Overview

In this section we'll be talking about angle chasing; the basic of olympiad geometry.

Angle chasing, as the name suggests, is about calculating angles. Angle chasing is the core of synthetic geometry, as it is related to some facts about lines and circles. More precisely,

  • Three points AA, BB, CC are collinear in this order, iff ∠ABC=0∘\angle ABC=0^\circ.
  • Four points AA, BB, CC, DD are concyclic in this order, iff ∠ABD=∠ACD\angle ABD=\angle ACD. (But ∠ABC=180∘−∠ADC\angle ABC=180^\circ -\angle ADC nontheless; we'll talk about this later).
  • Similar triangles! You should know SS, SAS, and ASA.

In most of the geometry problems, in order to prove the result, you will need to find the ``hidden'' line or circles, four points are concyclic, three points are collinear, etc. where angle chasing is one of the used way to prove those.

Directed angles

The most annoying issue about olympiad geometry is the configuration issue; let us introduce the example of that.

Example 1: Let AA, BB, XX, YY be four points on the plane.

  • If XX, YY is on the same side with respect to the line ABAB, those four are concyclic iff ∠AXB=∠AYB\angle AXB=\angle AYB.
  • If XX, YY is on the different side with respect to the line ABAB, those four are concyclic iff ∠AXB=180∘−∠AYB\angle AXB=180^\circ -\angle AYB.

Doesn't this look annoying? This means that if we use angles are usual, we sometimes need a casework about configuration issues. So, here's the trick. What if we make angles directed, mod 180∘180^\circ?

Definition 2: We define directed angles of ∠XYZ\angle XYZ, denoted as ∡XYZ\measuredangle XYZ, as follows:

  • The angle is taken modulo 180∘180^\circ, that is, ∡XYZ=∡XYZ+180∘=∡XYZ+180∘⋅2=…\measuredangle XYZ=\measuredangle XYZ +180^\circ=\measuredangle XYZ +180^\circ \cdot 2=\dots and so on. (Be careful that we use the "==" instead of "≡\equiv ". We somehow write 0∘=180∘0^\circ =180^\circ in terms of directed angles, but not 0∘≡180∘(mod180∘)0^\circ \equiv 180^\circ \pmod {180^\circ}).
  • We have ∡XYZ=∠XYZ\measuredangle XYZ=\angle XYZ iff XX, YY, and ZZ are in clockwise order, and ∡XYZ=−∠XYZ\measuredangle XYZ=-\angle XYZ otherwise.

What is this so cool about? Indeed, we have that:

Rephrased Example 1: Let AA, BB, XX, YY be four points on the plane. The four points are concyclic if and only if ∡AXB=∡AYB\measuredangle AXB=\measuredangle AYB.

So clean, right? Try to confirm that this is true by caseworking on configurations. this feels like considering complex roots in the polynomial.

Now you know how powerful the directed angle is, let me introduce some properties about directed angles. When you read this, try to confirm this by your sel (and also that it fails when we change ∡\measuredangle with ∠\angle).

  • We have ∡AOP+∡POB=∡AOB\measuredangle AOP+\measuredangle POB=\measuredangle AOB.
  • We have ∡ABC+∡BCA+∡CAB=0∘\measuredangle ABC+\measuredangle BCA+\measuredangle CAB=0^\circ.
  • Let QQ be any point. Then AA, PP, BB are collinear if and only if ∡APQ=∡BPQ\measuredangle APQ=\measuredangle BPQ.

If you think these are too much, don't worry, you'll get used to it. (Also note that directed angles are the "rewrite" technique, rather than a brand new theorem.) Read https://web.evanchen.cc/faq-contest.html#C-11 for more details.

When during contests, I recommend you to define directed angles before using it, they're somehow still not common (but getting popular these days).

Configurations

Using angle chasing, we'll be dealing with example problems, as well as introducing famous configuration that you should know.

Example 1: Orthocenter configuration

Let ABCABC be a triangle. Recall, the orthocenter is the intersection of the altitudes, say, ADAD, BEBE, and CFCF. Standardly, we denote the orthocenter as HH.

This still begs the question: why do the three altitudes concur at the aforementioned point. To show this holds, we use Ceva's theorem. Note the following observations:

  • BD=AB⋅sin⁡(B)BD = AB \cdot \sin(B) and CD=AC⋅sin⁡(C)CD = AC \cdot \sin(C) from right triangles ABDABD and ACDACD.
  • CE=BC⋅sin⁡(C)CE = BC \cdot \sin(C) and AE=BA⋅sin⁡(A)AE = BA \cdot \sin(A) from right triangles BCEBCE and BAEBAE.
  • AF=CA⋅sin⁡(A)AF = CA \cdot \sin(A) and BF=CB⋅sin⁡(B)BF = CB \cdot \sin(B) from right triangles CAFCAF and CBFCBF.

Therefore, as

BDCD⋅CEAE⋅AFBF=AB⋅sin⁡(B)AC⋅sin⁡(C)⋅BC⋅sin⁡(C)BA⋅sin⁡(A)⋅CA⋅sin⁡(A)CB⋅sin⁡(B)=1,\dfrac{BD}{CD} \cdot \dfrac{CE}{AE} \cdot \dfrac{AF}{BF} = \dfrac{AB\cdot \sin(B)}{AC\cdot \sin(C)}\cdot \dfrac{BC\cdot \sin(C)}{BA\cdot \sin(A)}\cdot \dfrac{CA\cdot \sin(A)}{CB\cdot \sin(B)} = 1,

then ADAD, BEBE, and CFCF concur at a single point, due to Ceva's Theorem. As remarked previously, this point is the orthocenter, usually denoted by HH.

With the knowledge of the existence of the orthocenter, we can now show you all the magic properties of the orthocenter! As the title suggests, we will use angle chasing to discover a bunch of slick properties!

Here is an outline of a sample angle chase with the goal of determining ∠BHC\angle BHC, in terms of ∠BAC\angle BAC.

  • Note that ∠BHC=∠DHB+∠DHC\angle BHC = \angle DHB + \angle DHC.
  • However, ∠DHB=∠ACB\angle DHB = \angle ACB as △BHD∼△BCE\triangle BHD \sim \triangle BCE and ∠DHC=∠ABC\angle DHC = \angle ABC as △CHD∼△CBF\triangle CHD \sim \triangle CBF.
  • Hence, ∠DHB+∠DHC=∠ACB+∠ABC=180∘−∠BAC\angle DHB + \angle DHC = \angle ACB + \angle ABC = 180^{\circ} - \angle BAC.
  • Putting all this together, then ∠BHC+∠BAC=180∘\angle BHC + \angle BAC = 180^{\circ}.

We have sure seen this property before where two angles sum to 180∘180^{\circ}! That being, when two angles sum to 180∘180^{\circ}, it usually means two angles are cyclic! I say usually because in this case ABHCABHC is concave. In particular, ∠BHC\angle BHC in the above proof actually corresponds to the angle outside of the quadrilateral ABHCABHC. And so, this actually means the reflection of HH over BCBC, which we will denote by H′H', lies on the circumcircle of ABCABC. In addition, the reflection of HH over the midpoint of BCBC, which we will denote by H′′H'', lies on the circumcircle of ABCABC, as well. Both are due to the fact that

∠BHC=∠BH′C=∠BH′′C.\angle BHC = \angle BH'C = \angle BH''C.

Nealty enough, this yields us to some further conclusions! First, introduce the circumcenter of the circumcircle of ABCABC which we will denote as OO. Consider the following outline of observations:

  • As H′H' and H′′H'' are both reflections of some sort of HH over some point on line BCBC, then the distances of H′H' and H′′H'' from BCBC are equal. Hence, H′H′′∥BCH'H'' \parallel BC.
  • In addition, as AH⊥BCAH \perp BC and AA, HH, and H′H' are collinear, then AH′⊥BCAH' \perp BC.
  • So, AH′⊥H′H′′AH' \perp H'H'', and finally ∠AH′H′′=90∘\angle AH'H'' = 90^{\circ}.
  • Remarkably, this implies OO lies on AH′′AH'' as AH′′AH'' would be the diameter of the circumcircle of ABCABC.

With that being said, this wraps our mini exploration into the orthocenter all thanks to our first angle chase!

Example 2: Incenter configuration

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Examples

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Practice Problems

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