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Reciprocal Trig Functions

You already know the reciprocal trig ratios cosecant, secant, and cotangent. Treating them as functions of an angle gives three new graphs, and each one can be sketched straight from the graph of its “partner”: sin⁡x\sin x, cos⁡x\cos x, or tan⁡x\tan x. All angles on this page are in radians.

csc⁡x=1sin⁡xsec⁡x=1cos⁡xcot⁡x=1tan⁡x=cos⁡xsin⁡x\csc x = \frac{1}{\sin x} \qquad\qquad \sec x = \frac{1}{\cos x} \qquad\qquad \cot x = \frac{1}{\tan x} = \frac{\cos x}{\sin x}

The rules are the same as for any reciprocal function y=1f(x)y = \dfrac{1}{f(x)}:

  • Where f(x)=0f(x) = 0, the reciprocal has a vertical asymptote.
  • Where f(x)=1f(x) = 1 or −1-1, the reciprocal has the same value (since 11=1\tfrac{1}{1} = 1 and 1−1=−1\tfrac{1}{-1} = -1). The graphs touch there.
  • Where f(x)f(x) is small (close to 00), the reciprocal is large, and the other way around.
  • The reciprocal has the same sign as f(x)f(x).

Because −1≤sin⁡x≤1-1 \le \sin x \le 1, its reciprocal is always 11 or more, or −1-1 or less. Where sin⁡x\sin x has a maximum of 11 (at π2\tfrac{\pi}{2}), csc⁡x\csc x has a local minimum of 11; where sin⁡x\sin x has a minimum of −1-1, csc⁡x\csc x has a local maximum of −1-1. The graph is a row of U-shapes, opening up and down alternately.

The same idea with cos⁡x\cos x. The U-shapes touch the cosine curve at its maximums and minimums, (0,1)(0, 1), (π,−1)(\pi, -1), (2π,1)(2\pi, 1), and the asymptotes are where cos⁡x=0\cos x = 0. The graph of y=sec⁡xy = \sec x is the graph of y=csc⁡xy = \csc x shifted π2\tfrac{\pi}{2} to the left, just as cosine is sine shifted π2\tfrac{\pi}{2} to the left.

Top: y = csc x with y = sin x dashed, from -pi to 2 pi. Vertical asymptotes at x = -pi, 0, pi and 2 pi, where sin x = 0. The branches touch the sine curve at (pi/2, 1), (-pi/2, -1) and (3 pi/2, -1). Bottom: y = sec x with y = cos x dashed. Vertical asymptotes at x = -pi/2, pi/2 and 3 pi/2, where cos x = 0. The branches touch the cosine curve at (0, 1), (pi, -1), (-pi, -1) and (2 pi, 1). y = csc x (solid) and y = sin x (dashed) −3 −2 −1 1 2 3 −π −π/2 π/2 π 3π/2 2π y = sec x (solid) and y = cos x (dashed) −3 −2 −1 1 2 3 −π −π/2 π/2 π 3π/2 2π
y=csc⁡xy = \csc x and y=sec⁡xy = \sec x (solid) with their partners y=sin⁡xy = \sin x and y=cos⁡xy = \cos x (dashed).

cot⁡x=cos⁡xsin⁡x\cot x = \dfrac{\cos x}{\sin x} has asymptotes where sin⁡x=0\sin x = 0, at x=nπx = n\pi, and zeros where cos⁡x=0\cos x = 0, at x=π2+nπx = \tfrac{\pi}{2} + n\pi. Those zeros are exactly where tan⁡x\tan x has its asymptotes: when tan⁡x\tan x is huge, its reciprocal is close to 00. Since tan⁡x\tan x increases on each branch, cot⁡x\cot x decreases on each branch.

Graph of y = cot x (solid) with y = tan x (dashed), from -pi to 2 pi. Vertical asymptotes of cot x at x = -pi, 0, pi and 2 pi. Zeros of cot x at -pi/2, pi/2 and 3 pi/2, where tan x has its asymptotes. The two graphs cross wherever tan x = 1 or -1, for example at (pi/4, 1) and (3 pi/4, -1). Each branch of cot x falls from left to right. −3 −2 −1 1 2 3 −π −π/2 π/2 π 3π/2 2π
y=cot⁡xy = \cot x (solid) and y=tan⁡xy = \tan x (dashed). The zeros of one are the asymptotes of the other.

For each, nn is any integer (n∈Zn \in \mathbb{Z}).

y=csc⁡xy = \csc xy=sec⁡xy = \sec xy=cot⁡xy = \cot x
Domain{x∈R∣x≠nπ}\{x \in \mathbb{R} \mid x \ne n\pi\}{x∈R∣x≠π2+nπ}\left\{x \in \mathbb{R} \mid x \ne \tfrac{\pi}{2} + n\pi\right\}{x∈R∣x≠nπ}\{x \in \mathbb{R} \mid x \ne n\pi\}
Range{y∈R∣y≤−1 or y≥1}\{y \in \mathbb{R} \mid y \le -1 \text{ or } y \ge 1\}{y∈R∣y≤−1 or y≥1}\{y \in \mathbb{R} \mid y \le -1 \text{ or } y \ge 1\}{y∈R}\{y \in \mathbb{R}\}
Period2π2\pi2π2\piπ\pi
Asymptotesx=nπx = n\pix=π2+nπx = \tfrac{\pi}{2} + n\pix=nπx = n\pi
Zerosnonenonex=π2+nπx = \tfrac{\pi}{2} + n\pi

Each reciprocal has the same period as its partner, because if ff repeats, so does 1f\tfrac{1}{f}.

The reciprocal of sin⁡x\sin x can be written as

csc⁡xor1sin⁡xor(sin⁡x)−1\csc x \qquad\text{or}\qquad \frac{1}{\sin x} \qquad\text{or}\qquad (\sin x)^{-1}

but not as sin⁡−1x\sin^{-1} x. The notation sin⁡−1x\sin^{-1} x (like f−1(x)f^{-1}(x) for inverse functions) means the inverse sine: the angle whose sine is xx. That’s a completely different thing. For example:

sin⁡−1(0.5)=π6≈0.524butcsc⁡(0.5)=1sin⁡0.5≈2.086\sin^{-1}(0.5) = \frac{\pi}{6} \approx 0.524 \qquad\text{but}\qquad \csc(0.5) = \frac{1}{\sin 0.5} \approx 2.086

This is an awkward exception: sin⁡2x\sin^2 x does mean (sin⁡x)2(\sin x)^2, but sin⁡−1x\sin^{-1} x does not mean (sin⁡x)−1(\sin x)^{-1}.

Example 1: Sketching y = sec x from y = cos x

Section titled “Example 1: Sketching y = sec x from y = cos x”

Describe how to sketch y=sec⁡xy = \sec x for 0≤x≤2π0 \le x \le 2\pi, starting from the graph of y=cos⁡xy = \cos x.

Solution. Work through the features of y=cos⁡xy = \cos x one at a time (see the bottom graph above).

  1. Zeros of cos x become asymptotes. cos⁡x=0\cos x = 0 at x=π2x = \tfrac{\pi}{2} and 3π2\tfrac{3\pi}{2}, so draw dashed vertical asymptotes there.
  2. Points where cos x = ±1 stay put. Mark (0,1)(0, 1), (π,−1)(\pi, -1), and (2π,1)(2\pi, 1). They’re on both graphs.
  3. Same sign, opposite size. From 00 to π2\tfrac{\pi}{2}, cos⁡x\cos x falls from 11 toward 00, so sec⁡x\sec x rises from 11 toward the asymptote. From π2\tfrac{\pi}{2} to 3π2\tfrac{3\pi}{2}, cos⁡x\cos x is negative, so sec⁡x\sec x is a downward U with its highest point at (π,−1)(\pi, -1). From 3π2\tfrac{3\pi}{2} to 2π2\pi, sec⁡x\sec x comes down from the asymptote to (2π,1)(2\pi, 1).

Check a point: sec⁡π3=1cos⁡(π/3)=11/2=2\sec\tfrac{\pi}{3} = \dfrac{1}{\cos(\pi/3)} = \dfrac{1}{1/2} = 2, on the first rising piece. ✓

Example 2: Properties of y = csc x on an interval

Section titled “Example 2: Properties of y = csc x on an interval”

For −2π≤x≤2π-2\pi \le x \le 2\pi, give the equations of the vertical asymptotes of y=csc⁡xy = \csc x, and all its local maximum and minimum points.

Solution. Asymptotes are where sin⁡x=0\sin x = 0:

x=−2π,x=−π,x=0,x=π,x=2πx = -2\pi,\quad x = -\pi,\quad x = 0,\quad x = \pi,\quad x = 2\pi

Local minimums (value 11) are where sin⁡x=1\sin x = 1: (−3π2,1)\left(-\tfrac{3\pi}{2}, 1\right) and (π2,1)\left(\tfrac{\pi}{2}, 1\right).

Local maximums (value −1-1) are where sin⁡x=−1\sin x = -1: (−π2,−1)\left(-\tfrac{\pi}{2}, -1\right) and (3π2,−1)\left(\tfrac{3\pi}{2}, -1\right).

Evaluate, if possible, to 44 decimal places: (a) csc⁡1.2\csc 1.2 (b) sin⁡−11.2\sin^{-1} 1.2 (c) cot⁡2\cot 2

Solution. In radian mode:

(a) csc⁡1.2=1sin⁡1.2≈10.9320≈1.0729\csc 1.2 = \dfrac{1}{\sin 1.2} \approx \dfrac{1}{0.9320} \approx 1.0729

(b) sin⁡−11.2\sin^{-1} 1.2 asks for an angle whose sine is 1.21.2. There isn’t one, because sine is never bigger than 11, so the calculator gives an error. This is a good reminder that sin⁡−1\sin^{-1} is not cosecant.

(c) cot⁡2=1tan⁡2≈1−2.1850≈−0.4577\cot 2 = \dfrac{1}{\tan 2} \approx \dfrac{1}{-2.1850} \approx -0.4577

Check (c) with CAST: 22 is between π2\tfrac{\pi}{2} and π\pi, in quadrant II, where tangent and cotangent are negative. ✓

Example 4: Explaining the asymptotes and zeros of cot x

Section titled “Example 4: Explaining the asymptotes and zeros of cot x”

For 0≤x≤2π0 \le x \le 2\pi, where is y=cot⁡xy = \cot x undefined, and where is it zero? Explain each using cot⁡x=cos⁡xsin⁡x\cot x = \dfrac{\cos x}{\sin x}.

Solution.

  • Undefined where the denominator sin⁡x=0\sin x = 0: x=0x = 0, π\pi, and 2π2\pi. Near these values, sin⁡x\sin x is tiny while cos⁡x\cos x is close to ±1\pm 1, so cot⁡x\cot x is huge: these are vertical asymptotes.
  • Zero where the numerator cos⁡x=0\cos x = 0 (and sin⁡x≠0\sin x \ne 0): x=π2x = \tfrac{\pi}{2} and 3π2\tfrac{3\pi}{2}.

Check: cot⁡π2=cos⁡(π/2)sin⁡(π/2)=01=0\cot\tfrac{\pi}{2} = \dfrac{\cos(\pi/2)}{\sin(\pi/2)} = \dfrac{0}{1} = 0. ✓ (You can’t get this from 1tan⁡(π/2)\dfrac{1}{\tan(\pi/2)}, since tan⁡π2\tan\tfrac{\pi}{2} is undefined, which is why the form cos⁡xsin⁡x\dfrac{\cos x}{\sin x} is useful.)

Writing sin⁻¹ x for csc x. sin⁡−1x\sin^{-1} x is the inverse sine (an angle). The reciprocal is csc⁡x\csc x, 1sin⁡x\dfrac{1}{\sin x}, or (sin⁡x)−1(\sin x)^{-1}.

Putting the asymptotes in the wrong places. The reciprocal’s asymptotes are at the zeros of its partner. For sec⁡x\sec x, that’s where cos⁡x=0\cos x = 0, at π2+nπ\tfrac{\pi}{2} + n\pi, not where sin⁡x=0\sin x = 0.

Drawing csc x or sec x between −1 and 1. Their range is y≤−1y \le -1 or y≥1y \ge 1. If a branch dips below 11 (or rises above −1-1), it’s wrong: the U-shapes only touch y=±1y = \pm 1 at their turning points.

Mixing up maximums and minimums. A maximum of sin⁡x\sin x becomes a local minimum of csc⁡x\csc x, because the U opens away from the axis.

Giving cot x a period of 2π. Like tangent, cotangent repeats every π\pi.

1. (Warm-up) Find the exact value: (a) csc⁡π6\csc\dfrac{\pi}{6} (b) sec⁡π3\sec\dfrac{\pi}{3} (c) cot⁡π4\cot\dfrac{\pi}{4}

Solution

(a) 1sin⁡(π/6)=11/2=2\dfrac{1}{\sin(\pi/6)} = \dfrac{1}{1/2} = 2

(b) 1cos⁡(π/3)=11/2=2\dfrac{1}{\cos(\pi/3)} = \dfrac{1}{1/2} = 2

(c) 1tan⁡(π/4)=11=1\dfrac{1}{\tan(\pi/4)} = \dfrac{1}{1} = 1

2. (Warm-up) Evaluate to 33 decimal places: (a) sec⁡2.5\sec 2.5 (b) csc⁡0.3\csc 0.3 (c) cot⁡4\cot 4

Solution

(a) sec⁡2.5=1cos⁡2.5≈−1.248\sec 2.5 = \dfrac{1}{\cos 2.5} \approx -1.248

(b) csc⁡0.3=1sin⁡0.3≈3.384\csc 0.3 = \dfrac{1}{\sin 0.3} \approx 3.384

(c) cot⁡4=1tan⁡4≈0.864\cot 4 = \dfrac{1}{\tan 4} \approx 0.864

3. (Warm-up) Which of these mean the reciprocal of sin⁡x\sin x? (a) sin⁡−1x\sin^{-1} x (b) csc⁡x\csc x (c) 1sin⁡x\dfrac{1}{\sin x} (d) (sin⁡x)−1(\sin x)^{-1}

Solution

(b), (c), and (d). Choice (a), sin⁡−1x\sin^{-1} x, is the inverse sine function.

4. (Core) State the domain, range, and period of y=sec⁡xy = \sec x, and the equations of its asymptotes for −π≤x≤π-\pi \le x \le \pi.

Solution

Domain {x∈R∣x≠π2+nπ, n∈Z}\left\{x \in \mathbb{R} \mid x \ne \tfrac{\pi}{2} + n\pi,\ n \in \mathbb{Z}\right\}. Range {y∈R∣y≤−1 or y≥1}\{y \in \mathbb{R} \mid y \le -1 \text{ or } y \ge 1\}. Period 2π2\pi.

Asymptotes for −π≤x≤π-\pi \le x \le \pi: x=−π2x = -\dfrac{\pi}{2} and x=π2x = \dfrac{\pi}{2}.

5. (Core) For 0≤x≤2π0 \le x \le 2\pi: (a) where does csc⁡x=1\csc x = 1? (b) where does csc⁡x=−1\csc x = -1? (c) where does sec⁡x=−1\sec x = -1?

Solution

(a) csc⁡x=1\csc x = 1 when sin⁡x=1\sin x = 1: x=π2x = \dfrac{\pi}{2}.

(b) csc⁡x=−1\csc x = -1 when sin⁡x=−1\sin x = -1: x=3π2x = \dfrac{3\pi}{2}.

(c) sec⁡x=−1\sec x = -1 when cos⁡x=−1\cos x = -1: x=πx = \pi.

6. (Core) y=sin⁡xy = \sin x has a maximum at (π2,1)\left(\tfrac{\pi}{2}, 1\right), but y=csc⁡xy = \csc x has a local minimum there. Explain why.

Solution

Near x=π2x = \tfrac{\pi}{2}, sin⁡x\sin x is at most 11, and slightly less than 11 on either side. Dividing 11 by a number slightly less than 11 gives a number slightly more than 11. So csc⁡x\csc x equals 11 at π2\tfrac{\pi}{2} and is bigger than 11 on either side, which makes (π2,1)\left(\tfrac{\pi}{2}, 1\right) a local minimum. The biggest value of sin⁡x\sin x gives the smallest value of its reciprocal.

7. (Core) For −2π≤x≤2π-2\pi \le x \le 2\pi, give the equations of the asymptotes and the zeros of y=cot⁡xy = \cot x.

Solution

Asymptotes where sin⁡x=0\sin x = 0: x=−2πx = -2\pi, x=−πx = -\pi, x=0x = 0, x=πx = \pi, x=2πx = 2\pi.

Zeros where cos⁡x=0\cos x = 0: x=−3π2,−π2,π2,3π2x = -\dfrac{3\pi}{2}, -\dfrac{\pi}{2}, \dfrac{\pi}{2}, \dfrac{3\pi}{2}.

8. (Challenge) Find all xx with 0≤x≤2π0 \le x \le 2\pi such that (a) sec⁡x=2\sec x = 2 (b) csc⁡x=−2\csc x = -\sqrt{2}.

Solution

(a) sec⁡x=2\sec x = 2 means cos⁡x=12\cos x = \tfrac{1}{2}. The related angle is π3\tfrac{\pi}{3}, and cosine is positive in quadrants I and IV:

x=π3orx=5π3x = \frac{\pi}{3} \qquad\text{or}\qquad x = \frac{5\pi}{3}

(b) csc⁡x=−2\csc x = -\sqrt{2} means sin⁡x=−12=−22\sin x = -\tfrac{1}{\sqrt{2}} = -\tfrac{\sqrt{2}}{2}. The related angle is π4\tfrac{\pi}{4}, and sine is negative in quadrants III and IV:

x=5π4orx=7π4x = \frac{5\pi}{4} \qquad\text{or}\qquad x = \frac{7\pi}{4}

9. (Challenge) State the period and range of y=csc⁡(2x)y = \csc(2x), and the equations of its asymptotes for 0≤x≤2π0 \le x \le 2\pi.

Solution

y=sin⁡(2x)y = \sin(2x) has period 2π2=π\tfrac{2\pi}{2} = \pi, so its reciprocal y=csc⁡(2x)y = \csc(2x) also has period π\pi. A horizontal compression doesn’t change the yy-values, so the range is still {y∈R∣y≤−1 or y≥1}\{y \in \mathbb{R} \mid y \le -1 \text{ or } y \ge 1\}.

Asymptotes where sin⁡(2x)=0\sin(2x) = 0: 2x=nπ2x = n\pi, so x=nπ2x = \tfrac{n\pi}{2}:

x=0,x=π2,x=π,x=3π2,x=2πx = 0,\quad x = \frac{\pi}{2},\quad x = \pi,\quad x = \frac{3\pi}{2},\quad x = 2\pi