List of Integrals of Hyperbolic Functions: Full Tables

#Calculus
TL;DR
The integral of sinh x is cosh x + C, with no minus sign. This list of integrals of hyperbolic functions gives every standard form with its domain, derivation and worked examples.
BT
Bhanzu TeamLast updated on October 11, 202618 min read

What Is The List Of Integrals Of Hyperbolic Functions?

The list of integrals of hyperbolic functions is the set of antiderivatives for sinh⁡x\sinh x, cosh⁡x\cosh x, tanh⁡x\tanh x, coth⁡x\coth x, sech⁡x\operatorname{sech} x and csch⁡x\operatorname{csch} x, together with their powers, products, inverse functions and the algebraic integrals whose answers are inverse hyperbolic functions. Every entry below was checked by differentiating the answer back to the integrand.

The hyperbolic functions are built from the exponential function:

sinh⁡x=ex−e−x2,cosh⁡x=ex+e−x2,\sinh x = \frac{e^{x} - e^{-x}}{2}, \qquad \cosh x = \frac{e^{x} + e^{-x}}{2},

with tanh⁡x=sinh⁡xcosh⁡x\tanh x = \frac{\sinh x}{\cosh x}, coth⁡x=cosh⁡xsinh⁡x\coth x = \frac{\cosh x}{\sinh x}, sech⁡x=1cosh⁡x\operatorname{sech} x = \frac{1}{\cosh x} and csch⁡x=1sinh⁡x\operatorname{csch} x = \frac{1}{\sinh x}. The full background on their graphs and identities sits on the hyperbolic functions page, so this list keeps to integration.

Three conventions run through every table:

  • CC is the arbitrary constant of integration, and it appears on every indefinite integral.

  • aa is a positive constant unless a row says otherwise.

  • "Valid for" gives the interval of xx on which the formula is a true antiderivative. Outside it, the integrand or the answer is undefined.

What Are The Integrals Of The Six Hyperbolic Functions?

The six basic integrals are below. The first two reverse the derivative rules directly; the other four each need one substitution, explained under the table.

Integrand

Integral

Valid for

sinh⁡x\sinh x

cosh⁡x+C\cosh x + C

all real xx

cosh⁡x\cosh x

sinh⁡x+C\sinh x + C

all real xx

tanh⁡x\tanh x

ln⁡(cosh⁡x)+C\ln(\cosh x) + C

all real xx

coth⁡x\coth x

ln⁡∣sinh⁡x∣+C\ln\lvert\sinh x\rvert + C

x≠0x \neq 0

sech⁡x\operatorname{sech} x

arctan⁡(sinh⁡x)+C\arctan(\sinh x) + C

all real xx

csch⁡x\operatorname{csch} x

ln⁡∣tanh⁡x2∣+C\ln\left\lvert\tanh\frac{x}{2}\right\rvert + C

x≠0x \neq 0

With a constant inside, divide by that constant: ∫sinh⁡(ax),dx=1acosh⁡(ax)+C\int \sinh(ax),dx = \frac{1}{a}\cosh(ax) + C and ∫cosh⁡(ax),dx=1asinh⁡(ax)+C\int \cosh(ax),dx = \frac{1}{a}\sinh(ax) + C.

These match NIST's reference list in the Digital Library of Mathematical Functions, section 4.40, which writes the coth and csch rows for x>0x > 0 without the absolute value.

How Do You Integrate Tanh And Coth?

Write each as a ratio and substitute the denominator. This answers a question that comes up on Quora as "How to evaluate an integral with tangent hyperbolic or cotangent hyperbolic".

For tanh⁡x=sinh⁡xcosh⁡x\tanh x = \frac{\sinh x}{\cosh x}, let u=cosh⁡xu = \cosh x, so du=sinh⁡x,dxdu = \sinh x,dx:

∫tanh⁡x,dx=∫sinh⁡xcosh⁡x,dx\int \tanh x,dx = \int \frac{\sinh x}{\cosh x},dx

=∫duu= \int \frac{du}{u}

=ln⁡∣u∣+C= \ln\lvert u\rvert + C

=ln⁡(cosh⁡x)+C= \ln(\cosh x) + C

The absolute value can go because cosh⁡x≥1\cosh x \geq 1 for every xx. For coth⁡x\coth x the same move with u=sinh⁡xu = \sinh x gives ln⁡∣sinh⁡x∣+C\ln\lvert\sinh x\rvert + C, and here the absolute value must stay, since sinh⁡x<0\sinh x < 0 whenever x<0x < 0. This is the integration by substitution pattern ∫f′(x)f(x),dx=ln⁡∣f(x)∣+C\int \frac{f'(x)}{f(x)},dx = \ln\lvert f(x)\rvert + C.

Why Does Sech Have Several Different Antiderivatives?

A Pearson Q&A puts it plainly: "There are several ways to express the indefinite integral of sech x". All of them are correct, because they differ only by a constant.

Multiply top and bottom by cosh⁡x\cosh x and use cosh⁡2x=1+sinh⁡2x\cosh^2 x = 1 + \sinh^2 x:

∫sech⁡x,dx=∫cosh⁡xcosh⁡2x,dx\int \operatorname{sech} x,dx = \int \frac{\cosh x}{\cosh^2 x},dx

=∫cosh⁡x1+sinh⁡2x,dx= \int \frac{\cosh x}{1 + \sinh^2 x},dx

=arctan⁡(sinh⁡x)+C= \arctan(\sinh x) + C

with u=sinh⁡xu = \sinh x in the last step. Three other forms appear in textbooks:

  • 2arctan⁡(ex)+C2\arctan\left(e^{x}\right) + C, from the exponential form sech⁡x=2exe2x+1\operatorname{sech} x = \frac{2e^{x}}{e^{2x} + 1}.

  • 2arctan⁡(tanh⁡x2)+C2\arctan\left(\tanh\frac{x}{2}\right) + C, from a half-argument substitution.

  • gd⁡x+C\operatorname{gd} x + C, the Gudermannian function, which is how NIST writes it.

Checking these against each other is worth doing once. arctan⁡(sinh⁡x)\arctan(\sinh x) and 2arctan⁡(ex)2\arctan\left(e^{x}\right) differ by exactly π2\frac{\pi}{2} at every xx, so they are the same antiderivative with different constants. The rule this teaches: two answers that look nothing alike can both be right, and the test is to differentiate them, not to compare them by eye.

How Do You Integrate Csch?

Rewrite csch⁡x\operatorname{csch} x in exponentials and substitute u=exu = e^{x}, so dx=duudx = \frac{du}{u}:

∫csch⁡x,dx=∫2exe2x−1,dx\int \operatorname{csch} x,dx = \int \frac{2e^{x}}{e^{2x} - 1},dx

=∫2u2−1,du= \int \frac{2}{u^{2} - 1},du

=ln⁡∣u−1u+1∣+C= \ln\left\lvert\frac{u - 1}{u + 1}\right\rvert + C

=ln⁡∣ex−1ex+1∣+C= \ln\left\lvert\frac{e^{x} - 1}{e^{x} + 1}\right\rvert + C

The step from the second line to the third is integration by partial fractions, since 2u2−1=1u−1−1u+1\frac{2}{u^{2} - 1} = \frac{1}{u - 1} - \frac{1}{u + 1}. The fraction ex−1ex+1\frac{e^{x} - 1}{e^{x} + 1} equals tanh⁡x2\tanh\frac{x}{2}, which gives the table entry ln⁡∣tanh⁡x2∣+C\ln\left\lvert\tanh\frac{x}{2}\right\rvert + C.

Which Integrals Come From Reading The Derivative Table Backwards?

Every derivative rule is also an integral rule read from right to left. Four hyperbolic derivatives give four integrals that are worth knowing on sight.

Integrand

Integral

Valid for

Comes from

sech⁡2x\operatorname{sech}^2 x

tanh⁡x+C\tanh x + C

all real xx

ddxtanh⁡x=sech⁡2x\frac{d}{dx}\tanh x = \operatorname{sech}^2 x

csch⁡2x\operatorname{csch}^2 x

−coth⁡x+C-\coth x + C

x≠0x \neq 0

ddxcoth⁡x=−csch⁡2x\frac{d}{dx}\coth x = -\operatorname{csch}^2 x

sech⁡xtanh⁡x\operatorname{sech} x\tanh x

−sech⁡x+C-\operatorname{sech} x + C

all real xx

ddxsech⁡x=−sech⁡xtanh⁡x\frac{d}{dx}\operatorname{sech} x = -\operatorname{sech} x\tanh x

csch⁡xcoth⁡x\operatorname{csch} x\coth x

−csch⁡x+C-\operatorname{csch} x + C

x≠0x \neq 0

ddxcsch⁡x=−csch⁡xcoth⁡x\frac{d}{dx}\operatorname{csch} x = -\operatorname{csch} x\coth x

The minus signs in this table copy the minus signs in the derivative table. Only the reciprocal functions (coth⁡\coth, sech⁡\operatorname{sech}, csch⁡\operatorname{csch}) have negative derivatives, so only their reversed rows carry a minus.

What Are The Integrals Of Powers And Products Of Hyperbolic Functions?

Powers and products reduce to the basic six through an identity, a substitution or integration by parts. The derivation column says which.

Integrand

Integral

How it is derived

sinh⁡2x\sinh^2 x

sinh⁡2x4−x2+C\frac{\sinh 2x}{4} - \frac{x}{2} + C

sinh⁡2x=cosh⁡2x−12\sinh^2 x = \frac{\cosh 2x - 1}{2}

cosh⁡2x\cosh^2 x

sinh⁡2x4+x2+C\frac{\sinh 2x}{4} + \frac{x}{2} + C

cosh⁡2x=cosh⁡2x+12\cosh^2 x = \frac{\cosh 2x + 1}{2}

tanh⁡2x\tanh^2 x

x−tanh⁡x+Cx - \tanh x + C

tanh⁡2x=1−sech⁡2x\tanh^2 x = 1 - \operatorname{sech}^2 x

coth⁡2x\coth^2 x, x≠0x \neq 0

x−coth⁡x+Cx - \coth x + C

coth⁡2x=1+csch⁡2x\coth^2 x = 1 + \operatorname{csch}^2 x

sinh⁡xcosh⁡x\sinh x\cosh x

sinh⁡2x2+C\frac{\sinh^2 x}{2} + C

u=sinh⁡xu = \sinh x

sinh⁡3x\sinh^3 x

cosh⁡3x3−cosh⁡x+C\frac{\cosh^3 x}{3} - \cosh x + C

sinh⁡3x=(cosh⁡2x−1)sinh⁡x\sinh^3 x = (\cosh^2 x - 1)\sinh x, u=cosh⁡xu = \cosh x

cosh⁡3x\cosh^3 x

sinh⁡x+sinh⁡3x3+C\sinh x + \frac{\sinh^3 x}{3} + C

cosh⁡3x=(1+sinh⁡2x)cosh⁡x\cosh^3 x = (1 + \sinh^2 x)\cosh x, u=sinh⁡xu = \sinh x

xsinh⁡(ax)x\sinh(ax)

xcosh⁡(ax)a−sinh⁡(ax)a2+C\frac{x\cosh(ax)}{a} - \frac{\sinh(ax)}{a^{2}} + C

by parts, u=xu = x

xcosh⁡(ax)x\cosh(ax)

xsinh⁡(ax)a−cosh⁡(ax)a2+C\frac{x\sinh(ax)}{a} - \frac{\cosh(ax)}{a^{2}} + C

by parts, u=xu = x

exsinh⁡xe^{x}\sinh x

e2x4−x2+C\frac{e^{2x}}{4} - \frac{x}{2} + C

exsinh⁡x=e2x−12e^{x}\sinh x = \frac{e^{2x} - 1}{2}

excosh⁡xe^{x}\cosh x

e2x4+x2+C\frac{e^{2x}}{4} + \frac{x}{2} + C

excosh⁡x=e2x+12e^{x}\cosh x = \frac{e^{2x} + 1}{2}

Two notes on this table. The sinh⁡xcosh⁡x\sinh x\cosh x row has other correct forms, such as cosh⁡2x2+C\frac{\cosh^2 x}{2} + C and cosh⁡2x4+C\frac{\cosh 2x}{4} + C, and each differs from the others by a constant. The square rows come from the double-argument identity cosh⁡2x=1+2sinh⁡2x=2cosh⁡2x−1\cosh 2x = 1 + 2\sinh^2 x = 2\cosh^2 x - 1, the hyperbolic twin of the one used for ∫sin⁡2x,dx\int \sin^2 x,dx in integration of trigonometric functions.

What Are The Integrals Of Inverse Hyperbolic Functions?

Each inverse hyperbolic function integrates by parts with uu equal to the inverse function and dv=dxdv = dx. For sinh⁡−1x\sinh^{-1} x (also written arsinh⁡x\operatorname{arsinh} x):

∫sinh⁡−1x,dx=xsinh⁡−1x−∫xx2+1,dx\int \sinh^{-1} x,dx = x\sinh^{-1} x - \int \frac{x}{\sqrt{x^{2} + 1}},dx

=xsinh⁡−1x−x2+1+C= x\sinh^{-1} x - \sqrt{x^{2} + 1} + C

The remaining integral uses w=x2+1w = x^{2} + 1. The same two steps produce the whole table.

Integrand

Integral

Valid for

sinh⁡−1x\sinh^{-1} x

xsinh⁡−1x−x2+1+Cx\sinh^{-1} x - \sqrt{x^{2} + 1} + C

all real xx

cosh⁡−1x\cosh^{-1} x

xcosh⁡−1x−x2−1+Cx\cosh^{-1} x - \sqrt{x^{2} - 1} + C

x>1x > 1

tanh⁡−1x\tanh^{-1} x

xtanh⁡−1x+12ln⁡(1−x2)+Cx\tanh^{-1} x + \frac{1}{2}\ln\left(1 - x^{2}\right) + C

∣x∣<1\lvert x\rvert < 1

coth⁡−1x\coth^{-1} x

xcoth⁡−1x+12ln⁡(x2−1)+Cx\coth^{-1} x + \frac{1}{2}\ln\left(x^{2} - 1\right) + C

∣x∣>1\lvert x\rvert > 1

sech⁡−1x\operatorname{sech}^{-1} x

xsech⁡−1x+arcsin⁡x+Cx\operatorname{sech}^{-1} x + \arcsin x + C

0<x<10 < x < 1

csch⁡−1x\operatorname{csch}^{-1} x

xcsch⁡−1x+sinh⁡−1∣x∣+Cx\operatorname{csch}^{-1} x + \sinh^{-1}\lvert x\rvert + C

x≠0x \neq 0

The csch row is the one most lists get half right. NIST gives xcsch⁡−1x+sinh⁡−1xx\operatorname{csch}^{-1} x + \sinh^{-1} x for x>0x > 0 only; for negative xx the sign of the second term flips, and writing sinh⁡−1∣x∣\sinh^{-1}\lvert x\rvert covers both sides at once.

Which Integrals Give Inverse Hyperbolic Functions As The Answer?

This is the part of the list you will use most. Square roots of x2+a2x^{2} + a^{2} and x2−a2x^{2} - a^{2}, and the fraction 1a2−x2\frac{1}{a^{2} - x^{2}}, all integrate to inverse hyperbolic functions, with a>0a > 0:

Integrand

Integral

Logarithm form

Valid for

1x2+a2\frac{1}{\sqrt{x^{2} + a^{2}}}

sinh⁡−1xa+C\sinh^{-1}\frac{x}{a} + C

ln⁡(x+x2+a2)+C\ln\left(x + \sqrt{x^{2} + a^{2}}\right) + C

all real xx

1x2−a2\frac{1}{\sqrt{x^{2} - a^{2}}}

cosh⁡−1xa+C\cosh^{-1}\frac{x}{a} + C

ln⁡(x+x2−a2)+C\ln\left(x + \sqrt{x^{2} - a^{2}}\right) + C

x>ax > a

1a2−x2\frac{1}{a^{2} - x^{2}}

1atanh⁡−1xa+C\frac{1}{a}\tanh^{-1}\frac{x}{a} + C

12aln⁡a+xa−x+C\frac{1}{2a}\ln\frac{a + x}{a - x} + C

∣x∣<a\lvert x\rvert < a

1a2−x2\frac{1}{a^{2} - x^{2}}

1acoth⁡−1xa+C\frac{1}{a}\coth^{-1}\frac{x}{a} + C

12aln⁡x+ax−a+C\frac{1}{2a}\ln\frac{x + a}{x - a} + C

∣x∣>a\lvert x\rvert > a

1xa2−x2\frac{1}{x\sqrt{a^{2} - x^{2}}}

−1asech⁡−1xa+C-\frac{1}{a}\operatorname{sech}^{-1}\frac{x}{a} + C

−1aln⁡a+a2−x2x+C-\frac{1}{a}\ln\frac{a + \sqrt{a^{2} - x^{2}}}{x} + C

0<x<a0 < x < a

1xa2+x2\frac{1}{x\sqrt{a^{2} + x^{2}}}

−1acsch⁡−1∣x∣a+C-\frac{1}{a}\operatorname{csch}^{-1}\frac{\lvert x\rvert}{a} + C

−1aln⁡a+a2+x2∣x∣+C-\frac{1}{a}\ln\frac{a + \sqrt{a^{2} + x^{2}}}{\lvert x\rvert} + C

x≠0x \neq 0

x2+a2\sqrt{x^{2} + a^{2}}

xx2+a22+a22sinh⁡−1xa+C\frac{x\sqrt{x^{2} + a^{2}}}{2} + \frac{a^{2}}{2}\sinh^{-1}\frac{x}{a} + C

xx2+a22+a22ln⁡(x+x2+a2)+C\frac{x\sqrt{x^{2} + a^{2}}}{2} + \frac{a^{2}}{2}\ln\left(x + \sqrt{x^{2} + a^{2}}\right) + C

all real xx

The two forms in each row agree up to a constant. The logarithm form is what most exam answer keys expect, and the inverse hyperbolic form is shorter to write; the general list of integrals uses the logarithm versions.

Why do these integrals land on hyperbolic functions at all? Substitute x=asinh⁡tx = a\sinh t in the first row. Then dx=acosh⁡t,dtdx = a\cosh t,dt and x2+a2=acosh⁡t\sqrt{x^{2} + a^{2}} = a\cosh t, so the integrand collapses to 11 and the integral is t=sinh⁡−1xat = \sinh^{-1}\frac{x}{a}. This is the hyperbolic version of trigonometric substitution, where x=atan⁡θx = a\tan\theta does the same job with a messier answer.

Note the two 1a2−x2\frac{1}{a^{2} - x^{2}} rows. The integrand is the same, but tanh⁡−1\tanh^{-1} only accepts inputs between −1-1 and 11, so the answer switches to coth⁡−1\coth^{-1} outside that interval.

How Do Hyperbolic Integrals Compare With Trigonometric Integrals?

The hyperbolic list mirrors the trig list, with sign changes in predictable places. Side by side:

Trig integral

Result

Hyperbolic integral

Result

∫sin⁡x,dx\int \sin x,dx

−cos⁡x+C-\cos x + C

∫sinh⁡x,dx\int \sinh x,dx

cosh⁡x+C\cosh x + C

∫cos⁡x,dx\int \cos x,dx

sin⁡x+C\sin x + C

∫cosh⁡x,dx\int \cosh x,dx

sinh⁡x+C\sinh x + C

∫tan⁡x,dx\int \tan x,dx

−ln⁡∣cos⁡x∣+C-\ln\lvert\cos x\rvert + C

∫tanh⁡x,dx\int \tanh x,dx

ln⁡(cosh⁡x)+C\ln(\cosh x) + C

∫sec⁡2x,dx\int \sec^2 x,dx

tan⁡x+C\tan x + C

∫sech⁡2x,dx\int \operatorname{sech}^2 x,dx

tanh⁡x+C\tanh x + C

∫sin⁡2x,dx\int \sin^2 x,dx

x2−sin⁡2x4+C\frac{x}{2} - \frac{\sin 2x}{4} + C

∫sinh⁡2x,dx\int \sinh^2 x,dx

sinh⁡2x4−x2+C\frac{\sinh 2x}{4} - \frac{x}{2} + C

∫dxa2−x2\int \frac{dx}{\sqrt{a^{2} - x^{2}}}

arcsin⁡xa+C\arcsin\frac{x}{a} + C

∫dxx2+a2\int \frac{dx}{\sqrt{x^{2} + a^{2}}}

sinh⁡−1xa+C\sinh^{-1}\frac{x}{a} + C

The sign differences trace back to one fact: ddxcos⁡x=−sin⁡x\frac{d}{dx}\cos x = -\sin x but ddxcosh⁡x=sinh⁡x\frac{d}{dx}\cosh x = \sinh x. Every trig minus sign that comes from differentiating cosine disappears in the hyperbolic column.

Examples Of Integrals Of Hyperbolic Functions

Example 1

Evaluate ∫cosh⁡(3x),dx\int \cosh(3x),dx.

Use the cosh⁡(ax)\cosh(ax) row with a=3a = 3:

∫cosh⁡(3x),dx=13sinh⁡(3x)+C\int \cosh(3x),dx = \frac{1}{3}\sinh(3x) + C

Check: ddx[13sinh⁡(3x)]=13⋅3cosh⁡(3x)=cosh⁡(3x)\frac{d}{dx}\left[\frac{1}{3}\sinh(3x)\right] = \frac{1}{3}\cdot 3\cosh(3x) = \cosh(3x).

Final answer: 13sinh⁡(3x)+C\frac{1}{3}\sinh(3x) + C

Example 2

Evaluate ∫0ln⁡2sinh⁡x,dx\int_{0}^{\ln 2} \sinh x,dx.

The trig habit says the integral of a sine is minus a cosine, so a first attempt reads:

[−cosh⁡x]0ln⁡2=−cosh⁡(ln⁡2)+cosh⁡0\left[-\cosh x\right]_{0}^{\ln 2} = -\cosh(\ln 2) + \cosh 0

With cosh⁡(ln⁡2)=2+122=54\cosh(\ln 2) = \frac{2 + \frac{1}{2}}{2} = \frac{5}{4}, this gives −54+1=−14-\frac{5}{4} + 1 = -\frac{1}{4}. But sinh⁡x>0\sinh x > 0 for every x>0x > 0, so the area under it from 00 to ln⁡2\ln 2 must be positive. A negative answer cannot be right.

The minus sign belongs to ∫sin⁡x,dx\int \sin x,dx, not to ∫sinh⁡x,dx\int \sinh x,dx. Since ddxcosh⁡x=sinh⁡x\frac{d}{dx}\cosh x = \sinh x, the antiderivative is cosh⁡x\cosh x:

∫0ln⁡2sinh⁡x,dx=[cosh⁡x]0ln⁡2\int_{0}^{\ln 2} \sinh x,dx = \left[\cosh x\right]_{0}^{\ln 2}

=cosh⁡(ln⁡2)−cosh⁡0= \cosh(\ln 2) - \cosh 0

=54−1= \frac{5}{4} - 1

=14= \frac{1}{4}

Final answer: 14\frac{1}{4}

Example 3

Evaluate ∫sech⁡xtanh⁡xsech⁡x,dx\int \operatorname{sech} x\tanh x\operatorname{sech} x,dx.

This is a Vedantu Q&A question, "How do you integrate sech x tanh x sech x dx". Collect the factors first: the integrand is sech⁡2xtanh⁡x\operatorname{sech}^2 x\tanh x. Let u=tanh⁡xu = \tanh x, so du=sech⁡2x,dxdu = \operatorname{sech}^2 x,dx:

∫sech⁡2xtanh⁡x,dx=∫u,du\int \operatorname{sech}^2 x\tanh x,dx = \int u,du

=u22+C= \frac{u^{2}}{2} + C

=tanh⁡2x2+C= \frac{\tanh^2 x}{2} + C

Choosing u=sech⁡xu = \operatorname{sech} x instead gives −sech⁡2x2+C-\frac{\operatorname{sech}^2 x}{2} + C. Both are correct, because tanh⁡2x2=12−sech⁡2x2\frac{\tanh^2 x}{2} = \frac{1}{2} - \frac{\operatorname{sech}^2 x}{2}, so they differ by the constant 12\frac{1}{2}.

Final answer: tanh⁡2x2+C\frac{\tanh^2 x}{2} + C (equivalently −sech⁡2x2+C-\frac{\operatorname{sech}^2 x}{2} + C)

Example 4

Evaluate ∫xcosh⁡(2x),dx\int x\cosh(2x),dx.

Use integration by parts with u=xu = x and dv=cosh⁡(2x),dxdv = \cosh(2x),dx, so du=dxdu = dx and v=12sinh⁡(2x)v = \frac{1}{2}\sinh(2x):

∫xcosh⁡(2x),dx=x2sinh⁡(2x)−∫12sinh⁡(2x),dx\int x\cosh(2x),dx = \frac{x}{2}\sinh(2x) - \int \frac{1}{2}\sinh(2x),dx

=x2sinh⁡(2x)−14cosh⁡(2x)+C= \frac{x}{2}\sinh(2x) - \frac{1}{4}\cosh(2x) + C

The step that gets skipped here is the second factor of 12\frac{1}{2}: integrating 12sinh⁡(2x)\frac{1}{2}\sinh(2x) needs another division by 22, which is where the 14\frac{1}{4} comes from.

Final answer: x2sinh⁡(2x)−14cosh⁡(2x)+C\frac{x}{2}\sinh(2x) - \frac{1}{4}\cosh(2x) + C

Example 5

Evaluate ∫01dx4−x2\int_{0}^{1} \frac{dx}{4 - x^{2}}.

Here a=2a = 2 and every xx in [0,1][0, 1] satisfies ∣x∣<2\lvert x\rvert < 2, so the tanh⁡−1\tanh^{-1} row applies:

∫01dx4−x2=[12tanh⁡−1x2]01\int_{0}^{1} \frac{dx}{4 - x^{2}} = \left[\frac{1}{2}\tanh^{-1}\frac{x}{2}\right]_{0}^{1}

=12tanh⁡−112−0= \frac{1}{2}\tanh^{-1}\frac{1}{2} - 0

=12⋅12ln⁡1+121−12= \frac{1}{2}\cdot\frac{1}{2}\ln\frac{1 + \frac{1}{2}}{1 - \frac{1}{2}}

=14ln⁡3= \frac{1}{4}\ln 3

≈0.2747\approx 0.2747

Final answer: ln⁡34≈0.2747\frac{\ln 3}{4} \approx 0.2747

Example 6

Evaluate ∫35dxx2−4\int_{3}^{5} \frac{dx}{\sqrt{x^{2} - 4}}.

Here a=2a = 2 and the interval [3,5][3, 5] lies inside x>2x > 2, so the cosh⁡−1\cosh^{-1} row applies:

∫35dxx2−4=[cosh⁡−1x2]35\int_{3}^{5} \frac{dx}{\sqrt{x^{2} - 4}} = \left[\cosh^{-1}\frac{x}{2}\right]_{3}^{5}

=cosh⁡−152−cosh⁡−132= \cosh^{-1}\frac{5}{2} - \cosh^{-1}\frac{3}{2}

=ln⁡5+212−ln⁡3+52= \ln\frac{5 + \sqrt{21}}{2} - \ln\frac{3 + \sqrt{5}}{2}

≈1.5668−0.9624\approx 1.5668 - 0.9624

≈0.6044\approx 0.6044

Final answer: cosh⁡−152−cosh⁡−132≈0.6044\cosh^{-1}\frac{5}{2} - \cosh^{-1}\frac{3}{2} \approx 0.6044

Why Do We Need Hyperbolic Integrals At All?

"Some square-root integrals have no tidy answer without them."

Without the hyperbolic list, ∫dxx2+1\int \frac{dx}{\sqrt{x^{2} + 1}} is still solvable, but only by a trig substitution with tan⁡θ\tan\theta and sec⁡θ\sec\theta followed by a long logarithm simplification. With it, the answer is one symbol: sinh⁡−1x+C\sinh^{-1} x + C.

The hyperbolic list closes three gaps in the ordinary table:

  • Square roots with a plus sign. x2+a2\sqrt{x^{2} + a^{2}} and x2−a2\sqrt{x^{2} - a^{2}} have no inverse-trig antiderivatives; sinh⁡−1\sinh^{-1} and cosh⁡−1\cosh^{-1} fill exactly that space.

  • Integrals that would otherwise need partial fractions every time. ∫dxa2−x2\int \frac{dx}{a^{2} - x^{2}} becomes a single tanh⁡−1\tanh^{-1}, with the logarithm form available when an answer key wants it.

  • Clean definite values. For example, ∫01dxx2+1=sinh⁡−11=ln⁡(1+2)≈0.8814\int_{0}^{1} \frac{dx}{\sqrt{x^{2} + 1}} = \sinh^{-1} 1 = \ln\left(1 + \sqrt{2}\right) \approx 0.8814, and the improper integral ∫0∞sech⁡x,dx\int_{0}^{\infty} \operatorname{sech} x,dx equals exactly π2\frac{\pi}{2}, since arctan⁡(sinh⁡x)\arctan(\sinh x) climbs from 00 to π2\frac{\pi}{2}.

  • Harder improper integrals with named answers. Two Quora threads ask how to evaluate ∫0∞(ln⁡(cosh⁡x)−ln⁡(sinh⁡x))dx\int_{0}^{\infty} \left(\ln(\cosh x) - \ln(\sinh x)\right)dx and ∫0∞sinh⁡xxcosh⁡2x,dx\int_{0}^{\infty} \frac{\sinh x}{x\cosh^2 x},dx. For the first, write ln⁡cosh⁡xsinh⁡x=ln⁡1+e−2x1−e−2x=2∑n odde−2nxn\ln\frac{\cosh x}{\sinh x} = \ln\frac{1 + e^{-2x}}{1 - e^{-2x}} = 2\sum_{n \text{ odd}} \frac{e^{-2nx}}{n} and integrate term by term: each term gives 1n2\frac{1}{n^{2}}, and the sum over odd nn is π28≈1.2337\frac{\pi^{2}}{8} \approx 1.2337. The second equals 4Gπ≈1.1662\frac{4G}{\pi} \approx 1.1662, where G≈0.9160G \approx 0.9160 is Catalan's constant; neither has an elementary antiderivative to plug limits into, which is where the basic list stops.

Where Are Integrals Of Hyperbolic Functions Used In Real Life?

The two most common applications are the length of a hanging cable and the distance an object falls against air resistance.

  • Length of a hanging cable. A cable of uniform weight hangs in the shape y=acosh⁡xay = a\cosh\frac{x}{a}. Its arc length uses 1+sinh⁡2u=cosh⁡2u1 + \sinh^2 u = \cosh^2 u, so the square root in the arc-length formula disappears and the integral is ∫cosh⁡xa,dx\int \cosh\frac{x}{a},dx. For y=10cosh⁡x10y = 10\cosh\frac{x}{10} from x=−15x = -15 to x=15x = 15 (in feet), the length is 20sinh⁡(1.5)≈42.585620\sinh(1.5) \approx 42.5856 feet, the worked problem in OpenStax Calculus Volume 1, section 6.9.

  • Distance fallen with drag. A body falling from rest with drag proportional to v2v^{2} has speed v(t)=gktanh⁡(gk,t)v(t) = \sqrt{\frac{g}{k}}\tanh\left(\sqrt{gk},t\right), where gg is gravitational acceleration and kk is the drag constant per unit mass. Integrating with the tanh⁡\tanh row gives the distance fallen: s(t)=1kln⁡(cosh⁡(gk,t))s(t) = \frac{1}{k}\ln\left(\cosh\left(\sqrt{gk},t\right)\right).

  • Exact values for physics tables. Integrals such as ∫0∞tanh⁡(ax)−tanh⁡(bx)x,dx=ln⁡ab\int_{0}^{\infty} \frac{\tanh(ax) - \tanh(bx)}{x},dx = \ln\frac{a}{b} for a,b>0a, b > 0 appear in NIST's reference list, where hyperbolic forms turn otherwise awkward integrals into closed values.

Where Solutions Go Off The Rails With Hyperbolic Integrals

Most errors on this topic come from carrying a trig habit across, or from using a formula outside its domain.

Mistake 1: Copying The Minus Sign From The Sine Integral

Where it slips in: Any ∫sinh⁡x,dx\int \sinh x,dx or ∫sinh⁡(ax),dx\int \sinh(ax),dx, usually right after a trig integration unit.

Don't do this: Write ∫sinh⁡x,dx=−cosh⁡x+C\int \sinh x,dx = -\cosh x + C because ∫sin⁡x,dx=−cos⁡x+C\int \sin x,dx = -\cos x + C.

The correct way: Write ∫sinh⁡x,dx=cosh⁡x+C\int \sinh x,dx = \cosh x + C, and check by differentiating: ddxcosh⁡x=sinh⁡x\frac{d}{dx}\cosh x = \sinh x, with no sign.

The first instinct on ∫sinh⁡x,dx\int \sinh x,dx is almost always −cosh⁡x-\cosh x, carried over from sine. The memoriser who learned "integral of sine is minus cosine" as a sound rather than as a reversed derivative is the one who makes it, and the one-line derivative check is the habit that catches it.

Mistake 2: Using Tanh Inverse Outside Its Domain

Where it slips in: Integrals like ∫dx1−x2\int \frac{dx}{1 - x^{2}} evaluated on an interval such as [2,3][2, 3].

Don't do this: Write [tanh⁡−1x]23\left[\tanh^{-1} x\right]_{2}^{3}. tanh⁡−12\tanh^{-1} 2 and tanh⁡−13\tanh^{-1} 3 do not exist as real numbers.

The correct way: For ∣x∣>1\lvert x\rvert > 1 use coth⁡−1x\coth^{-1} x, or the logarithm form 12ln⁡x+1x−1\frac{1}{2}\ln\frac{x + 1}{x - 1}. On [2,3][2, 3] the answer is 12ln⁡2−12ln⁡3=12ln⁡23≈−0.2027\frac{1}{2}\ln 2 - \frac{1}{2}\ln 3 = \frac{1}{2}\ln\frac{2}{3} \approx -0.2027, which is negative because 11−x2<0\frac{1}{1 - x^{2}} < 0 there.

Mistake 3: Dropping The Absolute Value In Coth And Csch

Where it slips in: ∫coth⁡x,dx\int \coth x,dx or ∫csch⁡x,dx\int \operatorname{csch} x,dx on an interval of negative xx.

Don't do this: Write ln⁡(sinh⁡x)\ln(\sinh x) for x<0x < 0, where sinh⁡x\sinh x is negative and the logarithm is undefined.

The correct way: Keep ln⁡∣sinh⁡x∣+C\ln\lvert\sinh x\rvert + C and ln⁡∣tanh⁡x2∣+C\ln\left\lvert\tanh\frac{x}{2}\right\rvert + C. The tanh⁡\tanh integral is the only one of the three where dropping the bars is safe, since cosh⁡x≥1\cosh x \geq 1.

The rusher who drops absolute values to save a stroke gets away with it on positive inputs, so the habit survives until the first problem set on negative intervals.

Mistake 4: Forgetting To Divide By The Inner Constant

Where it slips in: ∫cosh⁡(ax),dx\int \cosh(ax),dx, ∫sinh⁡(ax),dx\int \sinh(ax),dx and the xsinh⁡(ax)x\sinh(ax) rows.

Don't do this: Write ∫cosh⁡(5x),dx=sinh⁡(5x)+C\int \cosh(5x),dx = \sinh(5x) + C.

The correct way: Divide by aa: ∫cosh⁡(5x),dx=15sinh⁡(5x)+C\int \cosh(5x),dx = \frac{1}{5}\sinh(5x) + C, since differentiating sinh⁡(5x)\sinh(5x) produces a factor of 55.

Swapping a hyperbolic shape for a more familiar one has a real cost. For centuries the hanging chain was assumed to be a parabola, a claim Galileo made and that was refuted in 1669, as the MacTutor history of the catenary records. For the OpenStax cable above, a parabola through the same lowest point and the same two end points has length about 42.175642.1756 feet against the catenary's 42.585642.5856, so treating the cable as a parabola under-orders it by about 0.410.41 feet.

Practice Problems On The List Of Integrals Of Hyperbolic Functions

Evaluate each integral.

  1. ∫sinh⁡(4x),dx\int \sinh(4x),dx

  2. ∫0ln⁡2cosh⁡x,dx\int_{0}^{\ln 2} \cosh x,dx

  3. ∫xsinh⁡x,dx\int x\sinh x,dx

  4. ∫dxx2+4\int \frac{dx}{\sqrt{x^{2} + 4}}

  5. ∫cosh⁡2xsinh⁡x,dx\int \cosh^2 x\sinh x,dx

  6. ∫sech⁡xtanh⁡x,dx\int \operatorname{sech} x\tanh x,dx

Answer to Question 1: 14cosh⁡(4x)+C\frac{1}{4}\cosh(4x) + C

Answer to Question 2: sinh⁡(ln⁡2)=34\sinh(\ln 2) = \frac{3}{4}

Answer to Question 3: xcosh⁡x−sinh⁡x+Cx\cosh x - \sinh x + C

Answer to Question 4: sinh⁡−1x2+C\sinh^{-1}\frac{x}{2} + C, or ln⁡(x+x2+4)+C\ln\left(x + \sqrt{x^{2} + 4}\right) + C

Answer to Question 5: cosh⁡3x3+C\frac{\cosh^3 x}{3} + C

Answer to Question 6: −sech⁡x+C-\operatorname{sech} x + C

What To Remember About Integrals Of Hyperbolic Functions

  • The list of integrals of hyperbolic functions starts with ∫sinh⁡x,dx=cosh⁡x+C\int \sinh x,dx = \cosh x + C and ∫cosh⁡x,dx=sinh⁡x+C\int \cosh x,dx = \sinh x + C, with no minus sign.

  • Tanh and coth integrate to logarithms of cosh and sinh, and only the tanh answer can drop its absolute value.

  • Sech has several correct antiderivatives, and any two of them differ by a constant.

  • Square roots of x2+a2x^{2} + a^{2} and x2−a2x^{2} - a^{2} integrate to inverse hyperbolic functions, each valid only on its stated domain.

  • Differentiating the answer back is the fastest check for every row in the list.

Your Next Move

Work through practice problems 1 to 6 before checking the answers; if problem 4 trips you up, return to the section on integrals that give inverse hyperbolic functions and redo the x=asinh⁡tx = a\sinh t substitution with a=2a = 2. Book a free Bhanzu demo class:

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Frequently Asked Questions

On a calculator, there are options for sinh, cosh and tanh. What does the h represent, and when do we use those functions?
The h stands for hyperbolic. Those keys compute sinh⁡x=ex−e−x2\sinh x = \frac{e^{x} - e^{-x}}{2}, cosh⁡x\cosh x and tanh⁡x\tanh x, which you need whenever an answer from the list of integrals of hyperbolic functions has to be turned into a decimal, as in Examples 5 and 6 above.
The hyperbolic functions cosh and sinh can be implemented with the natural exponential function. Can you integrate them that way?
Yes, and it gives a fallback for any row you forget. Rewrite the integrand in exe^{x} and e−xe^{-x}, integrate the exponentials, then convert back. For instance, ∫cosh⁡x,dx=∫ex+e−x2,dx=ex−e−x2+C=sinh⁡x+C\int \cosh x,dx = \int \frac{e^{x} + e^{-x}}{2},dx = \frac{e^{x} - e^{-x}}{2} + C = \sinh x + C. The csch derivation above uses the same idea with u=exu = e^{x}.
What is the process for integrating sinh x cosh x?
Pick one factor as the derivative of the other. With u=sinh⁡xu = \sinh x, du=cosh⁡x,dxdu = \cosh x,dx and the integral is sinh⁡2x2+C\frac{\sinh^2 x}{2} + C. With u=cosh⁡xu = \cosh x you get cosh⁡2x2+C\frac{\cosh^2 x}{2} + C, and with sinh⁡xcosh⁡x=12sinh⁡2x\sinh x\cosh x = \frac{1}{2}\sinh 2x you get cosh⁡2x4+C\frac{\cosh 2x}{4} + C. All three are right, because cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1 makes them differ only by constants.
How do you calculate the integral of cosh x / (2 + 3 sinh x)?
Let u=2+3sinh⁡xu = 2 + 3\sinh x, so du=3cosh⁡x,dxdu = 3\cosh x,dx. The integral becomes 13∫duu=13ln⁡∣2+3sinh⁡x∣+C\frac{1}{3}\int \frac{du}{u} = \frac{1}{3}\ln\lvert 2 + 3\sinh x\rvert + C, valid wherever sinh⁡x≠−23\sinh x \neq -\frac{2}{3}.
How do you use the list of integrals of hyperbolic functions to evaluate the integral of sinh³x cosh x?
Substitute u=sinh⁡xu = \sinh x, so du=cosh⁡x,dxdu = \cosh x,dx and the integral becomes ∫u3,du=u44+C=sinh⁡4x4+C\int u^{3},du = \frac{u^{4}}{4} + C = \frac{\sinh^4 x}{4} + C.
Using the list of integrals of hyperbolic functions, how do you evaluate the definite integral of (sinh x + cosh x) from -6 to 6?
Use symmetry. sinh⁡x\sinh x is an odd function, so its integral over [−6,6][-6, 6] is 00; cosh⁡x\cosh x is even, so its integral is 2sinh⁡62\sinh 6. The total is 2sinh⁡6=e6−e−6≈403.42632\sinh 6 = e^{6} - e^{-6} \approx 403.4263, which you can confirm by noticing sinh⁡x+cosh⁡x=ex\sinh x + \cosh x = e^{x}.
How do you integrate 1 divided by cosh x sinh x?
Divide top and bottom by cosh⁡2x\cosh^2 x: 1sinh⁡xcosh⁡x=sech⁡2xtanh⁡x\frac{1}{\sinh x\cosh x} = \frac{\operatorname{sech}^2 x}{\tanh x}. With u=tanh⁡xu = \tanh x, du=sech⁡2x,dxdu = \operatorname{sech}^2 x,dx, so the integral is ∫duu=ln⁡∣tanh⁡x∣+C\int \frac{du}{u} = \ln\lvert\tanh x\rvert + C for x≠0x \neq 0. It is an elementary integral, even though some forum answers call it otherwise; differentiating ln⁡∣tanh⁡x∣\ln\lvert\tanh x\rvert gives back 1sinh⁡xcosh⁡x\frac{1}{\sinh x\cosh x}.
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