You just need to get the very first step
This is my original
∫ 0 π / 2 1 + sin x 1 d x
Hint: Think simple(Trigonometry you had probably learnt in 9th or 10th)
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Nice solution
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Haha... was looking over every step when the answer was still incorrect... At least I know I'm right now.
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Well, it would be easier if you replace sin x by cos (π/2-x)
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@Mayank Singh – It would have been much easier if we had multiplied numerator and denominator by (1-sinx)
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@Shivam Hinduja – How would that work? All I got was undefined things.
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@Jack Lam – Oh! Sorry I just evaluated (∞ - ∞) = 0 . But, the method would evaluate the indefinite integral.
such a long and bad method!!! uh!!
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Then maybe you can post a better one? I'm sure there are faster ways, but they're not immediately obvious to me.
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my method was similar to that of shivam hinduja!! +no offence to ur post really!!
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@A Former Brilliant Member – Would that require the use of limits or geometric analysis? Because the undefined states of the integral cannot be evaluated analytically...
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@Jack Lam – u simply had to change the sec-tan form to 1/(sec+tan) from then u would evaluate it
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@A Former Brilliant Member – Got it. Edited my solution to incorporate it as the third method.
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Solution 1: Make the substitution sin x = 1 + t 2 2 t where t = tan 2 x
Change the integration borders by substituting the values of x into t, which gives tan 0 = 0 and tan 4 π = 1
Take the derivative of t with respect to x, giving d x d t = 2 1 sec 2 2 x
Replacing with the identity sec 2 θ = 1 + tan 2 θ we get d x d t = 2 1 + t 2
Rearranging for dx, we get d x = 1 + t 2 2 d t
Returning back to the given integral, and substituting sinx, dx and the integration borders, we have ∫ 0 1 1 + 1 + t 2 2 t 1 1 + t 2 2 d t
Simplifying, we get ∫ 0 1 1 + t 2 + 2 t 2 d t
Note that the denominator is a perfect square. Using negative indices, we get ∫ 0 1 2 ( 1 + t ) − 2 d t
This can now be evaluated easily using the power rule, since the term being indexed is linear.
This yields − 2 ( 1 + t ) − 1 ∣ 0 1
Converting back into a fraction and applying the borders, we get 1 + 1 − 2 − 1 + 0 − 2
Which simplifies to 1
Solution 2: Make the substitution 1 + sin θ = 2 sin 2 4 2 θ + π
Let u = 4 2 x + π , d u = 2 d x
Using the identity sin θ 1 = csc θ and all the substitutions above, the integral is now transformed into ∫ 0 2 π csc 2 u d u
The integral of csc 2 u d u is − cot u
The integral is now − cot u ∣ 0 2 π
Substituting u back for x and evaluating the borders, we have − cot 4 π + π + cot 4 π
Which evaluates to 1
Solution 3: Multiply the numerator and denominator by 1 − sin x
Yielding 1 − sin 2 x 1 − sin x = cos 2 x 1 − sin x = sec 2 x − tan x sec x
The integral is now ∫ 0 2 π sec 2 x − sec x tan x
Standard Integrals:
∫ sec x tan x d x = sec x
∫ sec 2 x d x = tan x
Resulting in: ( tan x − sec x ) ∣ 0 2 π
Because we cannot evaluate this directly, we must transform the expression into something that can be evaluated.
tan x − sec x = tan x + sec x tan 2 x − sec 2 x
Since 1 + tan 2 x = sec 2 x it follows that tan 2 x − sec 2 x = − 1
tan x + sec x tan 2 x − sec 2 x = tan x + sec x − 1 = cos x sin x + 1 − 1 = 1 + sin x − cos x
This form can now be evaluated. Plugging in the borders:
1 + sin x − cos x ∣ 0 2 π = 1 + 1 0 − ( 1 + 0 − 1 ) = 1