Disk method it is, since both given options integrate with respect to <em>y</em>.
First find where the boundaries of the region intersect.
• <em>y</em> = <em>x</em> ³ and <em>y</em> = 1 intersect at (1, 1)
• <em>y</em> = <em>x</em> ³ and <em>x</em> = 3 intersect at (3, 27)
• <em>y</em> = 1 and <em>x</em> = 3 intersect at (1, 3)
So the bounded region is the set of points
{ (<em>x</em>, <em>y</em>) | 1 ≤ <em>x</em> ≤ 3 and 1 ≤ <em>y</em> ≤ <em>x</em> ³ }
But since we're integrating with respect to <em>y</em>, rewrite this set so that <em>y</em> has constant limits:
{ (<em>x</em>, <em>y</em>) | ∛<em>y</em> ≤ <em>x</em> ≤ 3 and 1 ≤ <em>y</em> ≤ 27 }
Pick some point <em>y</em> in the interval [1, 27] and construct a disk centered at the given axis of revolution (<em>x</em> = 3). Such a disk will have radius 3 - ∛<em>y </em>because <em>x</em> = ∛<em>y</em> is the horizontal distance from the <em>y</em>-axis to the curve <em>y</em> = <em>x</em> ³ and <em>x</em> = 3 is itself 3 units away from the <em>y</em>-axis. Its height will be some small change in <em>y</em>, call it ∆<em>y</em>. Then the volume of this disk is
<em>π</em> (3 - ∛<em>y</em> )² ∆<em>y</em>
Now do the same thing for every <em>y</em> in [1, 27] - infinitely many of them! - and make ∆<em>y</em> very small, such that ∆<em>y</em> → d<em>y</em>. The volume of the solid is the sum total of the volumes of these infinitely many disks, given by the integral
and so the answer is A (assuming the limits of integration are listed from upper to lower).