Miklós Laczkovich proved that a disc can be cut into finitely many pieces and reassembled into a square, and the pieces don’t even need rotating, only sliding. It takes around $10^{50}$ pieces, and they aren’t shapes but bizarre clouds of points that can be neither drawn nor cut out. How this is possible, and why it doesn’t violate area, is explained in chapter 54: that’s where big question 2 will be closed.
The cube and the tetrahedron
Let’s move into space. Volume, like area, is given by rules.
The volume of a polyhedron is a number assigned to it by the same four rules as area: it’s non-negative, the same for congruent polyhedra, additive under cutting, and equal to $1$ for a cube of edge $1$.
The volume of an $a \times b \times c$ box is $abc$: the proof repeats the argument about the rectangle word for word, only with little cubes instead of little squares and three edges instead of two sides. It would be natural to expect a three-dimensional analogue of the Bolyai–Gerwien theorem too: any two polyhedra of the same volume can be cut into each other. Then the volume of any pyramid could be found by re-cutting it into a box.
But school textbooks derive the volume of a pyramid differently: through an infinite sequence of ever finer cuts, as Euclid did in Book XII of the Elements. Gauss, in letters to his student Christian Gerling, regretted that the volume of a pyramid couldn’t be found without such a limiting process. In 1900, at the International Congress of Mathematicians in Paris, David Hilbert named 23 problems for the new century, and the third was exactly this: find two tetrahedra with equal bases and heights that can’t be re-cut into each other. In the same year it was solved by Hilbert’s student Max Dehn. It was the first problem on the list to be solved.
A cube and a regular tetrahedron of the same volume are not equidecomposable.
The full proof needs tools the course will reach later, so here’s its idea. Dehn found a quantity that, like volume, doesn’t change under cutting and rearranging, but is different for the cube and the tetrahedron. For each edge of the polyhedron take its length and the dihedral angle at it, that is, the angle between the faces meeting at the edge, and form a “sum of lengths times angles”. The addition has to be done cleverly: angles that are a rational fraction of $180^\circ$ count as zero. Then a cut through an edge divides the angle at it into parts that add up to the original angle, and new edges inside the solid bring angles adding up to $180^\circ$ or $360^\circ$, that is, zero. All the dihedral angles of a cube are right angles, half of $180^\circ$, and its Dehn invariant is zero. The dihedral angle of a regular tetrahedron is $\arccos\frac13 \approx 70.53^\circ$, which is not a rational fraction of $180^\circ$, so its Dehn invariant isn’t zero. Defining such “addition up to rational fractions” carefully is made possible by vector spaces over the rational numbers (chapter 37). And in 1965 the Swiss Jean-Pierre Sydler proved the converse: if two polyhedra have the same volume and the same Dehn invariant, they can be re-cut into each other.
The conclusion for the workshop is discouraging: for volumes scissors alone aren’t enough, and a limiting process is needed, slicing into infinitely thin layers. Its handiest version fits into a stack of coins.
A stack of coins
Stack up some coins and push the stack from the side. It will lean and bend, but it won’t gain or lose any metal: the coins are the same. If the coins are infinitely thin, shifting the layers turns an upright cylinder into a slanted one or into any curved “snake”, and the volume stays the same. In 1635 the Italian monk and mathematician Bonaventura Cavalieri, a pupil of Galileo, made a method out of this observation in his book Geometry, Developed by a New Method Through the Indivisibles of the Continua.
Let two solids lie between two parallel planes, and let every plane parallel to them cut both solids in figures of equal area. Then the volumes of the solids are equal.
A rigorous proof needs the integral: in chapter 28 the volume of a solid turns out to be the “sum” of the areas of its cross-sections, $\int S(z)\,dz$, and equal cross-sections give equal integrals. Here’s the idea that suggests that integral. Slice both solids into $n$ layers of equal thickness $\frac hn$ with planes parallel to the given ones. Replace each layer with a “coin”, an upright cylinder whose base is the cross-section at the bottom of the layer. By hypothesis the bases of corresponding coins in the two solids have equal areas, and the thicknesses are equal too, so the stacks of coins have equal volumes. The thinner the layers, the more closely each stack follows its solid: the difference between the solid and the stack is a thin “fringe” along the edges of the layers, and its volume tends to zero. So the volumes of the solids are limits of the same quantity, and they’re equal.
Cavalieri had a predecessor at the other end of the world. In China, around the turn of the fifth and sixth centuries, Zu Geng, son of the astronomer Zu Chongzhi (the one who found the fraction $\frac{355}{113}$ for $\pi$), stated the same rule: if the areas of the cross-sections at every height are equal, the volumes can’t differ. With it he found the volume of a ball, a problem at which the commentator on the Nine Chapters, Liu Hui, had stopped more than two centuries earlier.
A prism is a polyhedron two of whose faces (the bases) are congruent polygons in parallel planes, and the other faces parallelograms. A cylinder is built the same way, only its bases are discs.
The volume of a prism or cylinder is the area of the base times the height: $V = Sh$, even if the solid is slanted.
Put next to it a box of height $h$ with an $S \times 1$ rectangle as its base. Any plane parallel to the bases cuts the prism in a polygon congruent to the base: a shift along the lateral edges takes the base to the cross-section. So the area of the cross-section is $S$, the same as for the box. By Cavalieri’s principle the volumes are equal, and the box’s volume is $S \cdot 1 \cdot h = Sh$. For a cylinder the argument is the same.
A pyramid is a third of a prism
A pyramid is a polyhedron one face of which is a polygon (the base) and the other faces triangles with a common vertex. The height of a pyramid is the distance from this vertex to the plane of the base. A cone is built the same way, only its base is a disc.
That a pyramid takes up a third of the prism with the same base and height was known long before any proofs. The Moscow Mathematical Papyrus, written around 1850 BC and kept in the Pushkin Museum of Fine Arts in Moscow, finds in problem 14 the volume of a truncated pyramid with square bases $4$ and $2$ and height $6$ by a rule equivalent to the formula $V = \frac h3\left(a^2 + ab + b^2\right)$: it comes out as $2 \cdot (16 + 8 + 4) = 56$. According to Archimedes, the statement about the third was first made by Democritus and proved by Eudoxus.
It’s clearest of all on a cube: a cube can be cut into three identical pyramids with a common apex.
Each of the three pyramids has an $a \times a$ square as its base and the edge $a$ as its height, and its volume is a third of the cube: $\frac13 a^3 = \frac13 \cdot a^2 \cdot a$. For the general case we’ll need Cavalieri’s principle and one lemma.
Two pyramids (or a pyramid and a cone) with equal base areas and equal heights have equal volumes.
Compare the cross-sections at the same height and apply Cavalieri’s principle.
The volume of a pyramid is a third of the base area times the height: $V = \frac13 Sh$. The volume of a cone with base radius $r$ and height $h$ is $\frac13 \pi r^2 h$.
Euclid’s idea (proposition XII.7): a triangular prism is cut into three pyramids, and by the lemma they have pairwise equal volumes.
An ice-cream cone is a cone with base radius $3$ cm and height $10$ cm. How many cubic centimetres of ice cream does it hold, level with the rim? You can write the answer using $\pi$ or as a decimal.
$V = \frac13 \pi r^2 h = \frac13 \cdot \pi \cdot 9 \cdot 10 = 30\pi \approx 94.2$ cm³. A cylindrical tub of the same size would hold three times as much, $90\pi \approx 282.7$ cm³.
A ball in a cylinder
A sphere of radius $R$ is the surface consisting of all points of space at distance $R$ from the centre. A ball is the solid bounded by a sphere: all the points at distance at most $R$ from the centre. A sphere has an area, a ball a volume.
In 75 BC the quaestor of Sicily, Marcus Tullius Cicero, tracked down Archimedes’ grave near Syracuse, overgrown with brambles. He recognised it by a column on which a sphere and a cylinder around it were carved. According to Plutarch, Archimedes himself asked for this figure to be put on his grave: the volume of a ball is two thirds of the volume of the cylinder around it, and he valued this result above all others. Let’s prove it with the tools we already have: cross-sections.
The volume of a ball of radius $R$ is $\frac43 \pi R^3$.
We need a solid that has the same cross-section as a hemisphere at every height, but whose volume we already know how to compute.
One watermelon is $30$ cm across, another $20$ cm. How many times more flesh does the first have, treating watermelons as balls?
The ratio of the radii is $\frac32$, and volume is proportional to the cube of the radius: $\left(\frac32\right)^3 = \frac{27}{8} \approx 3.4$. The first watermelon is only one and a half times “wider”, but it has more flesh than three of the second.
What’s left is the area of the sphere. It too can be got from the volume, by the same trick that gets the area of a disc from the circumference.
The area of a sphere of radius $R$ is $4\pi R^2$: exactly four times the area of a great circle.
Cover the sphere with a fine grid, like a globe with parallels and meridians, and join each cell to the centre. The ball falls into a multitude of thin “pyramids” with their apex at the centre. The base of each is a cell of the sphere, almost flat if the cells are small, and the height is almost $R$. The volume of a little pyramid is roughly a third of the area of the cell times $R$. Adding up all the pyramids, we get that the volume of the ball is roughly $\frac13 R \cdot S$, where $S$ is the area of the sphere. As the grid gets finer the error tends to zero, and the equation becomes exact: $\frac43 \pi R^3 = \frac13 R S$. Hence $S = 4\pi R^2$. The rigorous justification of such a passage to the limit is given by the integral.
The radius of a ball is doubled. By what factor does its volume grow?
$\frac43 \pi (2R)^3 = 8 \cdot \frac43 \pi R^3$: by a factor of $8$. The area of the sphere grows only by $4$, and each square centimetre of surface now has twice as much volume behind it. That’s why large animals cool down more slowly than small ones.
Take-home orders
The workshop is closing, but there are orders left. The trainer has three levels: areas of polygons by the formulas of this chapter; squared paper, where Pick’s theorem comes to the rescue; volumes of prisms, pyramids, cylinders, cones and balls.
Where next
Everything we measured in this chapter could be touched: cut up, rearranged, put on the scales. But some sizes are out of reach of both scissors and tape measure. The height of Everest was calculated by the surveyors of British India in 1856, almost a hundred years before Edmund Hillary and Tenzing Norgay first reached the summit in 1953. The surveyors themselves never went near the mountain: their instruments stood on the plains of India, more than a hundred kilometres away, and measured only angles. How to find distances and heights from angles, and the size of the whole Earth along with them, is the business of trigonometry.