A region bounded by y = 2 x 2 and y = x is rotated about a line y = x . If the volume of revolution can be expressed as b a π , with a , b ∈ N and g c d ( a , b ) = 1 ,
what is a + b ?
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The parabola y = 2 x 2 is equivalent to 2 x 2 − y = 0 , an equation in standard form where A = 2 , E = − 1 , and B = C = D = 0 . If we rotate it by 4 5 ° , then:
A ′ = A cos 2 4 5 ° + B sin 4 5 ° cos 4 5 ° + C sin 2 4 5 ° = 2 2
B ′ = 2 ( C − A ) sin 4 5 ° cos 4 5 ° + B ( cos 2 4 5 ° − sin 2 4 5 ° ) = − 2
C ′ = A sin 2 4 5 ° − B sin 4 5 ° cos 4 5 ° + C cos 2 4 5 ° = 2 2
D ′ = D cos 4 5 ° + E sin 4 5 ° = − 2 2
E ′ = − D sin 4 5 ° + E cos 4 5 ° = − 2 2
for a new equation of 2 2 x 2 − 2 x y + 2 2 y 2 − 2 2 x − 2 2 y = 0 , which rearranges to y = x + 2 1 − 2 1 8 x + 1 .
The line y = x rotates to y = 0 after a 4 5 ° rotation, which intersects y = x + 2 1 − 2 1 8 x + 1 at ( 0 , 0 ) and ( 1 , 0 ) .
The volume is then V = ∫ 0 1 π ( x + 2 1 − 2 1 8 x + 1 ) 2 d x .
Substituting u = 8 x + 1 and rearranging gives V = ∫ 1 3 2 5 6 π ( u 5 − 8 u 4 + 2 2 u 3 − 2 4 u 2 + 9 u ) d u = 1 2 0 1 π .
Therefore, a = 1 , b = 1 2 0 , and a + b = 1 2 1 .
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The intersection of the two curves is at x = 2 x 2 , which is at x = 0 and x = 2 1 . Given a point ( x , 2 x 2 ) on the parabola, its perpendicular distance to the line y = x is given by
r = 2 1 ( x − 2 x 2 )
The thickness of the disc is 2 d x , hence the volume is given by
V = ∫ 0 2 1 2 π r 2 d x
Plugging the expression for r from above, we get
V = 2 ∫ 0 2 1 π 2 1 ( x − 2 x 2 ) 2 d x
Expanding, and integrating, this becomes,
V = 2 2 π ∫ 0 2 1 ( x 2 − 2 2 x 3 + 2 x 4 ) d x
V = 2 2 π ( 3 1 ( 2 1 ) 3 − 2 2 ( 1 / 2 ) + 5 2 ( 2 1 ) 5 )
V = 2 1 π ( 6 1 − 4 1 + 1 0 1 ) = 2 1 π ( 6 0 1 ) ( 1 0 − 1 5 + 6 ) = π ( 1 2 0 1 )
So that a = 1 , b = 1 2 0 , making the answer 1 + 1 2 0 = 1 2 1 .