As shown in the diagram, rectangle A B C D has side lengths A B = sin θ and A D = 1 . Point E inside rectangle A B C D is such that A E = A B and ∠ E A B = θ .
If S ( θ ) is area of quadrilateral A B C E , find θ → 0 + lim θ 3 S ( θ ) .
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Note that S ( θ ) = [ A B C E ] = [ A B C D ] − [ A E C D ] . To find [ A E C D ] , draw E F ∣ ∣ A D . Then:
S ( θ ) = [ A B C D ] − [ A E C D ] = [ A B C D ] − [ A E F D ] − [ C E F ] = A D × A B − 2 ( A D + E F ) × D F − 2 C F × E F = A D × A B − 2 A D × D F − 2 C D × E F = sin θ − 2 sin θ cos θ − 2 sin θ ( 1 − sin 2 θ ) = 2 sin θ ( 1 − cos θ + sin 2 θ ) = 4 2 sin θ − sin 2 θ + 2 sin 3 θ
Therefore,
θ → 0 + lim θ 3 S ( θ ) = θ → 0 + lim 4 θ 3 2 sin θ − sin 2 θ + θ → 0 + lim 2 1 ( θ sin θ ) 3 = θ → 0 + lim 1 2 θ 2 2 cos θ − 2 cos 2 θ + 2 1 ⋅ 1 3 = θ → 0 + lim 2 4 θ − 2 sin θ + 4 sin 2 θ + 2 1 = θ → 0 + lim 2 4 − 2 cos θ + 8 cos 2 θ + 2 1 = 2 4 6 + 2 1 = 4 3 A 0/0 case, L’H o ˆ pital’s rule applies. After differentiation, again 0/0 Again a 0/0 case Differentiate up and down w.r.t. θ
I calculated the limit more or less the same way(I applied L'Hospital's thrice), but I found the area differently: I let F be the foot of the altitude from E and split it into the area of two triangles( △ A B E and △ B E C ), which can be computed using trigonometry on △ A E F and 2 1 ⋅ b ⋅ h .
Draw a line segment from E till it intersects AB at F, which is perpendicular to AB. Draw a line segment from E till it intersects BC at G, which is perpendicular to BC. Then, the shaded area is the following:
S = A r e a ( △ A E F ) + A r e a ( △ E G C ) + A r e a ( E F B G )
E F B G is a rectangle. Let sin θ = r . Then the expression comes out to be:
S = 2 r 2 sin θ cos θ + 2 1 ( r − r cos θ ) ( 1 − r sin θ ) + ( r sin θ ) ( ( r − r cos θ )
This expression can be simplified to obtain the following:
S = 2 sin 3 θ cos θ + sin θ ( 1 − cos θ ) ( 1 − sin 2 θ ) + 2 sin 2 θ ( 1 − cos θ )
S = 2 sin 3 θ cos θ + sin θ ( 1 − cos θ ) cos 2 θ + 2 sin 2 θ ( 1 − cos θ )
Therefore:
θ → 0 + lim θ 3 S = θ → 0 + lim 2 θ 3 sin 3 θ cos θ + sin θ ( 1 − cos θ ) cos 2 θ + 2 sin 2 θ ( 1 − cos θ )
θ → 0 + lim θ 3 S = ( θ → 0 + lim 2 θ 3 sin 3 θ cos θ ) + ( θ → 0 + lim 2 θ 3 sin θ ( 1 − cos θ ) cos 2 θ ) + ( θ → 0 + lim 2 θ 3 2 sin 2 θ ( 1 − cos θ ) )
θ → 0 + lim θ 3 S = 2 1 + 4 1 + 0
θ → 0 + lim θ 3 S = 4 3
Each limit can be solved in more than one way. I have left out these evaluations.
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Set up coordinates with A at the origin and B on the x − axis. Then the coordinates of the points are A ( 0 , 0 ) , B ( sin θ , 0 ) , C ( sin θ , 1 ) , D ( 0 , 1 ) and E ( cos θ ⋅ sin θ , sin 2 θ ) .
The area of A B C E is the sum of the areas of A B E and B C E ; that is S ( θ ) = 2 1 sin 3 θ + 2 1 ( sin θ − cos θ ⋅ sin θ )
Using the small angle approximations sin θ ≈ θ and cos θ ≈ 1 − 2 1 θ 2 , this becomes S ( θ ) ≈ 2 1 θ 3 + 2 1 ( θ − θ + 2 1 θ 3 ) = 4 3 θ 3
Hence the required limit is 4 3 .