y=arcsec⁡xy = \operatorname{arcsec} x

The Inverse Secant y=arcsec⁡xy = \operatorname{arcsec} x

arcsec⁡x\operatorname{arcsec} x, the inverse secant, inverts sec⁡x=1cos⁡x\sec x = \dfrac{1}{\cos x}1. Since sec⁡\sec is periodic, a range must be chosen before an inverse exists, and the usual choice is [0,π][0, \pi], matching arccos⁡\arccos.

Definition and closed form

The equation sec⁡y=x\sec y = x is the same as cos⁡y=1x\cos y = \dfrac{1}{x}, so the function can be written in closed form.

arcsec⁡x=arccos⁡1x\operatorname{arcsec} x = \arccos\frac{1}{x}

Because arccos⁡\arccos is defined on [−1,1][-1, 1], we need ∣1x∣≤1\left|\dfrac{1}{x}\right| \leq 1, that is ∣x∣≥1|x| \geq 1.

Domain and range

  • The domain is x≤−1x \leq -1 or x≥1x \geq 1
  • The range is [0,π][0, \pi] with π2\dfrac{\pi}{2} removed
  • At x=1x = 1 the value is 00, and at x=−1x = -1 it is π\pi

There is no curve on −1<x<1-1 < x < 1, which mirrors the fact that ∣sec⁡y∣≥1|\sec y| \geq 1 always. Attaining π2\dfrac{\pi}{2} would require 1x=0\dfrac{1}{x} = 0, so that value is out of reach too.

Asymptote

As x→+∞x \to +\infty and as x→−∞x \to -\infty alike, 1x→0\dfrac{1}{x} \to 0 and hence y→π2y \to \dfrac{\pi}{2}, so the line y=π2y = \dfrac{\pi}{2} is a horizontal asymptote. The right branch approaches it from below and the left branch from above, so the two branches sandwich it. Since the value π2\dfrac{\pi}{2} is never attained, the asymptote is a boundary in the literal sense.

Notable values

xx1x\dfrac{1}{x}arcsec⁡x\operatorname{arcsec} x
−1-1−1-1π\pi
−2-2−12-\dfrac{1}{2}2π3\dfrac{2\pi}{3}
111100
2\sqrt{2}22\dfrac{\sqrt{2}}{2}π4\dfrac{\pi}{4}
2212\dfrac{1}{2}π3\dfrac{\pi}{3}

Monotonicity and tangents

The derivative is as follows.

ddxarcsec⁡x=1∣x∣x2−1\frac{d}{dx}\operatorname{arcsec} x = \frac{1}{|x|\sqrt{x^{2}-1}}

It is positive throughout the domain, so the function increases on both branches. As ∣x∣→1|x| \to 1 the factor x2−1\sqrt{x^{2}-1} tends to 00 and the derivative diverges, so the tangents at the endpoints (1,0)(1, 0) and (−1,π)(-1, \pi) are vertical. The curve stands up at its ends and lies down along the asymptote far away.

No discontinuity

Because the domain excludes −1<x<1-1 < x < 1, this function has neither jumps nor oscillation. Each branch is continuous and their ranges do not overlap. It too is an inverse taken through a reciprocal, but it avoids the trouble that arises for arccot⁡\operatorname{arccot}, whose domain straddles the origin and where the choice of principal value becomes a genuine question.

Relation to the inverse cosecant

arcsec⁡x+arccsc⁡x=π2\operatorname{arcsec} x + \operatorname{arccsc} x = \frac{\pi}{2}

This is nothing but arccos⁡u+arcsin⁡u=π2\arccos u + \arcsin u = \dfrac{\pi}{2} with u=1xu = \dfrac{1}{x}. The two graphs are therefore reflections of one another in the line y=π4y = \dfrac{\pi}{4}.

  1. Inverse trigonometric functions, Wikipedia