The graph of (as shown above) looks innocent enough to noticeably oscillate as increases. However, as approaches , the oscillations grow rapidly, making vary greatly from around this region, even at very infinitesimal values of .
That said, will cross the -axis for an infinite number of times from to , creating several regions of the first quadrant enclosed by the curve and the -axis.
If the sum of these regions is , then determine .
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We are tasked to find the area under the curve of f ( x ) between 0 and 1 provided that f ( x ) is above the x - axis.
We first find the antiderivative of f ( x ) = sin ( ln x ) .
Let I = ∫ sin ( ln x ) d x
By integration by parts, using u = sin ( ln x ) , and d v = d x , we get
I = x sin ( ln x ) − ∫ x x cos ( ln x ) d x
I = x sin ( ln x ) − ∫ cos ( ln x ) d x
Then again, we use the substitutions u = cos ( ln x ) and d v = d x to get
I = x sin ( ln x ) − [ x cos ( ln x ) + ∫ sin ( ln x ) d x ]
I = x sin ( ln x ) − x cos ( ln x ) − I
2 I = x sin ( ln x ) − x cos ( ln x )
I = 2 x [ sin ( ln x ) − cos ( ln x ) ] + C
Now, we check the behavior of the function. Note that f ( x ) = 0 when x = e π n for all integers. Additionally, note that 1 = e 0 . This implies that we are dealing with zeroes of f ( x ) of the form e π k where k ∈ Z , k ≤ 0 .
Since we can't find first zero of f ( x ) around the origin, we inspect its behavior around x = 1 and proceed to the left.
Notice that ∫ e − π 0 f ( x ) d x = − 2 1 ( 1 + e π ) e − π . Since we dealt with two adjacent zeroes, seeing this area as negative implies that this part of the graph occurs below the x - axis, and will not be considered.
By a similar manner, we can get the few succeeding zeroes, and get a pattern
∫ e − 2 π e − π f ( x ) d x = 2 1 ( 1 + e π ) e − 2 π
∫ e − 3 π e − 2 π f ( x ) d x = − 2 1 ( 1 + e π ) e − 3 π
∫ e − 4 π e − 3 π f ( x ) d x = 2 1 ( 1 + e π ) e − 4 π
In fact, we can see that the area alternates every time the graph crosses the x -axis. This will give us the sum for the areas above the x -axis under the curve.
A = 2 1 ( 1 + e π ) ( e − 2 π + e − 4 π + e − 6 π + . . . )
A = 2 1 ⋅ 1 − e − 2 π ( 1 + e π ) ( e − 2 π )
A = 2 1 ⋅ 1 − e − 2 π ( 1 + e π ) ( e − 2 π ) ⋅ e 2 π e 2 π
A = 2 1 ⋅ e 2 π − 1 1 + e π
A = 2 1 ⋅ ( e π + 1 ) ( e − π − 1 ) 1 + e π
A = 2 1 ⋅ e π − 1 1
A ≈ 0 . 0 2 2 5 8 2 8 5
so ⌊ 1 0 5 A ⌋ = 2 2 5 8 .