from to about the -axis.
A bullet is formed by revolving the area bounded by the the curveIt is then shot straight into a very thick wall (i.e. it does not pierce through the other side at all) making a closed cylindrical hole until it stops moving. Then the bullet is carefully extracted without affecting the hole at all, leaving an empty hole with a pointy end where the bullet once was.
The length of the entire hole is . If the volume of the hole can be expressed as where is a constant, find the value of .
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The radius of the base of the bullet is ln ( e ) = 1 and its length is e − 1 . So since the length of the entire hole is e + 1 , the volume of the hole is the volume of the bullet plus the volume of a cylinder of length 2 and radius 1 .
The volume of the cylindrical part of the hole is then 2 π , and the volume of the bullet is
∫ 1 e π ( ln ( x ) ) 2 d x .
We can solve this integral using the parts method. Let u = ( ln ( x ) ) 2 and d v = d x . Then d u = 2 x ln ( x ) d x and v = x , and the integral then becomes, (ignoring the bounds for the moment),
π x ( ln ( x ) ) 2 − 2 π ∫ ln ( x ) d x = π x ( ln ( x ) ) 2 − 2 π ( x ln ( x ) − x ) =
π x ( ( ln ( x ) ) 2 − 2 ln ( x ) + 2 ) ,
where another application of the parts method was used to determine ∫ ln ( x ) d x . Evaluating this from x = 1 to x = e gives us a volume of
π e ∗ ( 1 − 2 + 2 ) − π ∗ ( 0 − 0 + 2 ) = π ( e − 2 ) .
Adding to this the volume of the cylindrical part of the hole gives us a total volume of e π , implying that the constant i = 1 .