What is the area of the region defined by the following set of inequalities?
( 1 ) ( 2 ) − 1 < x y < 1 − 1 < x 2 − y 2 < 1
If the area is A , give ⌊ 1 0 0 A ⌋ .
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I apologize, the symmetry of the region is not over the x -axis, but over the line y = x .
I think the best way to approach this is through polar coordinates.
We need to find ∠ A O B and ∠ A O C .
To find it let us find the coordinates where both the curves meet.
We have x y = 1
So y = x 1
So putting it in x 2 − y 2 = 1
we have
x 4 − x 2 − 1 = 0
So x = 2 1 + 5 = a ( s a y )
So y = 1 + 5 2 = a 1
So ∠ A O B = arctan ( a 1 )
And ∠ A O C = arctan ( a )
There are 8 total regions like A O B and 4 total regions which are like B O C
For x 2 − y 2 = 1 using polar coordinates we have
r 2 = c o s ( 2 θ ) 1
For x y = 1 using polar coordinates we have:-
r 2 = 2 cosec ( 2 θ )
Area of A O B = ∫ 0 arctan ( a 1 ) 2 c o s ( 2 θ ) 1
There are 8 such regions so total area of them is ∫ 0 arctan ( a 1 ) 4 s e c ( 2 θ ) d θ
Area of B O C = ∫ arctan ( a 1 ) arctan ( a ) cosec ( 2 θ ) d θ
There are 4 such regions so their area is given by 4 ∫ arctan ( a 1 ) arctan ( a ) cosec ( 2 θ ) d θ
Now indefinite integrals of cosec ( x ) and sec ( x ) are well known.
Using them and plugging in the limits we get the total area as
∫ 0 arctan ( a 1 ) 4 s e c ( 2 θ ) d θ + 4 ∫ arctan ( a 1 ) arctan ( a ) cosec ( 2 θ ) d θ
We get our answer as ln ( 2 1 2 3 + 5 5 5 )
(Note that I have used the formula for area in polar coordinates : Area = ∫ 2 r 2 d θ
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Define u = x y and v = x 2 − y 2 . Then, du = y dx + x dy and dv = 2 x dx − 2 y dy . Solve this system of equations for dx and dy to get dx = x 2 + y 2 y du + 2 x 2 + 2 y 2 x dv and dy = x 2 + y 2 x du − 2 x 2 + 2 y 2 y dv . Thus, dA = dx ∧ dy = ( x 2 + y 2 y du + 2 x 2 + 2 y 2 x dv ) ∧ ( x 2 + y 2 x du − 2 x 2 + 2 y 2 y dv ) = ( − 2 ( x 2 + y 2 ) 2 x 2 ) du ∧ dv + ( 2 ( x 2 + y 2 ) 2 y 2 ) dv ∧ du = ( − 2 ( x 2 + y 2 ) 2 x 2 − 2 ( x 2 + y 2 ) 2 y 2 ) du ∧ dv = ( − 2 ( x 2 + y 2 ) 1 ) du ∧ dv . Call f = − 2 ( x 2 + y 2 ) 1 , and recall that u = x y and v = x 2 − y 2 . Observe then that f 2 = 4 ( x 4 + 2 x 2 y 2 + y 4 ) 1 = 4 ( 4 u 2 + v 2 ) 1 = 1 6 u 2 + 4 v 2 1 . Thus, f = ± 1 6 u 2 + 4 v 2 1 , where each solution for f corresponds to half of the problem region, as the two are symmetric over the x -axis. So, our area is ∬ dA = ∬ dx ∧ dy = 2 ∫ − 1 1 ∫ − 1 1 1 6 u 2 + 4 v 2 1 du dv = 4 1 ∫ − 2 2 ∫ − 4 4 a 2 + b 2 1 da db = lo g ( 2 1 2 3 + 5 5 5 ) ≈ 4 . 8 1 2 ⇒ ⌊ 1 0 0 A ⌋ = 4 8 1 .