Simply solve the limit of this integral for the case when the the constant of integration is equal to zero.
x → 0 lim ∫ ( 2 x sin ( x 1 ) − cos ( x 1 ) ) d x
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x → 0 lim [ ∫ 2 x sin ( x 1 ) − cos ( x 1 ) d x ]
x → 0 lim [ ∫ 2 x sin ( x 1 ) d x − ∫ cos ( x 1 ) d x ]
∫ f ( x ) g ′ ( x ) d x = f ( x ) g ( x ) − ∫ f ′ ( x ) g ( x ) d x
f ( x ) = sin ( x 1 ) and g ′ ( x ) = 2 x
then f ′ ( x ) = − x 2 cos ( x 1 ) and g ( x ) = x 2
∫ 2 x sin ( x 1 ) d x = x 2 sin ( x 1 ) + C − ∫ − x 2 cos ( x 1 ) x 2 d x
= x 2 sin ( x 1 ) + C + ∫ cos ( x 1 ) d x
implement this expression into the integral and simplify
= x → 0 lim [ x 2 sin ( x 1 ) + C + ∫ cos ( x 1 ) d x − ∫ cos ( x 1 ) d x ]
= x → 0 lim [ x 2 sin ( x 1 ) ] + C
the range of values for the sin ( x 1 ) function exists in the interval [-1,1]
− 1 ≤ sin ( x 1 ) ≤ 1
multiply the inequality by x 2 . All of the values that come from x 2 will be greater than or equal to zero, so it is unnecessary to flip any inequality signs.
− x 2 ≤ x 2 sin ( x 1 ) ≤ x 2 Next,
x → 0 lim − x 2 ≤ x → 0 lim x 2 sin ( x 1 ) ≤ x → 0 lim x 2
0 ≤ x → 0 lim x 2 sin ( x 1 ) ≤ 0
therefore, by use of the squeeze theorem, it can be said that the limit of x 2 sin ( x 1 ) = 0
As such, it seems safe to assume that the limit of this integral is equal to zero, or,
x → 0 lim [ ∫ 2 x sin ( x 1 ) − cos ( x 1 ) d x ] = 0
The L a T e x in front is not needed. Instead of $ ... $ replace them with \ ( ... \ ) (no space between the backslash \ and brackets ().
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Similar solution as @John Rozmarynowycz 's
I = ∫ ( 2 x sin x 1 − cos x 1 ) d x = ∫ 2 x sin x 1 d x − ∫ cos x 1 d x = x 2 sin x 1 + C − ∫ x 2 ( − x 2 1 cos x 1 ) d x − ∫ cos x 1 d x = x 2 sin x 1 + C + ∫ cos x 1 d x − ∫ cos x 1 d x = x 2 sin x 1 + C By integration by parts where C is the constant of integration
Therefore,
x → 0 lim I ∣ ∣ ∣ ∣ C = 0 = x → 0 lim x 2 sin x 1 = 0 Note that x → 0 lim sin x 1 ∈ [ − 1 , 1 ] is bounded.