JEE Challenger
More from Application of Derivatives

Symmetry and Monotonicity of Inverse Tangent Function

Let the function g:(−∞,∞)→(−π2,π2)g : (-\infty, \infty) \rightarrow \left(-\frac{\pi}{2}, \frac{\pi}{2}\right) be given by g(u)=2tan⁡−1(eu)−π2g(u) = 2\tan^{-1}(e^u) - \frac{\pi}{2}. Then,

gg is

Options

A

even and is strictly increasing in (0,∞)(0, \infty)

B

odd and is strictly decreasing in (−∞,∞)(-\infty, \infty)

C

odd and is strictly increasing in (−∞,∞)(-\infty, \infty)

Correct
D

neither even nor odd, but is strictly increasing in (−∞,∞)(-\infty, \infty)

Step-by-Step Solution

To determine the properties of the function g(u)=2tan⁡−1(eu)−π2g(u) = 2\tan^{-1}(e^u) - \frac{\pi}{2}, we analyze its symmetry (parity) and monotonicity.

1. Parity of g(u)g(u):

Substitute −u-u in place of uu:
g(−u)=2tan⁡−1(e−u)−π2g(-u) = 2\tan^{-1}(e^{-u}) - \frac{\pi}{2}

Using the inverse trigonometric identity tan⁡−1(x)+tan⁡−1(1x)=π2\tan^{-1}(x) + \tan^{-1}\left(\frac{1}{x}\right) = \frac{\pi}{2} for x>0x > 0, and noting that eu>0e^u > 0 for all u∈(−∞,∞)u \in (-\infty, \infty), we have:
tan⁡−1(e−u)=tan⁡−1(1eu)=π2−tan⁡−1(eu)\tan^{-1}(e^{-u}) = \tan^{-1}\left(\frac{1}{e^u}\right) = \frac{\pi}{2} - \tan^{-1}(e^u)

Substitute this back into the expression for g(−u)g(-u):
g(−u)=2(π2−tan⁡−1(eu))−π2g(-u) = 2\left(\frac{\pi}{2} - \tan^{-1}(e^u)\right) - \frac{\pi}{2}
g(−u)=π−2tan⁡−1(eu)−π2g(-u) = \pi - 2\tan^{-1}(e^u) - \frac{\pi}{2}
g(−u)=π2−2tan⁡−1(eu)g(-u) = \frac{\pi}{2} - 2\tan^{-1}(e^u)
g(−u)=−(2tan⁡−1(eu)−π2)=−g(u)g(-u) = -\left(2\tan^{-1}(e^u) - \frac{\pi}{2}\right) = -g(u)

Since g(−u)=−g(u)g(-u) = -g(u) for all u∈(−∞,∞)u \in (-\infty, \infty), the function g(u)g(u) is an odd function.


2. Monotonicity of g(u)g(u):

Differentiate g(u)g(u) with respect to uu:
g′(u)=ddu(2tan⁡−1(eu)−π2)g'(u) = \frac{d}{du}\left(2\tan^{-1}(e^u) - \frac{\pi}{2}\right)
g′(u)=2⋅11+(eu)2⋅ddu(eu)g'(u) = 2 \cdot \frac{1}{1 + (e^u)^2} \cdot \frac{d}{du}(e^u)
g′(u)=2eu1+e2ug'(u) = \frac{2e^u}{1 + e^{2u}}

Since eu>0e^u > 0 and 1+e2u>01 + e^{2u} > 0 for all real numbers uu:
g′(u)>0∀u∈(−∞,∞)g'(u) > 0 \quad \forall u \in (-\infty, \infty)

Since the derivative is strictly positive everywhere on its domain, g(u)g(u) is strictly increasing in (−∞,∞)(-\infty, \infty).


Conclusion:

The function gg is odd and is strictly increasing in (−∞,∞)(-\infty, \infty).

Correct Option: C