Equilateral △ABC has side length 111. There are four distinct triangles AD1E1, AD1E2, AD2E3, and AD2E4, each congruent to △ABC, with BD1=BD2=11. Find ∑k=14(CEk)2.
解析
Solution 1
Note that there are only two possible locations for points D1 and D2, as they are both 111 from point A and 11 from point B, so they are the two points where a circle centered at A with radius 111 and a circle centered at B with radius 11 intersect. Let D1 be the point on the opposite side of AB from C, and D2 the point on the same side of AB as C.
Let θ be the measure of angle BAD1 (also the measure of angle BAD2); by the Law of Cosines,
11211=1112+1112−2⋅111⋅111⋅cosθ=222(1−cosθ)
There are two equilateral triangles with AD1 as a side; let E1 be the third vertex that is farthest from C, and E2 be the third vertex that is nearest to C.
Angle E1AC=E1AD1+D1AB+BAC=60+θ+60=120+θ; by the Law of Cosines,
(E1C)2=(E1A)2+(AC)2−2(E1A)(AC)cos(120+θ)=111+111−222cos(120+θ)
Angle E2AC=θ; by the Law of Cosines,
(E2C)2=(E2A)2+(AC)2−2(E2A)(AC)cosθ=111+111−222cosθ
There are two equilateral triangles with AD2 as a side; let E3 be the third vertex that is farthest from C, and E4 be the third vertex that is nearest to C.
Angle E3AC=E3AB+BAC=(60−θ)+60=120−θ; by the Law of Cosines,
(E3C)2=(E3A)2+(AC)2−2(E3A)(AC)cos(120−θ)=111+111−222cos(120−θ)
Angle E4AC=θ; by the Law of Cosines,
(E4C)2=(E4A)2+(AC)2−2(E4A)(AC)cosθ=111+111−222cosθ
The solution is:
k=1∑4(CEk)2=(E1C)2+(E3C)2+(E2C)2+(E4C)2=222(1−cos(120+θ))+222(1−cos(120−θ))+222(1−cosθ)+222(1−cosθ)=222((1−(cos120cosθ−sin120sinθ))+(1−(cos120cosθ+sin120sinθ))+2(1−cosθ))=222(1−cos120cosθ+sin120sinθ+1−cos120cosθ−sin120sinθ+2−2cosθ)=222(1+21cosθ+1+21cosθ+2−2cosθ)=222(4−cosθ)=666+222(1−cosθ)
Substituting 11 for 222(1−cosθ) gives the solution 666+11=677.
Solution 2
This problem is pretty much destroyed by complex plane geometry, which is similar to vector geometry only with the power of easy rotation. Place the triangle in the complex plane by letting C be the origin, placing B along the x-axis, and A in the first quadrant. Let r=111. If ω denotes the primative sixth root of unity, eiπ/3, then we have C=0, B=r, and A=rω. Recall that counter-clockwise rotation in the complex plane by an angle θ is accomplished by multiplication by eiθ (and clockwise rotation is multiplication by its conjugate). So, we can find D1 and D2 by rotating B around A by angles of θ and −θ, where θ is the apex angle in the isoceles triangle with sides 111, 111, and 11. That is, let z=eiθ, and then:
D1=A+z(B−A), and D2=A+z(B−A). Now notice that B−A=A, so this simplifies further to:
D1=A+zA, and D2=A+zA.
Similarly, we can write E1, E2, E3, and E4 by rotating D1 and D2 around A by ±π/3:
Now to find some magnitudes, which is easy since we chose C as the origin:
∥E1∥2=(A+ωzA)(A+ωzA)=2∥A∥2+ωzA2+ωzA2,
∥E2∥2=(A+ωzA)(A+ωzA)=2∥A∥2+ωzA2+ωzA2,
∥E3∥2=(A+ωzA)(A+ωzA)=2∥A∥2+ωzA2+ωzA2,
∥E4∥2=(A+ωzA)(A+ωzA)=2∥A∥2+ωzA2+ωzA2.
Adding these up, the sum equals 8∥A∥2+(A2+A2)(ωz+ωz+ωz+ωz)=8∥A∥2+(A2+A2)(z+z)(ω+ω).
(Isn't that nice?) Notice that A2+A2=r2(ω2+ω2)=−r2, and ω+ω=1, so that this sum simplifies further to 888−111(z+z).
Finally, z+z=2cosθ, which is found using the law of cosines on that isoceles triangle: 11=111+111−222cosθ, so 2cosθ=211/111.
Thus, the sum equals 888−211=677.
Solution 3
This method uses complex numbers with A as the origin. Let A=0, B=111, C=111θ, where θ=eiπ/3=21+23i.
Also, let x be D1 or D2. Then
∣x∣=111,∣x−111∣=11
Therefore, 11=∣x−111∣2=∣x∣2+111−2111Re(x)=222−2111Re(x), so
2111Re(x)=211.
Since E1, E2 are one of D1θ or D1θ−1, without loss of generality, let E1=D1θ and E2=D1θ−1. Then
∣CE1∣2=∣111−D1∣2=∣111−x∣2=11∣CE2∣2=∣θ2111−D1∣2=222−2111Re(D1θ2)
One can similarly get ∣CE3∣=11 and ∣CE4∣=222−2111Re(D2θ2), so the desired sum is equal to
22+444−2111(Re(D1θ2)+Re(D1θ2))
Note that Re(D1,2θ2)=Re((Re(x)±Im(x)i)(−1/2+3/2i))=−(Re(x)/2±Im(x)3/2), so the sum of these two is just −Re(x). Therefore the desired sum is equal to
22+444+2111Re(x)=22+444+211=677.
Solution 4
This method uses the observation that every point is equidistant from A. Without loss of generality, we can assume C is on the same side of AB as D1.
We can start off by angle chasing the angles around A. We let ∠BAD1=α. Then, we note that BD1=BD2 and AD1=AB=AD2. Thus, △ABD1≅△ABD2. Thus, ∠BAD2=α also.
We can now angle chase the angles about A. Because ∠D2AE3=60, ∠D1AE3=60−2α. We can use all the congruent equilateral triangles in a similar manner obtaining:
∠D1AE3=60−2α∠E3AC=α∠CAE1=α∠D2AE2=60−2α∠E2AE4=2α
Now, AE3=AC=111 and ∠E3AC=α. Thus, △E3AC≅△BAD1. Thus, CE32=BD12=11.
Similarly, AC=AE1=111 and ∠CAE1=α. Thus, △CAE1≅△BAD1. Thus, CE12=BD12=11.
We can use △CAE2 to find CE22. Law of Cosines yields
CE22=AE22+AC2−2⋅AE2⋅AC⋅cos(∠E2AC).
Substituting the known lengths and angles gives
CE22=222−222⋅cos(120−α).
Expanding this with the Cosine Subtraction Identity we get
CE22=222−222(cos120cosα+sin120sinα).
We could attempt to calculate this but we can clear it up by simultaneously finding CE42 too. We use Law of Cosines on △CAE4 to get
CE42=AE42+AC2−2⋅AE4⋅AC⋅cos(∠E4AC).
Substituting the known lengths and angles gives
CE42=222−222⋅cos(120+α).
Expanding this with the Cosine Addition Identity we get
CE42=222−222(cos120cosα−sin120sinα).
Adding this to our equation for CE22, we get
CE22+CE42=444−222(cos120cosα−sin120sinα)−222(cos120cosα+sin120sinα).
Simplifying we get
CE22+CE42=444−444(cos120cosα)
We can find cosα by using Law of Cosines on △BAD1. This gives
11=222−222cosα.
Thus cosα=222211. Substituting it in gives
CE22+CE42=444−444(cos120⋅222211).
Thus
CE22+CE42=444+211=655.
Therefore the desired sum is equal to
11+11+655=677.
Solution 5
We create a diagram. Each of the red quadrilaterals are actually 60 degree rotations about point A. We easily get that CE1=11, and CE3=11. If we set ∠BAD2=θ, we can start angle chasing. In particular, we will like to find ∠DE4C, and ∠DE2C, since then we will be able to set up some Law Of Cosines. ∠DE4C=∠DE4A+∠AE4C=90−2θ+30+2θ=120∘ That was convenient! We can do it with the other angle as well. ∠DE2C=∠DE2A−∠CE2A=90−2θ−(30−2θ)=60∘. That means we are able to set up Law of Cosines, on triangles △DE4C and △DE2C, with some really convenient angles. Let CE2=x, and CE4=y.
333=11+x2−11x333=11+y2+11y
We subtract and get:
0=(x+y)(x−y−11)x+y obviously can't be 0, so x−y=11 We add and get:
666=22+x2+y2+11(y−x)
. y−x=−11. Thus, we can fill in and solve.
666=22+x2+y2−11655=x2+y2
Thus our answer is CE12+CE22+CE22+CE42=11+11+CE22+CE42=11+11+x2+y2=11+11+655=677.
-Alexlikemath
Solution 6
Let D2,E2,E4 be on the same side of AB as C. It is clear that CE2=CE4=11. Then, consider quadrilateral CE3BD2. Since △BD2E3 and △D2BC are congruent, D2BE3C is cyclic because ∠BE3D2≅∠BCD2. By Ptolemy's Theorem, we have CE3=11111−CD22. Similarly, CE1=11CD12−111.
Let ∠ABD2≅∠AD2B=θ. Then, cosθ=211111, so sinθ=2111433. Now, LoC on △BD2C gives CD22=11+111−211111cos(θ−60∘) and LoC on △BD1C gives CD12=11+111−211111cos(θ+60∘). By the cosine sum rule, we get \begin{align*} CE_3&=\frac{111-CD_2^2}{\sqrt{11}}\\ &=\frac{2\sqrt{11}\sqrt{111}\cos (\theta-60^\circ)-11}{\sqrt{11}}\\ &=2\sqrt{111}(\cos\theta\cos 60^\circ+\sin\theta\sin 60^\circ)-\sqrt{11}\\ &=2\sqrt{111}\left(\frac{\sqrt{11}+\sqrt{1299}}{4\sqrt{111}}\right)-\sqrt{11}\\ &=\frac{\sqrt{1299}-\sqrt{11}}{2}.\\ \end{align*} Similarly, \begin{align*} CE_1&=\frac{CD_1^2-111}{\sqrt{11}}\\ &=\frac{11-2\sqrt{11}\sqrt{111}\cos (\theta+60^\circ)}{\sqrt{11}}\\ &=\sqrt{11}-2\sqrt{111}(\cos\theta\cos 60^\circ-\sin\theta\sin 60^\circ)\\ &=\sqrt{11}-2\sqrt{111}\left(\frac{\sqrt{11}-\sqrt{1299}}{4\sqrt{111}}\right)\\ &=\frac{\sqrt{1299}+\sqrt{11}}{2}.\\ \end{align*} Therefore, our desired answer is \begin{align*} CE_1^2+CE_2^2+CE_3^2+CE_4^2&=CE_1^2+CE_3^2+11+11\\ &=2\left(\frac{\sqrt{1299}^2+\sqrt{11}^2}{2^2}\right)+22\\ &=\frac{1310}{2}+22\\ &=\boxed{677}.\\ \end{align*}
-pieMax2713
Solution 7
WLOG assume CD2>CD1,CE2>CE1,CE4>CE3.
We first know that CE1=CE3=11.
The supplementary angle of ∠E1CE2 is half the value of ∠E2AE1. Also, ∠E2AE1=∠D1AE1+∠D1AE2=120∘, so ∠E1CE2=180∘−2120∘=120∘.
We now use Law of Cosines on ΔCE1E2 and ∠E1CE2:
Let F be the midpoint of E3C. Since ΔAE3C is isosceles, AF is the altitude of E4C. Then
∠E3E4C=21∠E3AC=∠E3AFsin(∠E3E4C)=sin(∠E3AF)=111211=211111cos(∠E3E4C)=1−sin(∠E3E4C)2=2111433
Now the Law of Cosines on ΔCE3E4 and ∠E3E4C: