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Ceva's Theorem

Giovanni Ceva (1648-1734) proved a theorem bearing his name that is seldom mentioned in Elementary Geometry courses. It's a regrettable fact because not only it unifies several other more fortunate statements but its proof is actually as simple as that of the less general theorems. Additionally, the general approach affords, as is often the case, rich grounds for further meaningful explorations.

 

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Ceva's Theorem

In a triangle ABC, three lines AD, BE and CF intersect at a single point K if and only if

(1) AF/FB · BD/DC · CE/EA = 1

(The lines that meet at a point are said to be concurrent.)

Proof 1

Extend the lines BE and CF beyond the triangle until they meet GH, the line through A parallel to BC. There are several pairs of similar triangles: AHF and BCF, AEG and BCE, AGK and BDK, CDK and AHK. From these and in that order we derive the following proportions:

  AF/FB = AH/BC (*)
CE/EA = BC/AG (*)
AG/BD = AK/DK
AH/DC = AK/DK

from the last two we conclude that AG/BD = AH/DC and, hence,

  BD/DC = AG/AH (*).

Multiplying the identities marked with (*) we get

 
AF/FB · BD/DC · CE/EA= AH/BC · BC/AG · AG/AH
 = (AH·BC·AG)/(BC·AG·AH)
 = 1

Therefore, if the lines AD, BE and CF intersect at a single point K, the identity (1) does hold. Which is to say that the fact of the three lines intersecting at one point is sufficient for the condition (1) to hold. Let us now prove that it's also necessary. This would constitute the second part of the theorem. In other words, let us prove that if (1) holds then AD, BE, CF are concurrent.

Indeed, assume that K is the point of intersection of BE and CF and draw the line AK until its intersection with BC at a point D'. Then, from the just proven part of the theorem it follows that

  AF/FB · BD'/D'C · CE/EA = 1

On the other hand, it's given that

  AF/FB · BD/DC · CE/EA = 1

Combining the two we get

  BD'/D'C = BD/DC or
BD'/D'C + 1= BD/DC + 1 or
(BD' + D'C)/D'C = (BD + DC)/DC

Finally

  BC/D'C = BC/DC

which immediately implies D'C=DC. That is, D' and D are one and the same point.

Q.E.D.

Proof 2

Triangles CKD and BKD have a common altitude hK from K. For their areas we therefore have Area(ΔCKD) = DC·hK/2 and Area(ΔBKD) = BD·hK/2, from which

(2) BD/DC = Area(ΔBKD)/Area(ΔCKD)

Similarly, on considering triangles ACD and ABD,

(3) BD/DC = Area(ΔABD)/Area(ΔACD)

From (2) and (3) we derive

(4) BD/DC = Area(ΔAKB)/Area(ΔAKC)

The latter is a key identity because two similar ones could be written starting with the other two sides:

  AF/FB = Area(ΔAKC)/Area(ΔBKC)
CE/EA = Area(ΔBKC)/Area(ΔAKB).

All we need now is to multiply the three identities.

Proof 3

This proof is by Darij Grinberg and appeared at the geometry-college newsgroup. It is also available at his personal site.

 

For this proof I changed the notations somewhat. The three lines through the point K are now AA', BB' and CC'. Draw through K three lines -- AcBc||AB, BaCa||BC, and AbCb||AC, as shown in the diagram.

First off, since say, triangles ACC' and BcCK are similar as are triangles BCC' and AcCK, we have

  AC'/BcK = CC'/CK, and C'B/KAc = CC'/CK,

which gives

(5) AC'/C'B = BcK/KAc.

From similar triangles ABB' and BcKB' we get

  BcK/AB = KB'/BB',

while similarity of triangles ABA' and KAcA' yields

  KAc/AB = KA'/AA'.

The latter two identities combine into

  BcK/KAc = KB'/KA' : BB'/AA',

or, taking (5) into account,

(6c) AC'/C'B = KB'/KA' : BB'/AA'.

Cyclically, we also have

(6a)BA'/A'C = KC'/KB' : CC'/BB' and
(6b)CB'/B'A = KA'/KC' : AA'/CC'.

The product of the three is the Ceva identity

  AC'/C'B · BA'/A'C · CB'/B'A = 1.

Remark 1

Ceva's theorem is the reason lines in a triangle joining a vertex with a point on the opposite side are known as Cevians.

Remark 2

The points D, E, F may lie as well on extensions of the corresponding sides of the triangle, while the point of intersection K of the three cevians may lie outside the triangle. The proof remains the same for all possible configurations as long as all the points involved remain finite. Please look into this circumstance.

Remark 3

The theorem remains valid also if the lines AD, BE and CF are all parallel (in which case it's customary to say that the point K lies at infinity). This case is even simpler than the one just proven. Another exceptional case is when one (or two) of the points D, E, or F is (are) at infinity which means that one of the Cevians is parallel to the side it's supposed to cross. This case too must be treated separately.

Remark 4

An additional proof - a derivation from the 4 Travelers Problem - has been devised by Stuart Anderson.

Corollary 1 (center)

Medians in a triangle intersect at a single point.

Proof

Medians connect vertices with the midpoints of the opposite sides. Therefore, AF/FB = BD/DC = CE/EA = 1. Each of the ratios is 1 and so is their product.

Corollary 2 (incenter)

In a triangle, angle bisectors intersect at a single point.

Proof

For angle bisectors we know that AF/FB = AC/BC, BD/DC = AB/AC, CE/EA = BC/AB. Multiplying the three yields (1).

Corollary 3 (orthocenter)

In a triangle, altitudes intersect at a single point.

Proof

Indeed, right-angled triangles ACD and BCE are similar. Therefore CE/DC = BE/AD. In an analogous manner, AF/EA = CF/BE and BD/FB = AD/CF. Now

 
AF/FB · BD/DC · CE/EA= CE/DC · AF/EA · BD/FB
 = BE/AD · CF/BE · AD/CF
 = 1.

Remark

It's interesting to compare the direct proofs of the Corollaries with the ones we used for each case separately. Are the latter any easier?

Corollary 4 (Gergonne point)

Let D, E, F be the points where the inscribed circle touches the sides of the triangle ABC. Then the lines AD, BE and CF intersect at one point. (This is known as the Gergonne point, named after Joseph Diaz Gergonne (1771-1859). The ususal notation for the point is Ge.)

Proof

Sides of the triangle being tangent to the inscribed circle, AF = EA, FB = BD, DC = CE so that (1) indeed holds.

(An interactive illustration offers a convincing demonstration of the existence of Gergonne point and of an analogous property of excircles. The proof is virtually the same as in the case of the incircle. Curiously, the concurrency is observed also when one of the vertices of the base triangle is moved to infinity.)

Corollary 5 (Lemoine point)

Symmedians ASa, BSb, CSc intersect at a point (known as the Lemoine point.)

Proof

We'll make use of two ways to compute the area of a triangle. Namely, 2·S = a·b·sin(C) and 2·S = c·hc (and similarly for the other two vertices.) Thus we have

  Area(ΔBASa)/Area(ΔAMaC) = BSa/CMa = AB·ASa/AMa·AC
Area(ΔASaC)/Area(ΔAMaB) = CSa/BMa = AC·ASa/AMa·AB

Divide the first of these by the second:

  BSa/CMa · BMa/CSa = AB2/AC2

Or, since BMa = CMa,

  BSa/CSa = AB2/AC2

Similar identities hold for the other two vertices. All that remains is to multiply the three. (The symmedians have many interesting properties.)

Remark

Corollary 5 actually showed more than it set out to. The result is in fact more general. Let APa, BPb, and CPc be three concurrent Cevians. Reflect the line of APa in the bisector of angle A, and denote the resulting segment as AQa. Construct similarly BQb and CQc as reflections of the other two Cevians. Then the three lines AQa, BQb, and CQc are concurrent.

The lines APa and AQa are isogonal (or isogonal conjugates of each other.) The same is true of the other two pairs. For this reason the two points of concurrency, that of Cevians APa, BPb, and CPc and that of Cevians AQa, BQb, and CQc, are also said to be isogonal conjugates of each other.

Corollary 6

For three concurrent Cevians AD, BE, and CF, if the points D, E, and F are reflected in the midpoints of the corresponding sides, the resulting three lines form another triplet of concurrent Cevians. In other words, isotomic conjugates of concurrent Cevians are also concurrent.

Proof

Indeed, that the given lines are concurrent is reflected by the fact (1) that the product of the three ratios is 1. Now, note that reflection in the midpoint of a side inverts the corresponding ratio. Obviously, the product of the three inverted ratios is still 1.

Corollary 7 (Nagel point)

Let Xa be the point of tangency of side BC and the excircle with center Ia. Similarly define points Xb and Xc on sides AC and AB. Then three lines AXa, BXb and CXc are concurrent.

Proof

Point Xa has a remarkable property of being midway from the vertex A. More accurately, AB + BXa = AC + CXa. Let p be the semiperimeter of ΔABC. Then BXa = p - AB = p - c and CXa = p - AC = p - b. Therefore, BXa/CXa = (p - c)/(p - b). Write the corresponding ratios for side AB and AC and multiply all three equalities to prove the Corollary.

Corollary 8 (R. S. Hu)

Given three nonintersecting mutually external circles, connect the intersections of internal common tangents of each pair of circles with the center of the other circle. Then the resulting three line segments are concurrent.

 

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Circles B and C are homothetic in D - the point of intersection of their common internal tangents. Which means that BD/DC = rB/rC. Similarly, we have CE/EA = rC/rA and AF/FB = rA/rB.

(See R. B. Nelsen, Proofs Without Words II, MAA, 2000)

Remark

Ceva's theorem is implied by the theorem of Menelaus to which in fact it is equivalent. It also admits a very nice visual proof.

 

This applet requires Sun's Java VM 2 which your browser may perceive as a popup. Which it is not. If you want to see the applet work, visit Sun's website at http://www.java.com/en/download/index.jsp, download and install Java VM and enjoy the applet.


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Barycenter

The point where three medians of a triangle meet is called the barycenter - the center of gravity - of the triangle. There is a way to justify this designation. Place equal masses w at the vertices of the triangle. Then the midpoint D of BC will be the center of gravity of BC in the sense I plan to discuss at a later time. Intuitively, if we place the sum of two masses in their center of gravity then the moment (the mass times the distance) of such a material point relative to any other point will equal the sum of moments of the two original points.

Generally speaking, the center of gravity of two points L with mass wL and M with mass wM is point N with mass wL + wM that satisfies the rule of moments: LN·wL = NM·wM and carries the total mass of the two points. We shall adopt the notation

  N = Z(L, wL; M, wM)

for the center of gravity (the barycenter) of two material points L and M with masses wL and wM, respectively.

Returning to our case, the center of gravity K of the two points A and D satisfies AK·w = KD·2w or AK = 2KD. It's a well-known feature of the point where medians meet. The medians are divided in the ratio 1:2 at the point of their intersection. It's interesting to ask a general question: What if the masses we placed at the vertices A, B, C were not equal? The barycenter of the triangle still would of course exist. Assuming that the barycenter's location is independent of the way it's computed we would actually get a different proof of the Ceva Theorem. We shall have to demonstrate that for every D, C, E in the Ceva Theorem, it's possible to find masses wA, wB and wC such that the points D, E, and F will serve centers of gravity of the two vertices they lie between.

Actually this is easily done. Let wA> 0 be arbitrary. Find wB from wAAF = wBFB: wB = wAAF/FB. Next find wC from wBBD = wCDC: wC = wBBD/DC = wA·AF·BD/FB/DC. Now check that also wAEA = wCCE. Indeed,

  wCCE = wACE·AF·BD/FB/DC = wAEA

by (1).

Now, let K be an arbitrary point inside ΔABC. Through K draw three lines, AD, BE, and CF. Ceva's theorem guarantees condition (1). From the foregoing discussion, there exist three masses wA, wB, and wC such that, if placed at the corresponding vertices of ΔABC, their center of gravity (barycenter) will coincide with the point K.

Barycenter and Barycentric Coordinates

  1. 3D Quadrilateral - a Coffin Problem
  2. Barycentric Coordinates
  3. Barycentric Coordinates: a Tool
  4. Barycentric Coordinates and Geometric Probability
  5. Ceva's Theorem
  6. Determinants, Area, and Barycentric Coordinates
  7. Maxwell Theorem via the Center of Gravity
  8. Medians in a Quadrilateral
  9. Three glasses puzzle
  10. Van Obel Theorem and Barycentric Coordinates

Copyright © 1996-2008 Alexander Bogomolny

29706919Page copy protected against web site content infringement by Copyscape


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