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∫ csc x d x = ln ( csc x − cot x ) + C = ln ( t a n 2 x ) + C mayalso be applied for fast relief.
Anyway, I applied Wolfram Alpha.
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Thanks. You can use software to solve your problems, but please don't present it as a solution. I use Wolfram Alpha to check solutions.
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I shall try to write as a reply instead of another solution.
Nice job! You and I always seem to differ in our approaches but the outcome is always the same!
sin ( 2 x ) can be represented as 1 + tan 2 x 2 tan x .
= 2 1 ∫ 6 π 3 π tan x 1 + tan 2 x d x = 2 1 ∫ 6 π 3 π tan x sec 2 x d x Let u = tan x ; d u = sec 2 x d x = 2 1 ∫ x = 6 π x = 3 π u d u = 2 1 [ ln u ] x = 6 π x = 3 π = 2 1 [ ln tan x ] x = 6 π x = 3 π = 2 1 ln 3 = ln 3
∫ 6 π 3 π sin 2 x 1 d x = ∫ 6 π 3 π 2 sin x cos x sin 2 x + cos 2 x d x = − 2 1 ∫ 6 π 3 π − 2 sin x ( 2 cos x ) − 1 + 2 1 ∫ 6 π 3 π 2 cos x ( 2 sin x ) − 1 = { 3 π 6 π ( − 2 1 ln ∣ 2 cos x ∣ + 2 1 ln 2 sin x ) = ln 3
Clearly it is (sec(x))^2/tanx where substution tanx=t helps
Well, my solution includes tan x sec 2 x but it wasn't "clear" to me until I fiddled around with some trig ID's. But yes, from this trig substitution I was able to get the integral ∫ t d t , t = tan x and d t = sec 2 x d x
For the mean value theorem, the solution is >0.52 and <0.609. Only the correct answer is in that range
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∫ 6 π 3 π sin ( 2 x ) d x = ∫ 6 π 3 π 2 sin x cos x d x Let y = sin x ⇒ d y = cos x d x = ∫ 2 1 2 3 2 sin x cos 2 x d y = ∫ 2 1 2 3 2 y ( 1 − y 2 ) d y = 4 1 ∫ 2 1 2 3 ( 1 − y 1 + y 2 − 1 + y 1 ) d y = 4 1 [ − ln ( 1 − y ) + 2 ln y − ln ( 1 + y ) ] 2 1 2 3 = 4 1 [ ln ( 1 − y 2 y 2 ) ] 2 1 2 3 = 4 1 [ ln ( 1 − 4 3 4 3 ) − ln ( 1 − 4 1 4 1 ) ] = 4 1 [ ln 3 − ln ( 3 1 ) ] = 4 ln 9 = ln 3