Evaluate:
∫ 6 π 3 π cot ( x ) + 1 cot ( x ) sec 2 ( x ) d x
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the boundary of the 3rd row should be tan(pi/6) to tan(pi/3), not arctan(x), nice solution tho
brilliant! is your motivation is 'to only work with tan x and sec x ' ?
I don't like cot or sec, so I rewrite everything:
cot ( x ) + 1 cot ( x ) sec 2 ( x ) = sin ( x ) cos ( x ) + 1 sin ( x ) cos ( x ) 1 = cos ( x ) + sin ( x ) cos ( x ) 1
= cos ( x ) ( cos ( x ) + sin ( x ) ) 1
To integrate, it's better to have a sum of simplier fractions:
cos ( x ) ( cos ( x ) + sin ( x ) ) 1 = cos ( x ) sin ( x ) + cos ( x ) + sin ( x ) cos ( x ) − sin ( x )
That was a good idea as we have now:
cos ( x ) sin ( x ) + cos ( x ) + sin ( x ) cos ( x ) − sin ( x ) = − cos ( x ) cos ′ ( x ) + cos ( x ) + sin ( x ) ( cos ( x ) + sin ( x ) ) ′
After integrating, we have:
− ln ( cos ( x ) ) + ln ( cos ( x ) + sin ( x ) ) = ln ( cos ( x ) cos ( x ) + sin ( x ) ) = ln ( 1 + tan ( x ) )
Which evaluates to:
ln ( 1 + 3 ) − ln ( 1 + 3 1 ) = ln ( ( 3 + 1 ) / 3 1 + 3 ) = ln ( 3 ) = 2 1 ln ( 3 ) .
I like it! Breaking things down into constituent sines and cosines makes a problem easier sometimes.
First, begin by multiplying the integrand by tan ( x ) tan ( x ) . This transforms the integrand from cot ( x ) + 1 cot ( x ) sec 2 ( x ) to 1 + tan ( x ) sec 2 ( x ) .
Now we use the appropriate substitution, u = 1 + tan ( x ) , thus transforming the integral into ∫ u d u
Integrating and back-substituting gives us ln ( 1 + tan ( x ) ) ∣ ∣ ∣ 6 π 3 π = ln ( 1 + 3 ) − ln ( 1 + 3 3 ) = 2 1 ln ( 3 )
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Let the integral be I , then:
I = ∫ 6 π 3 π cot x + 1 cot x sec 2 x d x × tan x tan x = ∫ 6 π 3 π 1 + tan x sec 2 x d x Let t = tan x ⇒ d t = sec 2 x d x = ∫ 3 1 3 1 + t 1 d t = ln ( 1 + t ) ∣ ∣ ∣ ∣ 3 1 3 = ln ( 1 + 3 1 1 + 3 ) = ln 3 = 2 1 ln 3