Let
△
A
B
C
be a triangle with
B
C
=
5
,
C
A
=
6
,
A
B
=
7
.
Let
D
,
E
be the midpoints of
A
B
,
A
C
respectively. The circumcircles of
△
B
C
D
and
△
A
D
E
meet for a second time at
X
(
X
=
A
). Given that
A
X
2
=
b
a
for some coprime positive integers
a
,
b
,
find the last three digits of
a
+
b
.
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Yes u are right
Very nice solution. I'm adding one in Cartesian coordinates. Embed △ A B C into the first quadrant of a Cartesian coordinate system with origin in B and the directed line B C as x -axis. Apply cosine rule to triangle △ A B C to get 2 5 + 4 9 − 2 ⋅ 5 ⋅ 7 ⋅ cos ∠ A B C = 3 6 , hence cos ∠ A B C = 3 5 1 9 and consequently sin 2 ∠ A B C = 1 − 3 5 2 1 9 2 = 1 2 2 5 8 6 4 . Use Apollonius' theorem to the median C D , obtaining C D 2 = 4 2 ⋅ 5 2 + 2 ⋅ 6 2 − 7 2 = 4 7 3 If R is the circumradius of △ B C D , by sine rule we have 4 R 2 = sin 2 ∠ A B C C D 2 \hbox , w h e n c e R 2 = 1 3 8 2 4 1 2 5 1 9 5 Call F the circumcenter of △ B C D and J its x -projection. Then F J 2 = R 2 − 4 2 5 = 1 3 8 2 4 3 0 2 5 , hence the coordinates of F are ( 5 / 2 , 5 5 6 / 2 8 8 ) . Call I the x -projection of A , to get ∣ B I ∣ = ∣ A B ∣ cos ∠ A B C = 7 ⋅ 3 5 1 9 = 5 1 9 . Now if L is the x -projection of E , then ∣ B L ∣ = 2 1 ⋅ ( 5 + 2 1 9 ) = 5 2 2 . Now, if G is the circumcenter of △ A D E and N its x -projection, abscissa of G is given by ∣ B N ∣ = 2 ∣ B K ∣ + ∣ B L ∣ = 2 0 1 9 + 4 4 = 2 0 6 3 , where K is the x -projection of D . Let's call now r the circumradius of △ A D E . We get 4 r 2 = sin 2 ∠ A D E 3 2 = sin 2 ∠ A B C 3 2 \hbox , h e n c e r 2 = 3 8 4 1 2 2 5 If O is the mid-point of D E , we get G O 2 = r 2 − 4 D E 2 = 3 8 4 1 2 2 5 − 1 6 2 5 = 3 8 4 6 2 5 , hence ∣ G O ∣ = 4 8 2 5 6 . Moreover, we have D K 2 = ( 2 7 ) 2 sin 2 ∠ A B C = 2 5 2 1 6 , hence D K = 5 6 6 . The coordinates of point G are given by G : ( 2 0 6 3 , 5 6 6 + 4 8 2 5 6 ) = ( 2 0 6 3 , 2 4 0 4 1 3 6 ) . The system of equations of the two circumcircles is ⎩ ⎪ ⎨ ⎪ ⎧ ( x − 2 5 ) 2 + ( y − 2 8 8 5 5 6 ) 2 = 1 3 8 2 4 8 9 4 2 5 ( x − 2 0 6 3 ) 2 + ( y − 2 4 0 4 1 3 6 ) 2 = 3 8 4 1 2 2 5 The solution different from D is the point X : ( 4 0 8 1 1 5 9 0 5 , 4 0 8 1 4 0 2 0 6 ) and its squared distance to A is given by d 2 = ( 4 0 8 1 1 5 9 0 5 − 5 1 9 ) 2 + ( 4 0 8 1 4 3 2 0 6 − 5 1 2 6 ) 2 = = 5 8 3 6 3 0 0 = b a . Now the last three digits of a + b = 6 8 8 3 are 8 8 3 .
I hope. This answer is wrong. Make second approach triangle BEC similar to triangle ADX so AX.AX=931/100 so answer will be 031
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I find no particular reason why △ B E C should be similar to △ A D X . They have only one common angle ( ∠ A C D = ∠ A E D = ∠ E C B ). The following image disproves your claim.
Image link: http://s23.postimg.org/4axu1538b/Untitled.png
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OK, this is a horrible problem with a very inelegant solution. Apologies. The original problem asked to show that the second intersection point of the circumcircles of △ B C D , △ A D E and △ B C E , △ A D E are equidistant from A (which should be obvious from the following solution). The reader might refer to this helpful article on barycentric coordinates.
Set the normalized barycentric coordinates A = ( 1 , 0 , 0 ) , B = ( 0 , 1 , 0 ) , C = ( 0 , 0 , 1 ) . Then, the coordinates of D , E are ( 2 1 , 2 1 , 0 ) and ( 2 1 , 0 , 2 1 ) respectively.
Suppose the equation of circle ( A D E ) is a 2 y z + b 2 z x + c 2 x y = u x + v y + w z (normalized coordinates). Plugging the coordinates of A , we see that u = 0 . Plugging the coordinates of D , we see that 4 c 2 = 2 u + v ⟹ v = 2 c 2 . Similarly, plugging the coordinates of E shows that w = 2 b 2 . To sum it up, the equation of the circumcircle of △ A D E is a 2 y z + b 2 z x + c 2 x y = 2 c 2 y + b 2 z .
Let the equation of ( B C D ) be a 2 y z + b 2 z x + c 2 x y = p x + q y + r z . Plugging the coordinates for B and C show that q = r = 0 . Plugging the coordinates of D , we see that 4 c 2 = 2 p ⟹ p = 2 c 2 . To sum it up, the equation of the circumcircle of △ B C D is a 2 y z + b 2 z x + c 2 x y = 2 c 2 x .
Let ( x , y , z ) be the point of intersection of ( A D E ) and ( B C D ) apart from D (where x + y + z = 1 ).
The displacement vector A X is ( x − 1 , y , z ) , so ∣ A X ∣ 2 = − a 2 y z − b 2 z ( x − 1 ) − c 2 ( x − 1 ) y = − ( a 2 y z + b 2 z x + c 2 x y ) + ( b 2 z + c 2 y ) = − 2 c 2 y + b 2 z + b 2 z + c 2 y = 2 b 2 z + c 2 y = a 2 y z + b 2 z x + c 2 x y = 2 c 2 x .
Now, we know that x , y , z simultaneously satisfy the equations a 2 y z + b 2 z x + c 2 x y a 2 y z + b 2 z x + c 2 x y x + y + z = 2 c 2 x = 2 c 2 y + b 2 z = 1 . Equating a 2 y z + b 2 z x + c 2 x y from the first two equations and plugging z = 1 − x − y , we obtain c 2 x = c 2 y + b 2 ( 1 − x − y ) ⟹ y = c 2 − b 2 ( b 2 + c 2 ) x − b 2 .
This implies z = 1 − c 2 − b 2 ( b 2 + c 2 ) x − b 2 − x = b 2 − c 2 c 2 ( 2 x − 1 ) .
Plugging this in the second equation, we obtain 2 a 2 c 2 − b 2 ( b 2 + c 2 ) x − b 2 b 2 − c 2 c 2 ( 2 x − 1 ) + 2 b 2 c 2 − b 2 ( b 2 + c 2 ) x − b 2 x + 2 c 2 c 2 − b 2 ( b 2 + c 2 ) x − c 2 x = 0 .
We interpret this as a quadratic in x . We know that x = 2 1 is one solution (since D = ( 2 1 , 2 1 , 0 ) is a point of intersction of the circles in question). To find the other solution, it suffices to find the ratio of the constant term and coefficient of x 2 . Collecting terms, we find out that this ratio is [ x 2 ] [ x 0 ] = 2 a 2 ( b 2 + c 2 ) − ( b 2 − c 2 ) 2 a 2 b 2 . Hence, the other solution for x is 2 a 2 ( b 2 + c 2 ) − ( b 2 − c 2 ) 2 2 a 2 b 2 . Now, ∣ A X ∣ 2 = 2 c 2 x = 2 a 2 ( b 2 + c 2 ) − ( b 2 − c 2 ) 2 a 2 b 2 c 2 .
Plugging the values shows us that the last three digits of a + b are 8 8 3 .
Note that the expression of A X 2 is symmetric in b , c , which solves the original problem.