In △ A B C , A B = A C . Now a point D lies on A C so that A B = B D and a point E satisfies A D = B E as well as A C = C E . Interestingly, points B , E and D are collinear. If ∠ A B C = q p π radians where p and q are coprime positive integers, p + q = ?
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For simplicity, take A B = 1 . Also, let ∠ D C E = θ . Since B D = A B = A C and A D = B E , E D = B D − B E = A C − A D = C D , meaning that △ C D E is isosceles. Then, ∠ D E C = θ as well, and by the External Angle Theorem, ∠ B D A = 2 θ .
We use the fact that A D + D C = A C = 1 and write A D and D C in terms of θ to obtain an equation in θ .
Because △ B A D is isosceles, the perpendicular from B bisects A D , so A D = 2 B D cos 2 θ = 2 cos 2 θ . Likewise, since △ D C E is isosceles, the perpendicular from D bisects C E , so D C = cos θ 2 C E = 2 cos θ 1 .
Then, we have that 2 cos θ 1 + 2 cos 2 θ = 1 .
Using the identity cos 2 θ = 2 cos 2 θ − 1 , multiplying both sides by 2 cos θ , simplifying, this becomes 8 cos 3 θ − 6 cos θ + 1 = 0 .
Using the identity cos 3 θ = 4 cos 3 θ − 3 cos θ , we get 2 cos 3 θ + 1 = 0 , so θ = 9 2 π (any larger θ that satisfies the equation causes 2 θ to be greater than 9 0 ° , which doesn't work as the sum of the internal angles of △ B A D is greater than 4 θ ).
Finally, since △ A B C is isosceles with ∠ B A C = θ , ∠ A B C = 2 π − θ = 1 8 5 π , so our answer is 5 + 1 8 = 2 3 .
We have some isoscelese triangles:
Using the fact that the sum of angles in a triangle add up to π, we can easily find that
Scale the diagram such that A B = 1 . The cosine rule c 2 = a 2 + b 2 − 2 a b cos φ can be applied to △ A B D , so that, setting x = A D , x 2 = 2 − 2 cos ( 4 β − π ) = 2 + 2 cos 4 β Via the identity cos 2 t = 2 cos 2 t − 1 setting t = 2 β , we get x 2 = 4 cos 2 β ⇒ x = ∣ 2 cos β ∣ , and because α , δ > 0 ⇒ 4 1 π < β < 2 1 π ⇒ cos 2 β < 0 , this means that x = − 2 cos 2 β The cosine rule can also be applied to △ C D E , so that 1 2 = ( 1 − x ) 2 ( 2 − 2 cos 2 β ) Substituting x with − 2 cos 2 β , we obtain − 8 cos 3 2 β + 6 cos 2 β + 1 = 0 Because of the identity cos 3 t = 4 cos 3 t − 3 cos t and setting t = 2 β , we can rewrite this as 1 − 2 cos ( 6 β ) = 0 which solves to β = 1 8 6 k ± 1 π ( k ∈ Z )
To satisfy both 0 < x < 1 and 0 < β < π we need 4 1 π < β < 3 1 π , so that only β = 1 8 5 π = 5 0 ° is in this range and the answer is 5 + 1 8 = 2 3 .
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Let ∠ A B C = θ . We add a point F such that A C is parallel to B F and A B = B F . Considering that A B = B D , it follows that ∠ B A D = ∠ B D A = 2 π − ∠ A B D . Moreover, A C being parallel to B F tells us that ∠ B A D + ∠ A B F = π or ∠ B A D + ∠ A B D + ∠ D B F = π . Therefore ∠ D B F = π − ∠ A B D − ∠ B A D = π − ∠ A B D − 2 π − ∠ A B D = 2 π − ∠ A B D = ∠ B A D .
As given in the question, A D = B E and we stipulate that A B = B F . Considering that ∠ B A D = ∠ F B E , we conclude that △ B A D is congruent to △ F B E employing S A S congruence. This tells us that ∠ A B D = ∠ B F E = ∠ B F C − ∠ C F E = ∠ B A D − ∠ C F E . Note that ∠ B F C = ∠ B A D being opposite angles in rhombus A B F C .
Considering also that ∠ B A D = 2 π − ∠ A B D :
∠ B A D = 2 π − ( ∠ B A D − ∠ C F E )
2 ∠ B A D = π − ( ∠ B A D − ∠ C F E )
2 ∠ B A D + ∠ B A D − ∠ C F E = π
( 2 + 1 ) ∠ B A D = π + ∠ C F E
3 ∠ B A D = π + ∠ C F E
Considering that A B = A C and hence ∠ A C B = ∠ A B C in △ A B C , ∠ B A D = ∠ B A C = π − ∠ A B C − ∠ A C B = π − 2 ∠ A B C = π − 2 θ . Then:
3 ( π − 2 θ ) = π + ∠ C F E
3 π − 6 θ = π + ∠ C F E
6 θ + ∠ C F E = 2 π
A final observation to make is this:
Combining C E = C F and C E = E F , △ C E F is equilateral with C E = C F = E F . This means ∠ C E F = ∠ E C F = ∠ C F E = 3 π . Therefore:
6 θ + 3 π = 2 π
6 θ = 3 ( 6 − 1 ) π
6 θ = 3 5 π
θ = 6 × 3 5 π
θ = 1 8 5 π
So p + q = 5 + 1 8 = 2 3
.