PrepShorts · Study sheet · Class 9 Mathematics · Chapter 5, I’m Up and Down, and Round and Round
Chapter 5 · I’m Up and Down, and Round and Round
Total rotational symmetry, and why every diameter is an axis of reflection
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Watch a wheel go past twice and say which observation came first. You cannot, and that is the circle's symmetry doing its work.
The idea
The circle's symmetry is not an aesthetic remark; it is forced by the definition, and it is the reason later arguments are allowed to say "now turn the figure". The defining condition mentions one thing only — distance from the centre — so any motion that leaves every distance-from-the-centre unchanged must carry the circle onto itself. Turning about the centre does that for every angle, not just a chosen few, and reflecting in any line through the centre does it too. A square is carried onto itself by a short list of turns and has four axes; the circle has as many of each as there are numbers. That gap is where all of the chapter's later leverage comes from.
What you should be able to do
- Explain why a rotating wheel gives no way to tell one ground-contact point from another, and state the property this demonstrates
- State what complete rotational symmetry means, and contrast it with the finite rotational symmetry of a square, a regular pentagon and a regular hexagon
- Derive both symmetries from the defining condition rather than from a drawing
- Show by folding that a crease which brings the boundary onto itself must pass through the centre, and identify that crease as a diameter
- Say why every diameter is an axis, and why no other line is
- Give the length of the longest chord of a circle of stated radius, and explain what happens to chord length as the chord is pushed away from the centre
- Describe, as a locus, which points stand equally far from two given points, and say what has to be shown in each of the two directions for the claim to be complete
- Identify where in the chapter a symmetry argument is used, and where the chapter refuses to accept one
Words to know
| Term | Definition in one line | First introduced |
|---|---|---|
| rotational symmetry | the property of looking unchanged after being turned about a point | printed in §5.2, p. 94, and in the Chapter Summary, p. 117 |
| reflection symmetry | the property of looking unchanged after being flipped across a line | printed in §5.2, p. 94, and in the Chapter Summary, p. 116 |
| diameter | a chord that runs through the centre; here, each axis of reflection | printed in bold in §5.1, p. 93, and again in bold in §5.2, p. 94 |
| perpendicular bisector | the line cutting a segment in half at right angles | printed in the Think and Reflect hint, §5.2, p. 94 |
| locus | every point meeting a stated condition, gathered into one set | printed in bold in §5.1, p. 93; used again in §5.2, p. 94 |
| chord | a segment with both ends on the circle | printed in bold in §5.1, p. 93 |
| crease | the fold line left in the paper, standing in for an axis | printed in §5.2, p. 94, and repeatedly in §5.6, p. 102 |
| equidistant | at the same distance from | printed in §5.1, p. 93, and in the §5.2 hint, p. 94 |
| regular pentagon / regular hexagon | five- and six-sided figures with all sides and all angles equal | printed in Think and Reflect, §5.2, p. 94 |
| order of a rotational symmetry | the explanation's phrase for how many distinct turns carry a figure onto itself | an added term; §5.2 asks for the square's rotational symmetries and never names the count |
| distance-preserving motion | the explanation's label for a turn or flip that changes no distance | an added vocabulary; the chapter argues from symmetry without classifying the motions |
Where people slip up
- "Rotational symmetry means a few special angles." For a polygon, yes. For a circle, every angle works, and that is the difference the chapter is pointing at. A student who answers "the circle has rotational symmetry of order 4" because the picture looks like it has has missed the point entirely.
- "Only the horizontal and vertical diameters are axes." Every diameter is, because the fold can be started anywhere on the boundary. Textbook figures drawn axis-aligned make this hard to see.
- "Any line of symmetry of a circle is a diameter, so any line through the centre is a diameter." Careful: a diameter is a chord, hence a segment with its ends on the circle. The whole line through the centre is longer than the diameter it contains. The chapter uses "diameter" for the chord.
- "The fold shows it, so it is proved." The chapter itself blocks this reasoning two pages later. At the top of p. 103 it says plainly that a statement holding on many examples is not thereby true in general, and then gives an argument. Fold-and-look motivates; it does not license.
- "There must be a shortest chord." There is no shortest chord of positive length — lengths run down towards zero without ever reaching a smallest positive value. Students reach for "the shortest chord is the radius", which is not even a chord.
- "Symmetry can replace congruence." In this chapter the symmetry argument is always followed by a congruence argument — Theorem 6 on p. 103 is the clearest case. Symmetry tells you what to expect; the congruence tells you why.
- "Equidistant from two points means at the midpoint." The midpoint is one such point. The set is a whole line, and §5.3 depends on that.
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Worked answers to this chapter’s exercises · this video explains End-of-Chapter Exercises Q22, End-of-Chapter Exercises Q25
Transcript1,438 words
Watch a wheel go past, and note the point of the tyre that is touching the road. Look again a moment later, and note the point touching the road then. Now try to say which of those two observations came first. You cannot. Nothing about the wheel distinguishes them. That is not a remark about wheels. It is a fact about circles, and it is the strongest tool this whole subject has.
If turning a figure leaves you unable to tell the before from the after, then the turn changed nothing you could measure. So the question worth asking is how many turns do that, and the answer for a circle is unlike the answer for anything else you have met. A square has rotational symmetry. Turn it a quarter of the way round and it sits back down on itself, exactly as it was.
Turn it an eighth of the way round and it does not. So for a square the symmetry is a short list of angles, and between the entries on that list, nothing works at all. For a circle there is no list. Turn it one degree and it lands on itself. Turn it a hundredth of a degree and it lands on itself. Turn it by any amount you can name, and by any amount you cannot.
That is what complete rotational symmetry means. Not many angles. Every angle. The reason is one line long, and it is worth having exactly. A circle is the set of points at one fixed distance from one fixed point. The condition mentions distance from the centre, and it mentions nothing else. It says nothing about which way round the figure happens to be sitting. So take any motion that leaves every distance from the centre exactly as it was.
Every point that passed the test still passes it. Every point that failed still fails. The set comes back identical, and turning about the centre is exactly such a motion. Not because a circle looks round. Because the condition it is built from cannot see a rotation happening. Then the centre had better be the centre. Turn the circle about a point one unit off to the side instead. The image is still a circle of exactly the same size, but it is sitting somewhere else.
Two circles the same size with different middles cross at two points and no more. So a quarter turn about a point one unit out keeps two points of the circle and moves every other one off it. Push the pivot out to seven units and it still just clips, at two points. Push it to eight and the image misses the original completely. Nothing survives. The centre is not a convenience in that definition. It is the only pivot there is.
Reflection next, and this one you can do with your hands. Cut a disc out of paper. Fold it so that the boundary comes down on the boundary. Not roughly. Exactly. Press the crease flat, and open it out again. If you have ever been handed a paper circle and asked to find its middle without measuring anything, that fold is the answer. Now do it again in a different direction. The two creases cross at one point, and that point is the centre.
One more fold, in any direction at all, and the third crease runs through it too. Which is a fine thing to watch, and no reason at all to believe it. So why must the crease pass through the middle? Take one that does not. Reflecting in it slides the whole circle sideways, onto a circle of the same size with a different centre. And those two cross at two points. Two. Not the whole boundary.
So folding along a chord that misses the centre brings exactly two points of the edge back, and leaves all the rest hanging over. You can see the overhang in the paper. Slide the crease closer in and it is still two. A hundredth of a unit off centre is still two. Only when the miss is exactly nothing does the whole boundary come back. So the creases that work are exactly the lines through the centre.
And a line through the centre cuts the circle at two points, with a segment between them. That segment is a diameter. Every diameter is an axis of symmetry, and nothing that is not a diameter is one. Be careful with the wording, though. The crease is a whole line, and it runs off the edge of the paper in both directions. The diameter is the chord. The piece with both of its ends on the circle.
The line is longer than the diameter sitting inside it, and calling them the same thing will cost you later. And since the fold can be started anywhere on the boundary, there are as many axes as there are directions to point in. Put numbers against it. Not counting the turn that does nothing at all, a square comes back to itself after three turns, and it has four lines of symmetry.
A regular five-sided figure: four turns, five lines. A six-sided one: five turns, six lines. The pattern is obvious, and the obviousness is the point. The count is tied to the number of sides, so it is always finite. Now run twenty-seven different exact turns past a circle. All twenty-seven work. Run those same twenty-seven past a square, and three of them work. Same test, same turns. A circle is not a polygon that happens to have a lot of sides.
The symmetry earns its keep immediately. Take a circle of radius five and ask for its longest chord. The answer is ten, and it is a diameter, and you can see why without any algebra at all. Any chord that misses the centre gets cut short at both ends. So push a chord away from the middle and watch it shrink. Three units out from the centre, the chord measures eight.
Four units out, it measures six. Four point nine out, almost touching the edge, and it is under two units long. Every step outwards, shorter. The diameter is the one chord that gives nothing away, because it is the one that does not miss. So is there a shortest chord? The tempting answer is the radius, which is not a chord at all. It has only one end on the circle.
The honest answer is that there is no shortest one. Name any chord you like. Move it half of the remaining distance out towards the edge. That is still a chord, it still has a length, and it is shorter than the one you named. You can do that from anywhere, and you can do it again to whatever you get. The lengths run down towards nothing without ever arriving, so there is no smallest one to find, and looking for it is looking for something that is not there.
One more set built out of a condition, and a warning attached to it. Mark two points, and ask which points stand equally far from both. The middle of the segment joining them qualifies, but it is not the answer. The answer is a whole line: the one cutting that segment in half at right angles. And here is the warning. Showing that every point on that line stands equally far from both is only half of the job.
You have also to show that nothing off the line does. Skip the second half and all you have shown is that the line is inside the answer, not that it is the answer. Those are different claims, and only one of them is what was asked for. Which brings us to what symmetry is for, and what it is not for. A fold is persuasive. It is not a proof. Here is a case in point.
A crease two and a half units off the centre crosses the circle at exactly two points. But neither of those two lands on a whole number. So if you were checking by marking the whole-number points on the boundary, you would find nothing at all coming back, and conclude the crease misses the circle entirely. Move the crease out to three units and the very same check finds both of them.
The counting was right once and wrong once, and it looked equally convincing on both occasions. What settled it each time was the argument, not the count. Symmetry tells you what to expect. It does not tell you that you are right.
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
- Turning an observation into a definition: the circle as a locusClass 9 · Ch 5, I’m Up and Down, and Round and Round
Comes up again in
- Two points: infinitely many circles, centres on the perpendicular bisectorClass 9 · Ch 5, I’m Up and Down, and Round and Round
- Chords of equal length cut off equal central angles, and the converse (Theorems 2–3)Class 9 · Ch 5, I’m Up and Down, and Round and Round
- The centre-to-midpoint line is perpendicular, and the converse (Theorems 4–5)Class 9 · Ch 5, I’m Up and Down, and Round and Round
- Length and distance from the centre are the same fact twice (Theorems 6–8)Class 9 · Ch 5, I’m Up and Down, and Round and Round