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The Inscribed Angle Theorem

How to use
  1. ▶ Play runs the proof, Next → and ← Back step one scene at a time, Reset restores the opening scene and the original figure. Learn more about the controls
  2. Slide BB or CC round the circle, drag AA to change the radius or OO to move the circle; the readout under the canvas keeps the angle at OO at twice the angle at CC. Learn more about why it holds
  3. Labels toggles the point names, Measures writes each angle's size beside its arc. The Step explanations log keeps every step so far. Learn more about reading a scene
Proof?Draw the diameter from C through the centre O. It splits the angle at C into α and β, and the angle at O into two parts. Triangle OCA is isosceles, so ∠OAC = α, and the exterior angle at O is α + α = 2α; the same on the other side gives 2β. So the angle at the centre is 2(α + β), twice the angle at the circle. Slide A, B or C round the circle.Inscribed angle theorem
Display
Drag B or C round the circle, A for the radius, O for the centre
αβ2α2βOABC
∠AOB 126.2° = 2 × ∠ACB 63.1°
Step 1 / 6

Step explanations

1Angle at the circle, angle at the centre
Given
A, B, C lie on a circle with centre O. The inscribed angle ∠ACB and the central angle ∠AOB stand on the same arc AB. To prove: ∠AOB = 2 ∠ACB.
Both angles stand on the arc AB that does not contain C. Learn more about the statement




Getting Started with the Visualizer

DemoA run through the proof player
Step 0 of 7
Step through the proof, then slide the points round the circle to see that the angle at the centre stays exactly twice the angle at the circle. The picture below is the player with its parts numbered; the other tabs list what can be dragged, what each control does and what the step log shows.
Opening scene: the controls
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1Proof — the theorem loaded in the player; the ? gives its idea in one line
2Display — Labels shows the point names, Measures writes each angle's size beside its arc
3Draggable points — B and C slide round the circle, A sets the radius, O moves the circle; the hollow point D is the far end of the diameter through C
4Readout — the line under the figure: the angle at O against twice the angle at C, live while you drag
5Back, Play, Next, Reset — step through the proof or run it; Reset returns to step 1 and restores the original figure
6Speed and step counter — how fast Play advances, and which of the 6 steps is on screen
7Step explanations — every step reached so far, with its justification tag and a link to the section that explains it; click an entry to jump back to it
Proof complete: step 6 of 6
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1The central angle — at O, in two parts 2α and 2β on either side of the diameter
2The inscribed angle — at C, in two parts α and β; each part at O is twice the matching part at C
3The diameter CD — through the centre to the hollow point D; the line that splits both angles
4Justification tags — Given, Construction, Isosceles base angles, Exterior angle theorem, Same argument, Adding the parts
5Replay — at the last step Play becomes Replay and Next is off

The Statement

Take three points AA, BB, CC on a circle with centre OO. The angle ∠ACB\angle ACB, with its vertex on the circle, is an inscribed angle; the angle ∠AOB\angle AOB, with its vertex at the centre, is a central angle. Both stand on the same arc ABAB, the one that does not contain CC. The theorem, Proposition 20 of Book III of Euclid's Elements, says

∠AOB=2⋅∠ACB\angle AOB = 2 \cdot \angle ACB


the angle at the centre is twice the angle at the circle. Two things follow at once and are worth saying now: the inscribed angle does not depend on where CC is on its arc, since ∠AOB\angle AOB does not move; and when ABAB is a diameter the central angle is 180°180°, so the inscribed angle is 90°90°, which is Thales' theorem.

The proof on this page covers the case where the centre lies inside the inscribed angle, the one the player keeps you in. The other cases, centre on a side or outside the angle, use the same two ideas with a subtraction instead of an addition; see Why It Holds. The readout under the canvas shows both angles in degrees, live while you drag.
αβ2α2βOABC
Opening scene, frozen

A, B, C on the circle; the inscribed angle at C and the central angle at O, each shown in two parts.


The Diameter

The construction is the diameter through CC: join CC to the centre OO and extend the line to the point DD on the far side of the circle. In the player DD is hollow, because it is built from CC and OO and follows them.

The diameter does two things at once. It splits the inscribed angle at CC into two parts, α=∠ACD\alpha = \angle ACD on the side of AA and β=∠DCB\beta = \angle DCB on the side of BB; and it splits the central angle at OO into ∠AOD\angle AOD and ∠DOB\angle DOB. The proof will show that each part at OO is twice the matching part at CC. It also brings in the radii OAOA, OBOB and OCOC, all equal because they are radii (one tick each), which is what makes the two triangles OACOAC and OBCOBC isosceles.
αβ2α2βOABCD
The diameter, frozen

CD through O; the radii OA, OB, OC marked equal.


An Isosceles Triangle

In triangle OACOAC the sides OAOA and OCOC are radii, so they are equal and the triangle is isosceles with apex OO. By the isosceles base angles theorem its base angles are equal:

∠OAC=∠OCA=α\angle OAC = \angle OCA = \alpha


The angle at CC here is the part α\alpha of the inscribed angle on the side of AA; the angle at AA is new and is marked in the same colour. This is the same opening move as in Thales' theorem, where the two isosceles triangles on the radii did all the work.
αβ2α2βαOABCD
The isosceles triangle, frozen

OAC with OA = OC: the base angles at A and at C are both α.


The Exterior Angle

Since CC, OO and DD lie on one line, the angle ∠AOD\angle AOD at OO lies outside triangle OACOAC, between the side OAOA and the extension ODOD of the side COCO: it is an exterior angle of that triangle. By the exterior angle theorem it equals the sum of the two remote interior angles, which are α\alpha at AA and α\alpha at CC:

∠AOD=α+α=2α\angle AOD = \alpha + \alpha = 2\alpha


This is the whole mechanism of the proof: the isosceles triangle doubles the angle α\alpha by producing a second copy of it at AA, and the exterior angle collects both copies at the centre. The player highlights the three angles involved.
αβ2α2βαOABCD
The exterior angle, frozen

∠AOD is an exterior angle of triangle OAC: α + α = 2α.


The Other Side

The same two steps on the side of BB. Triangle OBCOBC has OB=OCOB = OC, so it is isosceles and ∠OBC=∠OCB=β\angle OBC = \angle OCB = \beta; and ∠DOB\angle DOB is an exterior angle of triangle OBCOBC at OO, so

∠DOB=β+β=2β\angle DOB = \beta + \beta = 2\beta


Both parts of the central angle are now known: ∠AOD=2α\angle AOD = 2\alpha and ∠DOB=2β\angle DOB = 2\beta, each twice the part of the inscribed angle on its own side of the diameter.
αβ2α2βαβOABCD
The other side, frozen

The same on the side of B: ∠OBC = β and ∠DOB = 2β.


Why It Holds

Add the two parts at OO and the two parts at CC:

∠AOB=∠AOD+∠DOB=2α+2β=2(α+β)=2⋅∠ACB\angle AOB = \angle AOD + \angle DOB = 2\alpha + 2\beta = 2(\alpha + \beta) = 2 \cdot \angle ACB


which is the statement. The end-of-proof mark ∎ in the log closes the argument. The tags name the facts used: the given circle, the diameter through CC with its equal radii, the isosceles base angles, the exterior angle theorem, the same two once more, and an addition.

The other two cases need one change. If OO lies on a side of the inscribed angle, say on CBCB, then β=0\beta = 0 and the first half of the proof is already the whole proof: ∠AOB=2α\angle AOB = 2\alpha. If OO lies outside the inscribed angle, both AA and BB are on the same side of the diameter CDCD; the two exterior angles are still 2α2\alpha and 2β2\beta, but now the central angle is their difference, 2β−2α=2(β−α)2\beta - 2\alpha = 2(\beta - \alpha), and the inscribed angle is β−α\beta - \alpha. Twice, in every case.
αβ2α2βαβOABCD
The conclusion, frozen

The two parts at O and the two parts at C: ∠AOB = 2α + 2β = 2∠ACB.


Dragging the Figure

Slide CC along its arc: α\alpha and β\beta trade places, the diameter swings round, and the readout keeps ∠AOB\angle AOB at exactly twice ∠ACB\angle ACB; and since ∠AOB\angle AOB does not change while CC moves on its arc, neither does ∠ACB\angle ACB. Slide BB to change the arc, or drag AA to change the radius and OO to move the circle.

The player keeps the figure in the case the proof covers: a drag that would carry CC past the diameter through AA or BB, putting the centre outside the inscribed angle, is refused, as is a drag that would flatten one of the triangles. The angle sum α+β\alpha + \beta at CC is always less than 90°90° in this case, since 2(α+β)2(\alpha + \beta) must fit inside a straight angle at OO.
αβ2α2βαβOABCD
After dragging, frozen

C slid along its arc and B moved: α and β have changed, the angle at the centre is still twice the angle at the circle.


Consequences

• Thales' theorem. When ABAB is a diameter the central angle is 180°180°, so every inscribed angle on it is 90°90°; see its own page.
• Angles in the same segment. All inscribed angles standing on the same arc are equal, since each is half of the same central angle. This is Euclid III.21 and the key to most circle problems.
• Cyclic quadrilaterals. For a quadrilateral inscribed in a circle, two opposite angles stand on arcs that together make the whole circle, so their central angles add up to 360°360° and the inscribed angles add up to 180°180°.
• Tangent and chord. The angle between a tangent and a chord equals the inscribed angle on the other side of the chord, the limiting case as CC slides into the point of tangency.