To determine the properties of the function g(u)=2tan−1(eu)−2π, we analyze its symmetry (parity) and monotonicity.
1. Parity of g(u):
Substitute −u in place of u:
g(−u)=2tan−1(e−u)−2π
Using the inverse trigonometric identity tan−1(x)+tan−1(x1)=2π for x>0, and noting that eu>0 for all u∈(−∞,∞), we have:
tan−1(e−u)=tan−1(eu1)=2π−tan−1(eu)
Substitute this back into the expression for g(−u):
g(−u)=2(2π−tan−1(eu))−2π
g(−u)=π−2tan−1(eu)−2π
g(−u)=2π−2tan−1(eu)
g(−u)=−(2tan−1(eu)−2π)=−g(u)
Since g(−u)=−g(u) for all u∈(−∞,∞), the function g(u) is an odd function.
2. Monotonicity of g(u):
Differentiate g(u) with respect to u:
g′(u)=dud(2tan−1(eu)−2π)
g′(u)=2⋅1+(eu)21⋅dud(eu)
g′(u)=1+e2u2eu
Since eu>0 and 1+e2u>0 for all real numbers u:
g′(u)>0∀u∈(−∞,∞)
Since the derivative is strictly positive everywhere on its domain, g(u) is strictly increasing in (−∞,∞).
Conclusion:
The function g is odd and is strictly increasing in (−∞,∞).
Correct Option: C