Find the value of:
x → 2 π − lim ( tan x ) cos x
Bonus : Prove that x → 2 π + lim f ( x ) does not exist.
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The limit is 1 from both directions.
Why is it from both directions? x → 2 π + lim ( cos x ) cos x is undefined.
tan(x)^cos(x)
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What do you mean?
You're mistaken, the left hand limit is defined, but the right hand limit is undefined.
They are both defined. You have agreed already that from below is defined.
lim x → ( 2 π ) + ( exp ( lo g ( tan cos x x ) ) )
\lim_{x\to \left(\frac{\pi }{2}\right)^+} \left(\exp \fbox{\$(\cos x) (\log (\tan x))\$}\right)
\fbox{\$\exp \left(\lim_{x\to \left(\frac{\pi }{2}\right)^+} ((\cos x) (\log (\tan x)))\right)\$}
The following step is only to set up an ∞ ∞ situation so that L'Hopital rule can be applied.
\exp \fbox{\$\frac{\lim_{x\to \left(\frac{\pi }{2}\right)^+} (\log (\tan x))}{\frac{1}{\cos x}}\$}
Added explanation: lo g ( tan ( 2 π ) ) ⇒ ∞ and cos ( 2 π ) 1 is complex infinity.
lim x → ( 2 π ) + cos x 1 ( lo g ( x tan ) ) =
lim x → ( 2 π ) + d x d ( cos x 1 ) d x d lo g ( x tan ) =
lim x → ( 2 π ) + ( cos x ) 2 sin ( x ) t a n ( x ) sec 2 =
l i m x → ( 2 π ) + ( sin x ) ( tan x ) 1
\exp \fbox{\$\frac{\lim_{x\to \left(\frac{\pi }{2}\right)^+} \left(\left(\cos ^2 x\right) \left(\sec ^2 x\right)\right)}{(\sin x) (\tan x)}\$}
\exp \fbox{\$\frac{\lim_{x\to \left(\frac{\pi }{2}\right)^+} \left(\left(\cos ^2 x\right) \left(\sec ^2 x\right)\right)}{\lim_{x\to \left(\frac{\pi }{2}\right)^+} ((\sin x) (\tan x))}\$}
\frac{\exp \fbox{\$\lim_{x\to \left(\frac{\pi }{2}\right)^+} 1\$}}{\lim_{x\to \left(\frac{\pi }{2}\right)^+} ((\sin x) (\tan x))}
lim x → ( 2 π ) + ( ( sin x ) ( tan x ) ) exp 1
\frac{\exp 1}{\fbox{\$\left(\lim_{x\to \left(\frac{\pi }{2}\right)^+} (\sin x)\right) \left(\lim_{x\to \left(\frac{\pi }{2}\right)^+} (\tan x)\right)\$}}
\frac{\exp 1}{\fbox{\$\lim_{x\to \left(\frac{\pi }{2}\right)^+} (\tan x)\$}}
e $ - \infty $ 1
1
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Your 4th step is wrong. You can't apply L'hopital rule as it is not in an indeterminate form.
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cos x 1 lo g ( tan x ) is an indefinite form. It is ∞ ∞ . To be precise, the denominator is a complex infinity whose polar form has an infinite magnitude and an unknown phase angle.
lo g ( tan ( 2 π ) ) ⇒ ∞ and cos ( 2 π ) 1 = 0 1 ⇒ complex ∞
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@A Former Brilliant Member – If we want to compute the left hand limit or the right hand limit of the function f ( x ) , then the variable x must only be a real number, so the following limit does not exist (it doesn't even become unboundedly large).
x → 2 π + lim ln ( tan x )
There is no point introducing the complex numbers into the limit.
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@Pi Han Goh – 1) There is nothing in the problem specification to eliminate complex numbers 2) The limit is the same from both directions. This is not a step discontinuity. 3) The fact that one infinity is in fact a complex infinity does not affect the final result.
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@A Former Brilliant Member – I think we have a disagreement in convention here. Whenever I see a limit that doesn't have any non-real numbers in it, then I'll only consider the real axis, which there are only two directions to approach a limit. Whereas in the complex plane, there are infinite ways to approach a limit.
Looking at this very question the author posed (with the added bonus question), I'm betting that it came from an introductory calculus text/course, where the functions encountered there are normally real-valued functions, that is, f : R → R .
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Let y = x → 2 π − lim ( tan x ) cos x . Then ln y = x → 2 π − lim cos x ⋅ ln ( tan x ) , which is in the indeterminate form of 0 × ∞ . L'Hôpital's Rule comes into play! ln y = x → 2 π − lim sec x ln ( tan x ) = x → 2 π − lim d x d sec x d x d ln ( tan x ) = x → 2 π − lim sec x tan x tan x sec 2 x = x → 2 π − lim sin 2 x cos x = 0 Our answer is y = e 0 = 1 .
For the bonus question:
Let z = x → 2 π + lim ( tan x ) cos x . Then ln z = x → 2 π + lim cos x ⋅ ln ( tan x ) , but since tan x is a negative number for 2 π < x < π , the natural logarithm of such number does not exist, so the(right hand) limit does not exist.