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Chapter 11 · Introduction to Three Dimensional Geometry

Applying the right-triangle rule twice to get out of the plane

Measuring between points14 min

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14 min.

The distance formula in three dimensions looks like Pythagoras with an extra term stapled on. It is Pythagoras applied twice, in two planes meeting along one line.

The idea

The three-dimensional distance rule is not a new theorem; it is Pythagoras used twice. What makes the two-step argument work is a fact §11.4 asserts and never argues: the first right angle is not between two lines that happen to look perpendicular, it is between a segment and an entire plane. The segment PA runs along one axis direction, AQ lies wholly inside the plane through A that direction is perpendicular to, and so PA meets AQ at a right angle however AQ happens to be oriented inside that plane. Once that is said, the three squares that appear in the answer stop looking like a pattern to memorise: they are the three axis-parallel steps of a path from P to Q, and the box in Fig 11.4 exists only to make those three steps visible.

What you should be able to do

  • Describe the box Fig 11.4 builds on the segment PQ and identify the two extra corners the derivation needs
  • Write the path from P to Q as three moves, each parallel to one axis, and state the coordinates of the two intermediate points
  • State why the angle at the first intermediate corner is a right angle, using the segment-to-plane fact the chapter omits
  • State why the angle at the second intermediate corner is a right angle, and say which plane that one lives in
  • Combine the two Pythagoras statements and identify the quantity that cancels
  • Write the distance between two general points in space, and specialise it to a distance from the origin without treating that as a separate result
  • Compute a distance from two given triples, including cases where one or two coordinates agree
  • Decide whether three points lie on a line by comparing three computed lengths, and explain why the comparison is conclusive
  • Test a triangle for a right angle by checking all three of the possible pairings, and say why checking one is not enough
  • Test four points for being a parallelogram, and say why equal opposite sides alone does not settle it in space
  • Turn a stated condition on distances into an equation in three variables, by naming the moving point and expanding

Words to know

TermDefinition in one lineFirst introduced
distance formulathe rule §11.4 arrives at for the length of a segment in spaceprinted in Example 5, p. 212, and the rule itself in §11.4, p. 212
parallelopipedthe box the derivation builds on PQ, spelled this way on the pageprinted in §11.4, p. 211
diagonalthe segment joining two opposite corners of that box, here PQ itselfprinted in §11.4, p. 211
collinearlying on one straight lineprinted in Example 4, p. 212
equidistantat equal distances from two named pointsprinted in Exercise 11.2 q4, p. 213
isosceleshaving two equal sidesprinted in Exercise 11.2 q3(i), p. 213
centroidthe point Example 9 works with, at which the three medians of a triangle meetprinted in Example 9, p. 214, and Miscellaneous Exercise q3, p. 215
medianthe segment from a vertex to the middle of the opposite sideprinted in Miscellaneous Exercise q2, p. 215
locusthe set of all points satisfying a stated conditionnot printed in this chapter; the explanation uses it in section 12, where the chapter instead asks for an equation of a set of points
triangle inequalitythe rule that two sides of a triangle together exceed the third unless the three points are in a linenot printed in this chapter; the explanation needs it in section 10 to justify Example 4's argument, which the chapter states without support
section formulathe rule locating a point that divides a segment in a given ratio, from which the midpoint and centroid rules follownot printed in this chapter at all, although three Miscellaneous items require it — see section 12 and the notes below

Where people slip up

  • "The formula is Pythagoras with an extra term stuck on." It is Pythagoras applied twice, in two planes that meet along a line. The extra term is not decoration; it is the second triangle's contribution, and skipping the second triangle leaves the result unproved.
  • "You can see that the angle at A is a right angle, so it is." You cannot see it — the figure is a flat drawing of a solid, and drawn angles there are unreliable. The reason is that PA runs perpendicular to a whole plane containing AQ. Section 4 is the section that makes this a proof rather than an appeal to the picture.
  • "Both right angles are in the same plane." They are not, and if they were the argument would collapse into two dimensions. The two triangles share only the segment AQ.
  • "The coordinate differences are lengths, so they cannot be negative." As the chapter writes them, they can be. They are squared immediately, which is why nothing goes wrong, and saying so is cheaper than letting a student silently doubt the working.
  • "Swapping which point is first changes the distance." It negates all three differences at once, and squaring undoes that. The formula is symmetric in the two points.
  • "The derivation needs a real box, so it fails when two coordinates agree." The drawing fails; the formula does not. Exercise 11.2 q1(i) and q1(iv) are exactly these flattened cases, and both work out — worth checking rather than asserting.
  • "Adding two lengths and getting the third is a coincidence." It is a characterisation. Two distances can only add to the third when the middle point sits on the segment joining the other two; anything else leaves a genuine triangle and a strict inequality.
  • "One failed right-angle test settles it." Example 5 tests one of the three possible vertices and stops. A triangle has three angles, and any of them could have been the right one, so a complete answer needs all three checks. Do them — they are three additions.
  • "Equal opposite sides make a parallelogram." In the plane that is safe; in space it is not, because four points with matching opposite sides need not lie in one plane at all. This is why the chapter's own Note offers the diagonal argument.
  • "Every question in the chapter can be answered from the chapter." Three of the four Miscellaneous items need a rule for the midpoint or the centroid that this edition does not print anywhere in the chapter.
Transcript2,007 words

You already know how to measure between two dots on a flat sheet. Two steps at right angles, and the square on the join is the sum of the two squares. Now lift one of the dots off the sheet. The question is what genuinely has to be new, and the answer is: almost nothing. The rule for three dimensions is not a fresh theorem with an extra term bolted onto it.

It is the same theorem, used twice, in two flat surfaces that meet along a line. The one thing that really is new is a fact about a segment and a whole surface, not about two lines that happen to look square in a drawing. That fact usually gets asserted in a single clause and walked past. Everything downstream of it depends on it, so we are going to argue it instead.

Take two places and build a box on them, with the two places at opposite corners, so that the span you want is the box's long diagonal. Two of the other corners matter, and the rest are scenery. Call them the first stop and the second stop. Their triples almost never get written down, and without them nothing that follows can be argued at all. The first stop keeps the start's first and third entries and takes the far end's second.

The second stop keeps only the start's third. Run that on a start of one, minus three, four and a far end of minus four, one, two. The first stop comes out one, one, four, and the second stop minus four, one, four. Now every corner has a name and a triple, and we can start measuring. Walk from the start to the far end in three moves. Each move changes exactly one entry and leaves the other two completely alone, so each one runs along a single direction.

Measured: the first move changes the second entry, the second move changes the first, and the third move changes the third. Their squared sizes come out sixteen, twenty-five and four. Add them and you get forty-five. Now measure the whole span from the start to the far end directly, in the space itself, using no rule whatsoever. Forty-five again. That is the entire result in one line, and one line is not an argument.

A coincidence at one pair of places proves nothing. What has to be shown is why those three squares are forced. Here is the step that usually gets asserted. The angle at the first stop is a right angle. You cannot see that, and you should not believe a picture that tells you so. A flat drawing of a solid does not report angles honestly; the whole figure is a projection, and projections bend angles.

So here is why it is actually true. The first move changes only the second entry, so it runs along the second direction. The first stop and the far end share their second entry, so the entire join from the stop to the far end lies inside the flat surface through that stop on which the second entry never changes. And that surface is precisely the one the second direction turns its back on.

So the first move meets every single line of that surface at a right angle, whichever way the line happens to be pointing. Measured rather than asserted: a hundred and sixty-eight lines were drawn through that stop across the surface, three more were taken deliberately off it, and of those hundred and seventy-one the number met at anything other than a right angle is three. Exactly the three taken off.

Notice what the argument never mentions: where the far end is. The right angle is structural, not a feature of the drawing. The second right angle is easier, and the important thing about it is where it lives. The second move changes only the first entry; the third move changes only the third. Two different directions, square to one another, meeting at the second stop, so that corner is square as well.

But this second triangle sits inside the surface on which the second entry never changes, and the first triangle does not. Measured: the surfaces the two triangles span are not parallel, and of the four corners involved the number that both surfaces hold is two. Those two are the ends of the face diagonal. The triangles share that diagonal and nothing else at all. This is exactly why one application is not enough.

If both right angles had sat in one surface, the whole argument would have collapsed back into two dimensions and told you nothing new. Now put the two statements together. The first triangle says the square on the span is the square on the first move plus the square on the face diagonal. The second says the square on the face diagonal is the square on the second move plus the square on the third.

Substitute the second into the first. The face diagonal was on both sides of the working, and it leaves without a trace. Its squared size here is twenty-nine, which is a real length and not nothing, so watching it cancel is watching something actually happen. What is left is three squares, one for each move. That is the rule, and it arrived as a consequence rather than as an announcement.

Now name the three moves. Each one is simply a difference of two entries, and here a perfectly fair objection arrives. These are supposed to be lengths, and a difference can come out negative. In the running example the three differences are minus five, four and minus two. Two of the three are negative. Nothing goes wrong, because every one of them is squared immediately, and squaring throws the sign away before it can do any harm.

The same fact settles a second worry. Swapping which place you call first negates all three differences at once, and squaring undoes that too. Measured over twenty-nine pairs of places, the number where taking the two the other way round changes the answer is zero. One more thing that looks like a second rule and is not. Put the first place at the crossing where the three lines meet, the place whose three entries are all nothing.

Then every difference is just the far place's own entry, and the squared span is the sum of its three squared entries. For the far end of the running example that comes out twenty-one. Measured across all twenty-nine pairs, the number where pinning the first place at the crossing gives anything other than the second place's own three squares is zero. It is the same rule with one triple made nothing.

Learning it separately is learning the same thing twice. Now a case the picture simply cannot draw. If the two places happen to share an entry, the box has no thickness in that direction, and its eight corners collapse onto four. Here are four offered pairs. Their squared spans are twenty, forty-three, a hundred and four, and twenty. Count the corners each box manages to keep: four, eight, eight, four.

So two of the four have gone flat, and the very first pair offered is one of them. Of those two flattened cases, the number the rule gets wrong is zero. The drawing fails; the rule does not. The box was scaffolding for the argument, and it was never part of the answer. Three places, and a question: are they in a line? Measure the three squared spans: fourteen, fifty-six, and a hundred and twenty-six.

Now ask, exactly and with no rounding at any point, whether the two shorter lengths add to the longest. They do. And of the three ways of choosing which one to leave out, the number where the other two add up to it is one, which also names which place is in the middle. Why is that conclusive rather than a coincidence? Because for any three places at all, the two shorter lengths add to at least the longest, with equality only when the middle place sits on the join between the other two.

A genuine triangle offered alongside, with squared spans nine, twenty-five and sixteen, has zero of its three choosings work. The equality is not evidence of a line; it is what being in a line looks like when you measure it. Now a triangle, and the question of whether it has a right angle anywhere. The three squared spans are six hundred and eighty-six, four thousand five hundred and seventy-one, and two thousand seven hundred and nine.

The working you will usually see picks one corner, adds the two squares meeting there, compares against the third, gets three thousand three hundred and ninety-five against four thousand five hundred and seventy-one, and stops. But a triangle has three corners, and any one of them could have been the square one. So do the other two. Five thousand two hundred and fifty-seven against two thousand seven hundred and nine, and seven thousand two hundred and eighty against six hundred and eighty-six.

Both also fail. Of the three corners, the number that come out square is zero, and only now has the conclusion been earned. One test out of three is not an answer, it is a start. Here is a second triangle, and its squared spans are eighteen, eighteen and thirty-six. Two of them match, so it has two equal sides. And eighteen plus eighteen is thirty-six exactly, so it does have a right angle, sitting at the middle corner rather than the first.

Test the first corner only and you would have walked straight past it. Now something stranger. Negate the first and third entries of each of its places, and this triangle turns into another one that gets asked about separately, as though it were a different shape. It is not a different shape. Measured, that map has measure one rather than minus one, so it is a turn and not a flip.

The same triangle, rotated about the middle direction, asked about twice, and each answer is true of both. Four places now, and the question of whether they make a parallelogram. Measure the four sides: their squares come out thirty-six, forty-three, thirty-six and forty-three, so opposite sides match. In flat geometry that would settle it completely. In space it does not, and this is worth seeing rather than being told. Here is a second set of four places whose squared sides are sixteen, nine, sixteen and nine, opposite sides matching just as neatly, and whose four places do not lie on one flat surface at all.

Matching sides cannot see out of a plane. What settles it is the diagonals. For the first set, both diagonals have the same middle place; for the second set they do not, which is exactly how the test tells them apart. And the first set's two squared diagonals are three and a hundred and fifty-five, which differ, so it is a parallelogram and not a rectangle. Last, turn a condition into an equation.

Name the moving place, write its two squared spans to two fixed places, add them, and expand every bracket. Out comes three squared terms, three plain multiples, and a bare number of a hundred and nine that nobody wrote down anywhere. It fell out of six brackets. Ask instead for the places equally far from two fixed ones, and the squared terms cancel completely: the number of them surviving is zero, and what is left is flat.

That is the whole method, and it is the same expansion every time. One closing warning, and it is not about mathematics. Of four items offered at the end of this material, three need a rule for the middle of a join or for where a triangle's three joins meet. Those are two different rules, and neither of them appears anywhere in what came before. Exactly one of the four can be answered from what you were actually given.

Where this fits

Taken from the notes each video was made from, not from the reading order — these are the ideas this one rests on and the ones that later rest on it.

Builds on

Either side of this one

The book

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