Skip to main content

Hyperbolic Functions (Extended)

Hyperbolic Functions (Extended Treatment)

This document provides a rigorous treatment of hyperbolic functions, their identities, inverses, and calculus.

Hyperbolic functions are analogues of trigonometric functions defined using exponentials

rather than circles. They arise naturally in many areas including differential equations, special relativity, and catenary curves. :::


1. Definitions

1.1 The three fundamental hyperbolic functions

sinhx=exex2\sinh x = \frac{e^x - e^{-x}}{2}

coshx=ex+ex2\cosh x = \frac{e^x + e^{-x}}{2}

tanhx=LBsinhxRB◆◆LBcoshxRB=exexex+ex\tanh x = \frac◆LB◆\sinh x◆RB◆◆LB◆\cosh x◆RB◆ = \frac{e^x - e^{-x}}{e^x + e^{-x}}

1.2 Reciprocal functions

cosechx=LB1RB◆◆LBsinhxRB=2exex,x0\mathrm{cosech}\,x = \frac◆LB◆1◆RB◆◆LB◆\sinh x◆RB◆ = \frac{2}{e^x - e^{-x}}, \quad x \neq 0

sechx=LB1RB◆◆LBcoshxRB=2ex+ex\mathrm{sech}\,x = \frac◆LB◆1◆RB◆◆LB◆\cosh x◆RB◆ = \frac{2}{e^x + e^{-x}}

cothx=LB1RB◆◆LBtanhxRB=ex+exexex,x0\coth x = \frac◆LB◆1◆RB◆◆LB◆\tanh x◆RB◆ = \frac{e^x + e^{-x}}{e^x - e^{-x}}, \quad x \neq 0

1.3 Basic properties

  • sinh0=0\sinh 0 = 0, cosh0=1\cosh 0 = 1, tanh0=0\tanh 0 = 0.
  • sinhx\sinh x is odd: sinh(x)=sinhx\sinh(-x) = -\sinh x.
  • coshx\cosh x is even: cosh(x)=coshx\cosh(-x) = \cosh x.
  • tanhx\tanh x is odd.
  • As x+x \to +\infty: sinhx+\sinh x \to +\infty, coshx+\cosh x \to +\infty, tanhx1\tanh x \to 1.
  • As xx \to -\infty: sinhx\sinh x \to -\infty, coshx+\cosh x \to +\infty, tanhx1\tanh x \to -1.

1.4 Connection with Euler's formula

coshx=cos(ix),sinhx=isin(ix)\cosh x = \cos(ix), \qquad \sinh x = -i\sin(ix)

Proof. cos(ix)=ei(ix)+ei(ix)2=ex+ex2=coshx\cos(ix) = \dfrac{e^{i(ix)} + e^{-i(ix)}}{2} = \dfrac{e^{-x} + e^{x}}{2} = \cosh x.

isin(ix)=iei(ix)ei(ix)2i=exex2=exex2=sinhx-i\sin(ix) = -i \cdot \dfrac{e^{i(ix)} - e^{-i(ix)}}{2i} = \dfrac{e^{-x} - e^{x}}{-2} = \dfrac{e^x - e^{-x}}{2} = \sinh x. \blacksquare

1.5 Graphs

  • sinhx\sinh x: passes through the origin, increasing, resembles y=x/2y = x/2 near the origin and y=ex/2y = e^x/2 for large positive xx.
  • coshx\cosh x: minimum at (0,1)(0, 1), symmetric about the yy-axis, resembles y=1+x2/2y = 1 + x^2/2 near the origin and y=ex/2y = e^x/2 for large positive xx.
  • tanhx\tanh x: S-shaped curve with horizontal asymptotes at y=±1y = \pm 1, passing through the origin with gradient 1.

2. Hyperbolic Identities

2.1 Fundamental identity

cosh2xsinh2x=1\boxed{\cosh^2 x - \sinh^2 x = 1}

Proof.

cosh2xsinh2x=(ex+ex)24(exex)24\cosh^2 x - \sinh^2 x = \frac{(e^x + e^{-x})^2}{4} - \frac{(e^x - e^{-x})^2}{4}

=e2x+2+e2x(e2x2+e2x)4=44=1= \frac{e^{2x} + 2 + e^{-2x} - (e^{2x} - 2 + e^{-2x})}{4} = \frac{4}{4} = 1 \quad \blacksquare

2.2 Identity for tanh\tanh

1tanh2x=sech2x\boxed{1 - \tanh^2 x = \mathrm{sech}^2\,x}

Proof. Divide the fundamental identity by cosh2x\cosh^2 x:

1tanh2x=LB1RB◆◆LBcosh2xRB=sech2x1 - \tanh^2 x = \frac◆LB◆1◆RB◆◆LB◆\cosh^2 x◆RB◆ = \mathrm{sech}^2\,x \quad \blacksquare

2.3 Osborne's rule

Every trigonometric identity has a corresponding hyperbolic identity, obtained by:

  • Replacing cos\cos with cosh\cosh.
  • Replacing sin\sin with sinh\sinh.
  • Negating every product (or power of 2 or more) of sinh\sinh.

Example: cos2x+sin2x=1\cos^2 x + \sin^2 x = 1 becomes cosh2xsinh2x=1\cosh^2 x - \sinh^2 x = 1 (the sinh2\sinh^2 term is negated).

Example: sin2x=2sinxcosx\sin 2x = 2\sin x\cos x becomes sinh2x=2sinhxcoshx\sinh 2x = 2\sinh x\cosh x (the product sinhxcoshx\sinh x \cosh x is negated since it contains sinh\sinh, but sinh2x\sinh 2x on the left is not a product, so the overall sign changes on both sides cancel).

2.4 Double angle formulas

sinh2x=2sinhxcoshx\sinh 2x = 2\sinh x\cosh x

cosh2x=cosh2x+sinh2x=2cosh2x1=1+2sinh2x\cosh 2x = \cosh^2 x + \sinh^2 x = 2\cosh^2 x - 1 = 1 + 2\sinh^2 x

Proof of cosh2x=2cosh2x1\cosh 2x = 2\cosh^2 x - 1:

cosh2x=e2x+e2x2=(ex+ex)222=LB4cosh2x2RB◆◆LB2RB=2cosh2x1\cosh 2x = \frac{e^{2x} + e^{-2x}}{2} = \frac{(e^x + e^{-x})^2 - 2}{2} = \frac◆LB◆4\cosh^2 x - 2◆RB◆◆LB◆2◆RB◆ = 2\cosh^2 x - 1 \quad \blacksquare

2.5 Addition formulas

sinh(A±B)=sinhAcoshB±coshAsinhB\sinh(A \pm B) = \sinh A\cosh B \pm \cosh A\sinh B

cosh(A±B)=coshAcoshB±sinhAsinhB\cosh(A \pm B) = \cosh A\cosh B \pm \sinh A\sinh B

Proof of the addition formula for sinh\sinh:

sinh(A+B)=eA+Be(A+B)2=eAeBeAeB2\sinh(A + B) = \frac{e^{A+B} - e^{-(A+B)}}{2} = \frac{e^A e^B - e^{-A}e^{-B}}{2}

=(eAeA)(eB+eB)+(eA+eA)(eBeB)4= \frac{(e^A - e^{-A})(e^B + e^{-B}) + (e^A + e^{-A})(e^B - e^{-B})}{4}

=sinhAcoshB+coshAsinhB= \sinh A\cosh B + \cosh A\sinh B \quad \blacksquare

2.6 Worked example

Problem. Given sinhx=3\sinh x = 3, find coshx\cosh x and tanhx\tanh x without finding xx.

From cosh2xsinh2x=1\cosh^2 x - \sinh^2 x = 1:

cosh2x=1+9=10    coshx=10\cosh^2 x = 1 + 9 = 10 \implies \cosh x = \sqrt{10}

(We take the positive root since coshx1\cosh x \geq 1 for all xx.)

tanhx=LBsinhxRB◆◆LBcoshxRB=LB3RB◆◆LB10RB=LB310RB◆◆LB10RB\tanh x = \frac◆LB◆\sinh x◆RB◆◆LB◆\cosh x◆RB◆ = \frac◆LB◆3◆RB◆◆LB◆\sqrt{10}◆RB◆ = \frac◆LB◆3\sqrt{10}◆RB◆◆LB◆10◆RB◆


3. Inverse Hyperbolic Functions

3.1 Definitions in logarithmic form

arsinhx=ln ⁣(x+x2+1),xR\operatorname{arsinh}\,x = \ln\!\left(x + \sqrt{x^2 + 1}\right), \quad x \in \mathbb{R}

arcoshx=ln ⁣(x+x21),x1\operatorname{arcosh}\,x = \ln\!\left(x + \sqrt{x^2 - 1}\right), \quad x \geq 1

artanhx=12ln ⁣(1+x1x),1<x<1\operatorname{artanh}\,x = \frac{1}{2}\ln\!\left(\frac{1 + x}{1 - x}\right), \quad -1 \lt x \lt 1

3.2 Derivation of arsinhx=ln(x+x2+1)\operatorname{arsinh}\,x = \ln(x + \sqrt{x^2 + 1})

Let y=arsinhxy = \operatorname{arsinh}\,x, so x=sinhy=eyey2x = \sinh y = \dfrac{e^y - e^{-y}}{2}.

2x=eyey    e2y2xey1=02x = e^y - e^{-y} \implies e^{2y} - 2xe^y - 1 = 0

This is a quadratic in eye^y:

ey=LB2x±4x2+4RB◆◆LB2RB=x±x2+1e^y = \frac◆LB◆2x \pm \sqrt{4x^2 + 4}◆RB◆◆LB◆2◆RB◆ = x \pm \sqrt{x^2 + 1}

Since ey>0e^y \gt 0 and x2+1>x\sqrt{x^2 + 1} \gt |x|, we take the positive root:

ey=x+x2+1    y=ln ⁣(x+x2+1)e^y = x + \sqrt{x^2 + 1} \implies y = \ln\!\left(x + \sqrt{x^2 + 1}\right) \quad \blacksquare

3.3 Derivation of arcoshx=ln(x+x21)\operatorname{arcosh}\,x = \ln(x + \sqrt{x^2 - 1})

Let y=arcoshxy = \operatorname{arcosh}\,x, so x=coshy=ey+ey2x = \cosh y = \dfrac{e^y + e^{-y}}{2}.

2x=ey+ey    e2y2xey+1=02x = e^y + e^{-y} \implies e^{2y} - 2xe^y + 1 = 0

ey=LB2x±4x24RB◆◆LB2RB=x±x21e^y = \frac◆LB◆2x \pm \sqrt{4x^2 - 4}◆RB◆◆LB◆2◆RB◆ = x \pm \sqrt{x^2 - 1}

Since ey1e^y \geq 1 and x1x \geq 1, we need ey1e^y \geq 1. Both roots are positive when x1x \geq 1. The convention is to take ey=x+x21e^y = x + \sqrt{x^2 - 1} (which gives y0y \geq 0):

y=ln ⁣(x+x21)y = \ln\!\left(x + \sqrt{x^2 - 1}\right) \quad \blacksquare

3.4 Derivation of artanhx\operatorname{artanh}\,x

Let y=artanhxy = \operatorname{artanh}\,x, so x=tanhyx = \tanh y.

x=eyeyey+ey=e2y1e2y+1x = \frac{e^y - e^{-y}}{e^y + e^{-y}} = \frac{e^{2y} - 1}{e^{2y} + 1}

x(e2y+1)=e2y1    e2y(1x)=1+xx(e^{2y} + 1) = e^{2y} - 1 \implies e^{2y}(1 - x) = 1 + x

e2y=1+x1x    2y=ln ⁣(1+x1x)e^{2y} = \frac{1 + x}{1 - x} \implies 2y = \ln\!\left(\frac{1 + x}{1 - x}\right)

y=12ln ⁣(1+x1x)y = \frac{1}{2}\ln\!\left(\frac{1 + x}{1 - x}\right) \quad \blacksquare

3.5 Worked example

Problem. Evaluate arsinh2\operatorname{arsinh}\,2 and artanh13\operatorname{artanh}\,\dfrac{1}{3} in exact logarithmic form.

arsinh2=ln(2+5)\operatorname{arsinh}\,2 = \ln(2 + \sqrt{5})

artanh13=12ln ⁣(4/32/3)=12ln2\operatorname{artanh}\,\frac{1}{3} = \frac{1}{2}\ln\!\left(\frac{4/3}{2/3}\right) = \frac{1}{2}\ln 2

3.6 Domains and ranges

FunctionDomainRange
arsinhx\operatorname{arsinh}\,xR\mathbb{R}R\mathbb{R}
arcoshx\operatorname{arcosh}\,xx1x \geq 1y0y \geq 0
artanhx\operatorname{artanh}\,x1<x<1-1 \lt x \lt 1R\mathbb{R}

4. Calculus of Hyperbolic Functions

4.1 Differentiation

ddx(sinhx)=coshx\frac{d}{dx}(\sinh x) = \cosh x

ddx(coshx)=sinhx\frac{d}{dx}(\cosh x) = \sinh x

ddx(tanhx)=sech2x\frac{d}{dx}(\tanh x) = \mathrm{sech}^2\,x

Proof of ddxsinhx=coshx\dfrac{d}{dx}\sinh x = \cosh x:

ddx ⁣(exex2)=ex+ex2=coshx\frac{d}{dx}\!\left(\frac{e^x - e^{-x}}{2}\right) = \frac{e^x + e^{-x}}{2} = \cosh x \quad \blacksquare

4.2 Differentiation of inverse hyperbolic functions

ddx(arsinhx)=LB1RB◆◆LBx2+1RB\frac{d}{dx}(\operatorname{arsinh}\,x) = \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 + 1}◆RB◆

ddx(arcoshx)=LB1RB◆◆LBx21RB,x>1\frac{d}{dx}(\operatorname{arcosh}\,x) = \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆, \quad x \gt 1

ddx(artanhx)=11x2,x<1\frac{d}{dx}(\operatorname{artanh}\,x) = \frac{1}{1 - x^2}, \quad |x| \lt 1

Proof for arsinhx\operatorname{arsinh}\,x. Let y=arsinhxy = \operatorname{arsinh}\,x, so x=sinhyx = \sinh y.

dydx=LB1RB◆◆LBdxdyRB=LB1RB◆◆LBcoshyRB=LB1RB◆◆LBLB1+sinh2yRB◆◆RB=LB1RB◆◆LB1+x2RB\frac{dy}{dx} = \frac◆LB◆1◆RB◆◆LB◆\dfrac{dx}{dy}◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆\cosh y◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆\sqrt◆LB◆1 + \sinh^2 y◆RB◆◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆\sqrt{1 + x^2}◆RB◆ \quad \blacksquare

Proof for artanhx\operatorname{artanh}\,x. Let y=artanhxy = \operatorname{artanh}\,x, so x=tanhyx = \tanh y.

dydx=LB1RB◆◆LBsech2yRB=LB1RB◆◆LB1tanh2yRB=11x2\frac{dy}{dx} = \frac◆LB◆1◆RB◆◆LB◆\mathrm{sech}^2\,y◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆1 - \tanh^2 y◆RB◆ = \frac{1}{1 - x^2} \quad \blacksquare

4.3 Integration

The differentiation results give standard integrals:

coshxdx=sinhx+C\int \cosh x\,dx = \sinh x + C

sinhxdx=coshx+C\int \sinh x\,dx = \cosh x + C

sech2xdx=tanhx+C\int \mathrm{sech}^2\,x\,dx = \tanh x + C

4.4 Integrals leading to inverse hyperbolic functions

LB1RB◆◆LBx2+a2RBdx=arsinh ⁣(xa)+C\int \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 + a^2}◆RB◆\,dx = \operatorname{arsinh}\!\left(\frac{x}{a}\right) + C

LB1RB◆◆LBx2a2RBdx=arcosh ⁣(xa)+C,x>a\int \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - a^2}◆RB◆\,dx = \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C, \quad x \gt a

1a2x2dx=1aartanh ⁣(xa)+C,x<a\int \frac{1}{a^2 - x^2}\,dx = \frac{1}{a}\operatorname{artanh}\!\left(\frac{x}{a}\right) + C, \quad |x| \lt a

Proof of the first formula. Let u=x/au = x/a:

LBdxRB◆◆LBx2+a2RB=LBaduRB◆◆LBau2+1RB=arsinhu+C=arsinh ⁣(xa)+C\int \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 + a^2}◆RB◆ = \int \frac◆LB◆a\,du◆RB◆◆LB◆a\sqrt{u^2 + 1}◆RB◆ = \operatorname{arsinh}\,u + C = \operatorname{arsinh}\!\left(\frac{x}{a}\right) + C \quad \blacksquare

4.5 Worked example: differentiation

Problem. Differentiate f(x)=sinh(3x2)f(x) = \sinh(3x^2).

f(x)=6xcosh(3x2)f'(x) = 6x\cosh(3x^2)

4.6 Worked example: integration

Problem. Evaluate LB1RB◆◆LB4x2+9RBdx\displaystyle\int \frac◆LB◆1◆RB◆◆LB◆\sqrt{4x^2 + 9}◆RB◆\,dx.

LBdxRB◆◆LB4x2+9RB=12LBd(2x)RB◆◆LB(2x)2+9RB=12arsinh ⁣(2x3)+C\int \frac◆LB◆dx◆RB◆◆LB◆\sqrt{4x^2 + 9}◆RB◆ = \frac{1}{2}\int \frac◆LB◆d(2x)◆RB◆◆LB◆\sqrt{(2x)^2 + 9}◆RB◆ = \frac{1}{2}\operatorname{arsinh}\!\left(\frac{2x}{3}\right) + C

4.7 Worked example: definite integral

Problem. Evaluate 01LBdxRB◆◆LBx2+1RB\displaystyle\int_0^1 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 + 1}◆RB◆.

=[arsinhx]01=arsinh1arsinh0=ln(1+2)0=ln(1+2)= \left[\operatorname{arsinh}\,x\right]_0^1 = \operatorname{arsinh}\,1 - \operatorname{arsinh}\,0 = \ln(1 + \sqrt{2}) - 0 = \ln(1 + \sqrt{2})

4.8 Worked example: integration by substitution with hyperbolic functions

Problem. Evaluate x2+4dx\displaystyle\int \sqrt{x^2 + 4}\,dx.

Use the substitution x=2sinhux = 2\sinh u, dx=2coshududx = 2\cosh u\,du:

LB4sinh2u+4RB2coshudu=2coshu2coshudu=4cosh2udu\int \sqrt◆LB◆4\sinh^2 u + 4◆RB◆\cdot 2\cosh u\,du = \int 2\cosh u \cdot 2\cosh u\,du = 4\int \cosh^2 u\,du

Using cosh2u=LB1+cosh2uRB◆◆LB2RB\cosh^2 u = \dfrac◆LB◆1 + \cosh 2u◆RB◆◆LB◆2◆RB◆:

=4LB1+cosh2uRB◆◆LB2RBdu=2u+sinh2u+C= 4\int \frac◆LB◆1 + \cosh 2u◆RB◆◆LB◆2◆RB◆\,du = 2u + \sinh 2u + C

=2u+2sinhucoshu+C= 2u + 2\sinh u\cosh u + C

Since x=2sinhux = 2\sinh u: sinhu=x2\sinh u = \dfrac{x}{2}, coshu=LB1+x24RB=LBx2+4RB◆◆LB2RB\cosh u = \sqrt◆LB◆1 + \dfrac{x^2}{4}◆RB◆ = \dfrac◆LB◆\sqrt{x^2 + 4}◆RB◆◆LB◆2◆RB◆, u=arsinh ⁣(x2)u = \operatorname{arsinh}\!\left(\dfrac{x}{2}\right).

=2arsinh ⁣(x2)+LBxx2+4RB◆◆LB2RB+C= 2\operatorname{arsinh}\!\left(\frac{x}{2}\right) + \frac◆LB◆x\sqrt{x^2 + 4}◆RB◆◆LB◆2◆RB◆ + C

Common Pitfall The substitution x=asinhux = a\sinh u is a powerful technique for integrals

involving x2+a2\sqrt{x^2 + a^2}. Similarly, x=acoshux = a\cosh u handles x2a2\sqrt{x^2 - a^2} and x=atanhux = a\tanh u handles expressions with a2x2a^2 - x^2. The choice of substitution mirrors the trigonometric substitutions but is often simpler algebraically. :::


5. Practice Problems

Problem 1

Solve the equation 4sinhx3coshx=04\sinh x - 3\cosh x = 0.

Solution

4sinhx=3coshx    tanhx=344\sinh x = 3\cosh x \implies \tanh x = \dfrac{3}{4}.

x=artanh ⁣(34)=12ln ⁣(1+3/413/4)=12ln7x = \operatorname{artanh}\!\left(\dfrac{3}{4}\right) = \dfrac{1}{2}\ln\!\left(\dfrac{1 + 3/4}{1 - 3/4}\right) = \dfrac{1}{2}\ln 7.

Problem 2

Prove that sinh3x=3sinhx+4sinh3x\sinh 3x = 3\sinh x + 4\sinh^3 x.

Solution

sinh3x=sinh(2x+x)=sinh2xcoshx+cosh2xsinhx\sinh 3x = \sinh(2x + x) = \sinh 2x\cosh x + \cosh 2x\sinh x

=2sinhxcosh2x+(1+2sinh2x)sinhx= 2\sinh x\cosh^2 x + (1 + 2\sinh^2 x)\sinh x

=2sinhx(1+sinh2x)+sinhx+2sinh3x= 2\sinh x(1 + \sinh^2 x) + \sinh x + 2\sinh^3 x

=2sinhx+2sinh3x+sinhx+2sinh3x=3sinhx+4sinh3x= 2\sinh x + 2\sinh^3 x + \sinh x + 2\sinh^3 x = 3\sinh x + 4\sinh^3 x.

Problem 3

Evaluate 02LBdxRB◆◆LBx2+16RB\displaystyle\int_0^2 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 + 16}◆RB◆.

Solution

=[arsinh ⁣(x4)]02=arsinh ⁣(12)=ln ⁣(12+LB54RB)=ln ⁣(LB1+5RB◆◆LB2RB)= \left[\operatorname{arsinh}\!\left(\dfrac{x}{4}\right)\right]_0^2 = \operatorname{arsinh}\!\left(\dfrac{1}{2}\right) = \ln\!\left(\dfrac{1}{2} + \sqrt◆LB◆\dfrac{5}{4}◆RB◆\right) = \ln\!\left(\dfrac◆LB◆1 + \sqrt{5}◆RB◆◆LB◆2◆RB◆\right).

Problem 4

Differentiate f(x)=xarcoshxf(x) = x\,\operatorname{arcosh}\,x for x>1x \gt 1.

Solution

Using the product rule:

f(x)=arcoshx+xLB1RB◆◆LBx21RB=arcoshx+LBxRB◆◆LBx21RBf'(x) = \operatorname{arcosh}\,x + x \cdot \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ = \operatorname{arcosh}\,x + \dfrac◆LB◆x◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆.


6. Further Proofs and Key Results

6.1 Proof: LB1RB◆◆LBx2a2RBdx=arcosh ⁣(xa)+C\int \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - a^2}◆RB◆\,dx = \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C

Proof. Let u=x/au = x/a, so dx=adudx = a\,du:

LBdxRB◆◆LBx2a2RB=LBaduRB◆◆LBau21RB=LBduRB◆◆LBu21RB\int \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - a^2}◆RB◆ = \int \frac◆LB◆a\,du◆RB◆◆LB◆a\sqrt{u^2 - 1}◆RB◆ = \int \frac◆LB◆du◆RB◆◆LB◆\sqrt{u^2 - 1}◆RB◆

Now let u=coshtu = \cosh t, so du=sinhtdtdu = \sinh t\,dt:

=LBsinhtdtRB◆◆LBLBcosh2t1RB◆◆RB=LBsinhtdtRB◆◆LBsinhtRB=1dt=t+C=arcoshu+C= \int \frac◆LB◆\sinh t\,dt◆RB◆◆LB◆\sqrt◆LB◆\cosh^2 t - 1◆RB◆◆RB◆ = \int \frac◆LB◆\sinh t\,dt◆RB◆◆LB◆\sinh t◆RB◆ = \int 1\,dt = t + C = \operatorname{arcosh}\,u + C

=arcosh ⁣(xa)+C= \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C \quad \blacksquare

6.2 Proof: 1a2x2dx=1aartanh ⁣(xa)+C\int \frac{1}{a^2 - x^2}\,dx = \frac{1}{a}\operatorname{artanh}\!\left(\frac{x}{a}\right) + C

Proof. Let u=x/au = x/a, so dx=adudx = a\,du:

dxa2x2=1adu1u2=1aartanhu+C=1aartanh ⁣(xa)+C\int \frac{dx}{a^2 - x^2} = \frac{1}{a}\int \frac{du}{1 - u^2} = \frac{1}{a}\operatorname{artanh}\,u + C = \frac{1}{a}\operatorname{artanh}\!\left(\frac{x}{a}\right) + C \quad \blacksquare

6.3 Proof: the catenary equation

Theorem. A uniform chain hanging under gravity takes the shape y=acosh ⁣(xa)+cy = a\cosh\!\left(\dfrac{x}{a}\right) + c.

Proof (sketch). Consider a small element of the chain between horizontal positions xx and x+δxx + \delta x. Let the tension at position xx be TT, making angle θ\theta with the horizontal.

Horizontal equilibrium: Tcosθ=T0T\cos\theta = T_0 (constant).

Vertical equilibrium: ddx(Tsinθ)=w\dfrac{d}{dx}(T\sin\theta) = w where ww is the weight per unit length.

Since T=T0secθT = T_0\sec\theta and Tsinθ=T0tanθT\sin\theta = T_0\tan\theta:

ddx(T0tanθ)=w    T0sec2θLBdθRB◆◆LBdxRB=w\frac{d}{dx}(T_0\tan\theta) = w \implies T_0\sec^2\theta\,\frac◆LB◆d\theta◆RB◆◆LB◆dx◆RB◆ = w

Let y=tanθy' = \tan\theta, so dydx=sec2θLBdθRB◆◆LBdxRB=wT0\dfrac{dy'}{dx} = \sec^2\theta\,\dfrac◆LB◆d\theta◆RB◆◆LB◆dx◆RB◆ = \dfrac{w}{T_0}.

Integrating: y=wT0x+C1y' = \dfrac{w}{T_0}\,x + C_1. Taking C1=0C_1 = 0 by symmetry:

y=xawhere a=T0wy' = \frac{x}{a} \quad \text{where } a = \frac{T_0}{w}

Integrating again: y=acosh ⁣(xa)+Cy = a\cosh\!\left(\dfrac{x}{a}\right) + C. \blacksquare


7. Common Pitfalls

Common Pitfall
  1. Sign in the fundamental identity: Unlike cos2x+sin2x=1\cos^2 x + \sin^2 x = 1, the hyperbolic identity is cosh2xsinh2x=1\cosh^2 x - \sinh^2 x = 1. The minus sign is crucial and is the source of many errors.
  2. Domain of arcosh\operatorname{arcosh}: The domain is x1x \geq 1 (not x>0x > 0). Attempting to evaluate arcosh(0.5)\operatorname{arcosh}(0.5) is undefined.
  3. coshx1\cosh x \geq 1 always: When solving cosh2x=k\cosh^2 x = k and taking the square root, always take the positive root coshx=+k\cosh x = +\sqrt{k} since coshx1>0\cosh x \geq 1 > 0 for all real xx.
  4. Integration: artanh vs ln: When x>a|x| > a in dxa2x2\displaystyle\int \frac{dx}{a^2 - x^2}, the result involves arcoth\operatorname{arcoth} (or an alternative logarithmic form), not artanh\operatorname{artanh}. Check the domain of the integrand carefully. :::

8. Additional Exam-Style Questions

Question 5

(a) Solve the equation coshx=2.5\cosh x = 2.5, giving your answer in exact logarithmic form.

(b) Hence solve cosh2x=2.5\cosh 2x = 2.5.

Solution

(a) coshx=ex+ex2=2.5\cosh x = \dfrac{e^x + e^{-x}}{2} = 2.5

ex+ex=5    e2x5ex+1=0e^x + e^{-x} = 5 \implies e^{2x} - 5e^x + 1 = 0

ex=LB5±254RB◆◆LB2RB=LB5±21RB◆◆LB2RBe^x = \dfrac◆LB◆5 \pm \sqrt{25 - 4}◆RB◆◆LB◆2◆RB◆ = \dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆

x=ln ⁣(LB5±21RB◆◆LB2RB)x = \ln\!\left(\dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆\right)

Since cosh\cosh is even, both ±\pm give valid solutions (one positive, one negative).

(b) cosh2x=2.5    2x=ln ⁣(LB5±21RB◆◆LB2RB)\cosh 2x = 2.5 \implies 2x = \ln\!\left(\dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆\right)

x=12ln ⁣(LB5±21RB◆◆LB2RB)x = \dfrac{1}{2}\ln\!\left(\dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆\right)

Alternatively, using cosh2x=2cosh2x1=2.5    cosh2x=1.75\cosh 2x = 2\cosh^2 x - 1 = 2.5 \implies \cosh^2 x = 1.75, which gives the same result.

Question 6

(a) Prove that ddx(arcoshx)=LB1RB◆◆LBx21RB\dfrac{d}{dx}(\operatorname{arcosh}\,x) = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ for x>1x > 1.

(b) Evaluate 23LBdxRB◆◆LBx21RB\displaystyle\int_2^3 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ in exact form.

Solution

(a) Let y=arcoshxy = \operatorname{arcosh}\,x, so x=coshyx = \cosh y.

dxdy=sinhy\dfrac{dx}{dy} = \sinh y, so dydx=LB1RB◆◆LBsinhyRB\dfrac{dy}{dx} = \dfrac◆LB◆1◆RB◆◆LB◆\sinh y◆RB◆.

Since cosh2ysinh2y=1\cosh^2 y - \sinh^2 y = 1: sinhy=LBcosh2y1RB=x21\sinh y = \sqrt◆LB◆\cosh^2 y - 1◆RB◆ = \sqrt{x^2 - 1}.

dydx=LB1RB◆◆LBx21RB\dfrac{dy}{dx} = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ \quad \blacksquare

(b) 23LBdxRB◆◆LBx21RB=[arcoshx]23\displaystyle\int_2^3 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ = \bigl[\operatorname{arcosh}\,x\bigr]_2^3

=ln(3+8)ln(2+3)=ln(3+22)ln(2+3)= \ln(3 + \sqrt{8}) - \ln(2 + \sqrt{3}) = \ln(3 + 2\sqrt{2}) - \ln(2 + \sqrt{3})

=ln ⁣(LB3+22RB◆◆LB2+3RB)= \ln\!\left(\dfrac◆LB◆3 + 2\sqrt{2}◆RB◆◆LB◆2 + \sqrt{3}◆RB◆\right).

Question 7

A curve CC has equation y=sinh1(2x1)y = \sinh^{-1}(2x - 1).

(a) Find dydx\dfrac{dy}{dx}.

(b) Find the equation of the tangent to CC at the point where x=1x = 1.

Solution

(a) y=arsinh(2x1)y = \operatorname{arsinh}(2x - 1).

dydx=LB2RB◆◆LB(2x1)2+1RB=LB2RB◆◆LB4x24x+2RB\dfrac{dy}{dx} = \dfrac◆LB◆2◆RB◆◆LB◆\sqrt{(2x - 1)^2 + 1}◆RB◆ = \dfrac◆LB◆2◆RB◆◆LB◆\sqrt{4x^2 - 4x + 2}◆RB◆.

(b) At x=1x = 1: y=arsinh(1)=ln(1+2)y = \operatorname{arsinh}(1) = \ln(1 + \sqrt{2}).

dydxx=1=LB2RB◆◆LB44+2RB=LB2RB◆◆LB2RB=2\dfrac{dy}{dx}\bigg|_{x=1} = \dfrac◆LB◆2◆RB◆◆LB◆\sqrt{4 - 4 + 2}◆RB◆ = \dfrac◆LB◆2◆RB◆◆LB◆\sqrt{2}◆RB◆ = \sqrt{2}.

Equation of tangent: yln(1+2)=2(x1)y - \ln(1 + \sqrt{2}) = \sqrt{2}(x - 1), i.e.

y=2x2+ln(1+2)y = \sqrt{2}\,x - \sqrt{2} + \ln(1 + \sqrt{2}).


9. Advanced Worked Examples

Example 9.1: Solving hyperbolic equations

Problem. Solve 3sinhx+4coshx=53\sinh x + 4\cosh x = 5, giving your answer in exact logarithmic form.

Solution. Using the exponential definitions:

3exex2+4ex+ex2=53\cdot\frac{e^x - e^{-x}}{2} + 4\cdot\frac{e^x + e^{-x}}{2} = 5

3ex3ex+4ex+4ex=103e^x - 3e^{-x} + 4e^x + 4e^{-x} = 10

7ex+ex=107e^x + e^{-x} = 10

Multiplying by exe^x: 7e2x+1=10ex7e^{2x} + 1 = 10e^x

7e2x10ex+1=07e^{2x} - 10e^x + 1 = 0

This is a quadratic in exe^x:

ex=LB10±10028RB◆◆LB14RB=LB10±72RB◆◆LB14RB=LB10±62RB◆◆LB14RB=LB5±32RB◆◆LB7RBe^x = \frac◆LB◆10 \pm \sqrt{100 - 28}◆RB◆◆LB◆14◆RB◆ = \frac◆LB◆10 \pm \sqrt{72}◆RB◆◆LB◆14◆RB◆ = \frac◆LB◆10 \pm 6\sqrt{2}◆RB◆◆LB◆14◆RB◆ = \frac◆LB◆5 \pm 3\sqrt{2}◆RB◆◆LB◆7◆RB◆

x=ln ⁣(LB5+32RB◆◆LB7RB)orx=ln ⁣(LB532RB◆◆LB7RB)x = \ln\!\left(\frac◆LB◆5 + 3\sqrt{2}◆RB◆◆LB◆7◆RB◆\right) \quad \text{or} \quad x = \ln\!\left(\frac◆LB◆5 - 3\sqrt{2}◆RB◆◆LB◆7◆RB◆\right)

Since LB532RB◆◆LB7RB0.109>0\dfrac◆LB◆5 - 3\sqrt{2}◆RB◆◆LB◆7◆RB◆ \approx 0.109 > 0, both solutions are valid.

Example 9.2: Integration using hyperbolic substitution

Problem. Evaluate x29dx\displaystyle\int \sqrt{x^2 - 9}\,dx for x3x \geq 3.

Solution. Use the substitution x=3coshux = 3\cosh u, dx=3sinhududx = 3\sinh u\,du:

LB9cosh2u9RB3sinhudu=3sinhu3sinhudu=9sinh2udu\int \sqrt◆LB◆9\cosh^2 u - 9◆RB◆\cdot 3\sinh u\,du = \int 3\sinh u \cdot 3\sinh u\,du = 9\int \sinh^2 u\,du

Using sinh2u=LBcosh2u1RB◆◆LB2RB\sinh^2 u = \dfrac◆LB◆\cosh 2u - 1◆RB◆◆LB◆2◆RB◆:

=9LBcosh2u1RB◆◆LB2RBdu=92(LBsinh2uRB◆◆LB2RBu)+C=94sinh2u92u+C= 9\int \frac◆LB◆\cosh 2u - 1◆RB◆◆LB◆2◆RB◆\,du = \frac{9}{2}\left(\frac◆LB◆\sinh 2u◆RB◆◆LB◆2◆RB◆ - u\right) + C = \frac{9}{4}\sinh 2u - \frac{9}{2}u + C

Since x=3coshux = 3\cosh u: coshu=x3\cosh u = \dfrac{x}{3}, sinhu=LBx291RB=LBx29RB◆◆LB3RB\sinh u = \sqrt◆LB◆\dfrac{x^2}{9} - 1◆RB◆ = \dfrac◆LB◆\sqrt{x^2 - 9}◆RB◆◆LB◆3◆RB◆.

sinh2u=2sinhucoshu=LB2xx29RB◆◆LB9RB\sinh 2u = 2\sinh u\cosh u = \dfrac◆LB◆2x\sqrt{x^2 - 9}◆RB◆◆LB◆9◆RB◆.

u=arcosh ⁣(x3)=ln ⁣(x3+LBx291RB)u = \operatorname{arcosh}\!\left(\dfrac{x}{3}\right) = \ln\!\left(\dfrac{x}{3} + \sqrt◆LB◆\dfrac{x^2}{9} - 1◆RB◆\right).

=LBxx29RB◆◆LB2RB92arcosh ⁣(x3)+C= \frac◆LB◆x\sqrt{x^2 - 9}◆RB◆◆LB◆2◆RB◆ - \frac{9}{2}\operatorname{arcosh}\!\left(\frac{x}{3}\right) + C

Example 9.3: Proving an identity using Osborne's rule

Problem. Prove that cosh3x=4cosh3x3coshx\cosh 3x = 4\cosh^3 x - 3\cosh x.

Solution. From the trigonometric identity cos3θ=4cos3θ3cosθ\cos 3\theta = 4\cos^3\theta - 3\cos\theta, applying Osborne's rule: since cos3θ\cos^3\theta contains no products of sin\sin, it remains unchanged. Therefore:

cosh3x=4cosh3x3coshx\cosh 3x = 4\cosh^3 x - 3\cosh x

Direct proof. Starting from cosh3x=cosh(2x+x)\cosh 3x = \cosh(2x + x):

=cosh2xcoshx+sinh2xsinhx=(2cosh2x1)coshx+2sinh2xcoshx= \cosh 2x\cosh x + \sinh 2x\sinh x = (2\cosh^2 x - 1)\cosh x + 2\sinh^2 x\cosh x

=2cosh3xcoshx+2(cosh2x1)coshx=2cosh3xcoshx+2cosh3x2coshx= 2\cosh^3 x - \cosh x + 2(\cosh^2 x - 1)\cosh x = 2\cosh^3 x - \cosh x + 2\cosh^3 x - 2\cosh x

=4cosh3x3coshx= 4\cosh^3 x - 3\cosh x \quad \blacksquare

Example 9.4: Differentiation involving multiple hyperbolic functions

Problem. Find dydx\dfrac{dy}{dx} where y=LBsinhxRB◆◆LB1+coshxRBy = \dfrac◆LB◆\sinh x◆RB◆◆LB◆1 + \cosh x◆RB◆ and simplify your answer.

Solution. Using the quotient rule:

dydx=LBcoshx(1+coshx)sinhxsinhxRB◆◆LB(1+coshx)2RB=LBcoshx+cosh2xsinh2xRB◆◆LB(1+coshx)2RB\frac{dy}{dx} = \frac◆LB◆\cosh x(1 + \cosh x) - \sinh x \cdot \sinh x◆RB◆◆LB◆(1 + \cosh x)^2◆RB◆ = \frac◆LB◆\cosh x + \cosh^2 x - \sinh^2 x◆RB◆◆LB◆(1 + \cosh x)^2◆RB◆

Using cosh2xsinh2x=1\cosh^2 x - \sinh^2 x = 1:

=LBcoshx+1RB◆◆LB(1+coshx)2RB=LB1RB◆◆LB1+coshxRB=sech2 ⁣(x2)= \frac◆LB◆\cosh x + 1◆RB◆◆LB◆(1 + \cosh x)^2◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆1 + \cosh x◆RB◆ = \mathrm{sech}^2\!\left(\frac{x}{2}\right)

The final simplification uses the identity 1+coshx=2cosh2(x/2)1 + \cosh x = 2\cosh^2(x/2).

Example 9.5: Definite integral with inverse hyperbolic functions

Problem. Evaluate 01LBdxRB◆◆LB1+4x2RB\displaystyle\int_0^1 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{1 + 4x^2}◆RB◆.

Solution. Write 1+4x2=4(x2+1/4)=2x2+(1/2)2\sqrt{1 + 4x^2} = \sqrt{4(x^2 + 1/4)} = 2\sqrt{x^2 + (1/2)^2}.

01LBdxRB◆◆LB1+4x2RB=1201LBdxRB◆◆LBx2+1/4RB=12[arsinh ⁣(x1/2)]01\int_0^1 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{1 + 4x^2}◆RB◆ = \frac{1}{2}\int_0^1 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 + 1/4}◆RB◆ = \frac{1}{2}\left[\operatorname{arsinh}\!\left(\frac{x}{1/2}\right)\right]_0^1

=12[arsinh2arsinh0]=12ln(2+5)= \frac{1}{2}\bigl[\operatorname{arsinh}\,2 - \operatorname{arsinh}\,0\bigr] = \frac{1}{2}\ln(2 + \sqrt{5})

Example 9.6: Parametric differentiation with hyperbolic functions

Problem. A curve is given parametrically by x=2coshtx = 2\cosh t, y=3sinhty = 3\sinh t. Find the value of dydx\dfrac{dy}{dx} at t=ln2t = \ln 2.

Solution. dxdt=2sinht\dfrac{dx}{dt} = 2\sinh t, dydt=3cosht\dfrac{dy}{dt} = 3\cosh t.

dydx=LB3coshtRB◆◆LB2sinhtRB=32cotht\frac{dy}{dx} = \frac◆LB◆3\cosh t◆RB◆◆LB◆2\sinh t◆RB◆ = \frac{3}{2}\coth t

At t=ln2t = \ln 2: cosh(ln2)=2+1/22=54\cosh(\ln 2) = \dfrac{2 + 1/2}{2} = \dfrac{5}{4}, sinh(ln2)=21/22=34\sinh(\ln 2) = \dfrac{2 - 1/2}{2} = \dfrac{3}{4}.

dydxt=ln2=LB35/4RB◆◆LB23/4RB=15/43/2=52\frac{dy}{dx}\bigg|_{t = \ln 2} = \frac◆LB◆3 \cdot 5/4◆RB◆◆LB◆2 \cdot 3/4◆RB◆ = \frac{15/4}{3/2} = \frac{5}{2}

Example 9.7: Verifying a reduction formula

Problem. Let In=0π/2coshn(sinx)dxI_n = \displaystyle\int_0^{\pi/2} \cosh^n(\sin x)\,dx is not well-formed. Instead, verify that tanh3xdx=ln(coshx)12sech2xtanhx+C\displaystyle\int \tanh^3 x\,dx = \ln(\cosh x) - \dfrac{1}{2}\mathrm{sech}^2\,x\tanh x + C is incorrect, and find the correct integral.

Solution. Let us compute tanh3xdx\displaystyle\int \tanh^3 x\,dx correctly.

Write tanh3x=tanhxtanh2x=tanhx(1sech2x)=tanhxtanhxsech2x\tanh^3 x = \tanh x \cdot \tanh^2 x = \tanh x(1 - \mathrm{sech}^2\,x) = \tanh x - \tanh x\,\mathrm{sech}^2\,x.

tanh3xdx=tanhxdxtanhxsech2xdx\int \tanh^3 x\,dx = \int \tanh x\,dx - \int \tanh x\,\mathrm{sech}^2\,x\,dx

The first integral: tanhxdx=ln(coshx)+C\displaystyle\int\tanh x\,dx = \ln(\cosh x) + C.

For the second integral, let u=tanhxu = \tanh x, du=sech2xdxdu = \mathrm{sech}^2\,x\,dx:

udu=u22+C=LBtanh2xRB◆◆LB2RB+C\int u\,du = \frac{u^2}{2} + C = \frac◆LB◆\tanh^2 x◆RB◆◆LB◆2◆RB◆ + C

Therefore:

tanh3xdx=ln(coshx)LBtanh2xRB◆◆LB2RB+C\boxed{\int \tanh^3 x\,dx = \ln(\cosh x) - \frac◆LB◆\tanh^2 x◆RB◆◆LB◆2◆RB◆ + C}

Example 9.8: Arc length of a hyperbolic cosine curve

Problem. Find the arc length of y=acosh(x/a)y = a\cosh(x/a) from x=0x = 0 to x=bx = b.

Solution. dydx=sinh(x/a)\dfrac{dy}{dx} = \sinh(x/a).

s=0bLB1+sinh2(x/a)RBdx=0bcosh(x/a)dx=[asinh(x/a)]0b=asinh(b/a)s = \int_0^b \sqrt◆LB◆1 + \sinh^2(x/a)◆RB◆\,dx = \int_0^b \cosh(x/a)\,dx = \bigl[a\sinh(x/a)\bigr]_0^b = a\sinh(b/a)


10. Connections to Other Topics

10.1 Hyperbolic functions and differential equations

The differential equation d2ydx2y=0\dfrac{d^2y}{dx^2} - y = 0 has general solution y=Acoshx+Bsinhxy = A\cosh x + B\sinh x, which can also be written y=Cex+Dexy = Ce^x + De^{-x}. See Differential Equations.

10.2 Hyperbolic functions and complex numbers

The identities coshx=cos(ix)\cosh x = \cos(ix) and sinhx=isin(ix)\sinh x = -i\sin(ix) connect the two topics. See Complex Numbers.

10.3 Hyperbolic functions and integration techniques

Hyperbolic substitutions (x=asinhux = a\sinh u, x=acoshux = a\cosh u) are powerful alternatives to trigonometric substitutions. See Further Calculus.

10.4 The catenary and mechanics

The shape y=acosh(x/a)y = a\cosh(x/a) describes a hanging chain. The arc length is s=asinh(x/a)s = a\sinh(x/a). See Further Mechanics.


11. Additional Exam-Style Questions

Question 8

(a) Given sinhx=125\sinh x = \dfrac{12}{5}, find the exact value of coshx\cosh x and tanhx\tanh x.

(b) Hence evaluate arcosh ⁣(135)\operatorname{arcosh}\!\left(\dfrac{13}{5}\right) in exact logarithmic form.

Solution

(a) cosh2x=1+sinh2x=1+14425=16925\cosh^2 x = 1 + \sinh^2 x = 1 + \dfrac{144}{25} = \dfrac{169}{25}, so coshx=135\cosh x = \dfrac{13}{5} (positive root).

tanhx=LBsinhxRB◆◆LBcoshxRB=12/513/5=1213\tanh x = \dfrac◆LB◆\sinh x◆RB◆◆LB◆\cosh x◆RB◆ = \dfrac{12/5}{13/5} = \dfrac{12}{13}.

(b) Since coshx=135\cosh x = \dfrac{13}{5}:

arcosh ⁣(135)=x=ln ⁣(135+LB169251RB)=ln ⁣(135+125)=ln5\operatorname{arcosh}\!\left(\frac{13}{5}\right) = x = \ln\!\left(\frac{13}{5} + \sqrt◆LB◆\frac{169}{25} - 1◆RB◆\right) = \ln\!\left(\frac{13}{5} + \frac{12}{5}\right) = \ln 5

Question 9

Find the exact value of 0ln2cosh2xdx\displaystyle\int_0^{\ln 2} \cosh 2x\,dx.

Solution

0ln2cosh2xdx=[LBsinh2xRB◆◆LB2RB]0ln2=LBsinh(2ln2)RB◆◆LB2RB\int_0^{\ln 2}\cosh 2x\,dx = \left[\frac◆LB◆\sinh 2x◆RB◆◆LB◆2◆RB◆\right]_0^{\ln 2} = \frac◆LB◆\sinh(2\ln 2)◆RB◆◆LB◆2◆RB◆

sinh(2ln2)=LBe2ln2e2ln2RB◆◆LB2RB=41/42=158\sinh(2\ln 2) = \dfrac◆LB◆e^{2\ln 2} - e^{-2\ln 2}◆RB◆◆LB◆2◆RB◆ = \dfrac{4 - 1/4}{2} = \dfrac{15}{8}.

0ln2cosh2xdx=1516\int_0^{\ln 2}\cosh 2x\,dx = \frac{15}{16}

Question 10

Prove by induction that dndxn(sinhx)=sinhx\dfrac{d^n}{dx^n}(\sinh x) = \sinh x when nn is even and dndxn(sinhx)=coshx\dfrac{d^n}{dx^n}(\sinh x) = \cosh x when nn is odd.

Solution

Base case (n=0n = 0): d0dx0(sinhx)=sinhx\dfrac{d^0}{dx^0}(\sinh x) = \sinh x. Correct for n=0n = 0 (even).

Base case (n=1n = 1): ddx(sinhx)=coshx\dfrac{d}{dx}(\sinh x) = \cosh x. Correct for n=1n = 1 (odd).

Inductive step. Assume the result holds for n=kn = k.

If kk is even: dkdxk(sinhx)=sinhx\dfrac{d^k}{dx^k}(\sinh x) = \sinh x. Then dk+1dxk+1(sinhx)=ddx(sinhx)=coshx\dfrac{d^{k+1}}{dx^{k+1}}(\sinh x) = \dfrac{d}{dx}(\sinh x) = \cosh x. Since k+1k + 1 is odd, the result holds.

If kk is odd: dkdxk(sinhx)=coshx\dfrac{d^k}{dx^k}(\sinh x) = \cosh x. Then dk+1dxk+1(sinhx)=ddx(coshx)=sinhx\dfrac{d^{k+1}}{dx^{k+1}}(\sinh x) = \dfrac{d}{dx}(\cosh x) = \sinh x. Since k+1k + 1 is even, the result holds. \blacksquare

Question 11

Evaluate 3/22LB3RB◆◆LB4x29RBdx\displaystyle\int_{3/2}^2 \frac◆LB◆3◆RB◆◆LB◆\sqrt{4x^2 - 9}◆RB◆\,dx in exact form.

Solution

3/22LB3RB◆◆LB4x29RBdx=323/22LBdxRB◆◆LBx29/4RB=32[arcosh ⁣(2x3)]3/22\int_{3/2}^2 \frac◆LB◆3◆RB◆◆LB◆\sqrt{4x^2 - 9}◆RB◆\,dx = \frac{3}{2}\int_{3/2}^2 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - 9/4}◆RB◆ = \frac{3}{2}\left[\operatorname{arcosh}\!\left(\frac{2x}{3}\right)\right]_{3/2}^2

=32[arcosh ⁣(43)arcosh(1)]=32arcosh ⁣(43)= \frac{3}{2}\left[\operatorname{arcosh}\!\left(\frac{4}{3}\right) - \operatorname{arcosh}(1)\right] = \frac{3}{2}\operatorname{arcosh}\!\left(\frac{4}{3}\right)

=32ln ⁣(43+LB1691RB)=32ln ⁣(LB4+7RB◆◆LB3RB)= \frac{3}{2}\ln\!\left(\frac{4}{3} + \sqrt◆LB◆\frac{16}{9} - 1◆RB◆\right) = \frac{3}{2}\ln\!\left(\frac◆LB◆4 + \sqrt{7}◆RB◆◆LB◆3◆RB◆\right)

Question 12

Given that y=ln(sinhx)y = \ln(\sinh x), show that d2ydx2=cosech2x\dfrac{d^2y}{dx^2} = -\mathrm{cosech}^2\,x.

Solution

dydx=LBcoshxRB◆◆LBsinhxRB=cothx\frac{dy}{dx} = \frac◆LB◆\cosh x◆RB◆◆LB◆\sinh x◆RB◆ = \coth x

d2ydx2=ddx(cothx)=cosech2x=LB1RB◆◆LBsinh2xRB\frac{d^2y}{dx^2} = \frac{d}{dx}(\coth x) = -\mathrm{cosech}^2\,x = \frac◆LB◆-1◆RB◆◆LB◆\sinh^2 x◆RB◆ \quad \blacksquare

Question 13

(a) Express sinh(2ln3)\sinh(2\ln 3) in the form ab\dfrac{a}{b} where a,ba, b are integers.

(b) Hence find ln3ln2\ln 3 - \ln 2 in terms of inverse hyperbolic functions.

Solution

(a) sinh(2ln3)=2sinh(ln3)cosh(ln3)\sinh(2\ln 3) = 2\sinh(\ln 3)\cosh(\ln 3).

sinh(ln3)=31/32=43\sinh(\ln 3) = \dfrac{3 - 1/3}{2} = \dfrac{4}{3}, cosh(ln3)=3+1/32=53\cosh(\ln 3) = \dfrac{3 + 1/3}{2} = \dfrac{5}{3}.

sinh(2ln3)=24353=409\sinh(2\ln 3) = 2 \cdot \dfrac{4}{3} \cdot \dfrac{5}{3} = \dfrac{40}{9}.

(b) ln3ln2=ln(3/2)\ln 3 - \ln 2 = \ln(3/2). Since arsinhx=ln(x+x2+1)\operatorname{arsinh}\,x = \ln(x + \sqrt{x^2+1}):

arsinh ⁣(34)=ln ⁣(34+LB916+1RB)=ln ⁣(34+54)=ln2\operatorname{arsinh}\!\left(\dfrac{3}{4}\right) = \ln\!\left(\dfrac{3}{4} + \sqrt◆LB◆\dfrac{9}{16}+1◆RB◆\right) = \ln\!\left(\dfrac{3}{4} + \dfrac{5}{4}\right) = \ln 2.

Therefore ln2=arsinh(3/4)\ln 2 = \operatorname{arsinh}(3/4) and ln3=ln2+ln(3/2)=arsinh(3/4)+artanh(1/5)\ln 3 = \ln 2 + \ln(3/2) = \operatorname{arsinh}(3/4) + \operatorname{artanh}(1/5) (using artanh(1/5)=12ln(6/4)=12ln(3/2)\operatorname{artanh}(1/5) = \frac{1}{2}\ln(6/4) = \frac{1}{2}\ln(3/2)).

So ln3ln2=artanh(1/5)\ln 3 - \ln 2 = \operatorname{artanh}(1/5).


12. Summary of Extended Results

IdentityFormula
Triple anglesinh3x=3sinhx+4sinh3x\sinh 3x = 3\sinh x + 4\sinh^3 x
Triple anglecosh3x=4cosh3x3coshx\cosh 3x = 4\cosh^3 x - 3\cosh x
Half anglecosh2 ⁣(x2)=LB1+coshxRB◆◆LB2RB\cosh^2\!\left(\dfrac{x}{2}\right) = \dfrac◆LB◆1 + \cosh x◆RB◆◆LB◆2◆RB◆
Half anglesinh2 ⁣(x2)=LBcoshx1RB◆◆LB2RB\sinh^2\!\left(\dfrac{x}{2}\right) = \dfrac◆LB◆\cosh x - 1◆RB◆◆LB◆2◆RB◆
Integral of tanh\tanhtanhxdx=ln(coshx)+C\displaystyle\int\tanh x\,dx = \ln(\cosh x) + C
Integral of coth\cothcothxdx=ln(sinhx)+C\displaystyle\int\coth x\,dx = \ln(\sinh x) + C
Integral of tanh3\tanh^3tanh3xdx=ln(coshx)LBtanh2xRB◆◆LB2RB+C\displaystyle\int\tanh^3 x\,dx = \ln(\cosh x) - \dfrac◆LB◆\tanh^2 x◆RB◆◆LB◆2◆RB◆ + C
Arc length of catenarys=asinh(b/a)s = a\sinh(b/a) for y=acosh(x/a)y = a\cosh(x/a)

13. Further Common Pitfalls

Common Pitfall
  1. Substitution domain errors: When using x=acoshux = a\cosh u, the substitution requires xax \geq a (since coshu1\cosh u \geq 1). Attempting to use x=acoshux = a\cosh u for x<ax < a leads to an error. Use x=asinhux = a\sinh u for x2+a2\sqrt{x^2 + a^2} and x=acoshux = a\cosh u for x2a2\sqrt{x^2 - a^2}.
  2. Confusing artanh\operatorname{artanh} and ln\ln forms: The formula dxa2x2=12aln ⁣a+xax\displaystyle\int\frac{dx}{a^2 - x^2} = \frac{1}{2a}\ln\!\left|\frac{a+x}{a-x}\right| is valid for all xa|x| \neq a, but 1aartanh(x/a)\dfrac{1}{a}\operatorname{artanh}(x/a) is only valid for x<a|x| < a. For x>a|x| > a, use the logarithmic form or arcoth\operatorname{arcoth}.
  3. No absolute value needed for cosh\cosh: Unlike cosx|\cos x|, LBcosh2xRB=coshx\sqrt◆LB◆\cosh^2 x◆RB◆ = \cosh x (no absolute value needed) since coshx1>0\cosh x \geq 1 > 0 for all real xx.
  4. Differential equation solutions: The equation yy=0y'' - y = 0 has solutions in both exponential and hyperbolic forms. When boundary conditions involve y(0)y(0) and y(0)y'(0), the hyperbolic form y=Acoshx+Bsinhxy = A\cosh x + B\sinh x is often more convenient since cosh0=1\cosh 0 = 1 and sinh0=0\sinh 0 = 0. :::

14. Advanced Worked Examples

Example 14.1: Integration using sinh\sinh substitution

Problem. Evaluate x2+9dx\displaystyle\int \sqrt{x^2 + 9}\,dx.

Solution. Let x=3sinhux = 3\sinh u, dx=3coshududx = 3\cosh u\,du.

3coshu3coshudu=9cosh2udu=9LB1+cosh2uRB◆◆LB2RBdu=92 ⁣(u+LBsinh2uRB◆◆LB2RB)\int 3\cosh u \cdot 3\cosh u\,du = 9\int \cosh^2 u\,du = 9\int \frac◆LB◆1+\cosh 2u◆RB◆◆LB◆2◆RB◆\,du = \frac{9}{2}\!\left(u + \frac◆LB◆\sinh 2u◆RB◆◆LB◆2◆RB◆\right)

=9u2+LB9sinhucoshuRB◆◆LB2RB=92arsinh ⁣(x3)+LBxx2+9RB◆◆LB2RB+C= \frac{9u}{2} + \frac◆LB◆9\sinh u\cosh u◆RB◆◆LB◆2◆RB◆ = \frac{9}{2}\operatorname{arsinh}\!\left(\frac{x}{3}\right) + \frac◆LB◆x\sqrt{x^2+9}◆RB◆◆LB◆2◆RB◆ + C

Example 14.2: Solving y4y=0y'' - 4y = 0 with hyperbolic functions

Problem. Solve y4y=0y'' - 4y = 0 with y(0)=3y(0) = 3 and y(0)=8y'(0) = 8.

Solution. Auxiliary: m24=0    m=±2m^2 - 4 = 0 \implies m = \pm 2.

y=Acosh2x+Bsinh2xy = A\cosh 2x + B\sinh 2x.

y(0)=A=3y(0) = A = 3. y(0)=2B=8    B=4y'(0) = 2B = 8 \implies B = 4.

y=3cosh2x+4sinh2x\boxed{y = 3\cosh 2x + 4\sinh 2x}

In exponential form: y=3e2x+e2x2+4e2xe2x2=72e2x12e2xy = 3 \cdot \dfrac{e^{2x}+e^{-2x}}{2} + 4 \cdot \dfrac{e^{2x}-e^{-2x}}{2} = \dfrac{7}{2}e^{2x} - \dfrac{1}{2}e^{-2x}.

Example 14.3: Arc length of a catenary

Problem. Find the arc length of y=coshxy = \cosh x from x=0x = 0 to x=1x = 1.

Solution. y=sinhxy' = \sinh x. ds=LB1+sinh2xRBdx=coshxdxds = \sqrt◆LB◆1 + \sinh^2 x◆RB◆\,dx = \cosh x\,dx.

s=01coshxdx=[sinhx]01=sinh1=ee121.175s = \int_0^1 \cosh x\,dx = [\sinh x]_0^1 = \sinh 1 = \frac{e - e^{-1}}{2} \approx \boxed{1.175}

Example 14.4: Osborn's rule applied to tan2x\tan 2x

Problem. Using Osborn's rule, find tanh2x\tanh 2x in terms of tanhx\tanh x.

Solution. tan2x=LB2tanxRB◆◆LB1tan2xRB\tan 2x = \dfrac◆LB◆2\tan x◆RB◆◆LB◆1-\tan^2 x◆RB◆. Apply Osborn's rule (change tan2x\tan^2 x to tanh2x-\tanh^2 x):

tanh2x=LB2tanhxRB◆◆LB1+tanh2xRB\boxed{\tanh 2x = \frac◆LB◆2\tanh x◆RB◆◆LB◆1+\tanh^2 x◆RB◆}

Example 14.5: Deriving the Gudermannian function relationship

Problem. The Gudermannian function relates circular and hyperbolic functions: secθ=coshu\sec\theta = \cosh u where u=gd1(θ)u = \operatorname{gd}^{-1}(\theta). Show that LBdθRB◆◆LBduRB=sechu\dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = \operatorname{sech}\, u.

Solution. secθ=coshu    cosθ=sechu\sec\theta = \cosh u \implies \cos\theta = \operatorname{sech}\, u.

Differentiating implicitly with respect to uu: sinθLBdθRB◆◆LBduRB=sechutanhu-\sin\theta \cdot \dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = -\operatorname{sech}\,u \tanh u.

LBdθRB◆◆LBduRB=LBsechutanhuRB◆◆LBsinθRB\dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = \dfrac◆LB◆\operatorname{sech}\,u \tanh u◆RB◆◆LB◆\sin\theta◆RB◆.

Since cosθ=sechu\cos\theta = \operatorname{sech}\,u: sinθ=LB1sech2uRB=LB1LB1RB◆◆LBcosh2uRB◆◆RB=LBLBcosh2u1RB◆◆RB◆◆LBcoshuRB=LBsinhuRB◆◆LBcoshuRB=tanhu\sin\theta = \sqrt◆LB◆1-\operatorname{sech}^2 u◆RB◆ = \sqrt◆LB◆1-\dfrac◆LB◆1◆RB◆◆LB◆\cosh^2 u◆RB◆◆RB◆ = \dfrac◆LB◆\sqrt◆LB◆\cosh^2 u - 1◆RB◆◆RB◆◆LB◆\cosh u◆RB◆ = \dfrac◆LB◆\sinh u◆RB◆◆LB◆\cosh u◆RB◆ = \tanh u.

LBdθRB◆◆LBduRB=LBsechutanhuRB◆◆LBtanhuRB=sechu\dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = \dfrac◆LB◆\operatorname{sech}\,u \tanh u◆RB◆◆LB◆\tanh u◆RB◆ = \boxed{\operatorname{sech}\,u}. \blacksquare


15. Additional Exam-Style Questions

Question 16

Evaluate 12LBdxRB◆◆LBx21RB\displaystyle\int_1^2 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆.

Solution

=[arcoshx]12=ln(2+3)ln1=ln(2+3)= [\operatorname{arcosh}\, x]_1^2 = \ln(2+\sqrt{3}) - \ln 1 = \boxed{\ln(2+\sqrt{3})}.

Question 17

Prove that sinh(x+y)=sinhxcoshy+coshxsinhy\sinh(x+y) = \sinh x\cosh y + \cosh x\sinh y.

Solution

sinhxcoshy+coshxsinhy=(exex)(ey+ey)+(ex+ex)(eyey)4\sinh x\cosh y + \cosh x\sinh y = \dfrac{(e^x-e^{-x})(e^y+e^{-y}) + (e^x+e^{-x})(e^y-e^{-y})}{4}

=ex+y+exyex+yexy+ex+yexy+ex+yexy4= \dfrac{e^{x+y}+e^{x-y}-e^{-x+y}-e^{-x-y}+e^{x+y}-e^{x-y}+e^{-x+y}-e^{-x-y}}{4}

=2ex+y2e(x+y)4=ex+ye(x+y)2=sinh(x+y)= \dfrac{2e^{x+y}-2e^{-(x+y)}}{4} = \dfrac{e^{x+y}-e^{-(x+y)}}{2} = \sinh(x+y). \blacksquare

Question 18

Find ddx[arcoshx]\dfrac{d}{dx}[\operatorname{arcosh}\, x] and state the domain.

Solution

Let y=arcoshxy = \operatorname{arcosh}\, x, so x=coshyx = \cosh y and x1x \geq 1.

1=sinhydydx1 = \sinh y \cdot \dfrac{dy}{dx}.

dydx=LB1RB◆◆LBsinhyRB=LB1RB◆◆LBLBcosh2y1RB◆◆RB=LB1RB◆◆LBx21RB\dfrac{dy}{dx} = \dfrac◆LB◆1◆RB◆◆LB◆\sinh y◆RB◆ = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt◆LB◆\cosh^2 y - 1◆RB◆◆RB◆ = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2-1}◆RB◆.

ddx[arcoshx]=LB1RB◆◆LBx21RB\boxed{\dfrac{d}{dx}[\operatorname{arcosh}\, x] = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2-1}◆RB◆} for x>1x > 1.


16. Advanced Topics

16.1 The Gudermannian function

The Gudermannian function gd(x)\mathrm{gd}(x) relates circular and hyperbolic functions without complex numbers:

sin(gdx)=tanhx\sin(\mathrm{gd}\,x) = \tanh x, cos(gdx)=sechx\cos(\mathrm{gd}\,x) = \mathrm{sech}\,x, tan(gdx)=sinhx\tan(\mathrm{gd}\,x) = \sinh x.

ddxgd(x)=sechx\dfrac{d}{dx}\mathrm{gd}(x) = \mathrm{sech}\,x.

16.2 Hyperbolic functions and the Lorentz transformation

In special relativity, the Lorentz transformation uses hyperbolic functions. If β=v/c\beta = v/c and γ=(1β2)1/2=coshϕ\gamma = (1-\beta^2)^{-1/2} = \cosh\phi where tanhϕ=β\tanh\phi = \beta, then:

t=tcoshϕxsinhϕ/ct' = t\cosh\phi - x\sinh\phi/c, x=xcoshϕctsinhϕx' = x\cosh\phi - ct\sinh\phi.

16.3 Inverse hyperbolic functions in logarithmic form

| Function | Logarithmic Form | Domain | | -------------------------- | -------------------------------------------------------------- | -------------- | --- | ---- | | arsinhx\operatorname{arsinh}\,x | ln(x+x2+1)\ln(x+\sqrt{x^2+1}) | all real xx | | arcoshx\operatorname{arcosh}\,x | ln(x+x21)\ln(x+\sqrt{x^2-1}) | x1x \geq 1 | | artanhx\operatorname{artanh}\,x | 12ln ⁣(1+x1x)\dfrac{1}{2}\ln\!\left(\dfrac{1+x}{1-x}\right) | x<1 | x | < 1 | | arcothx\operatorname{arcoth}\,x | 12ln ⁣(x+1x1)\dfrac{1}{2}\ln\!\left(\dfrac{x+1}{x-1}\right) | x>1 | x | > 1 | | arsechx\operatorname{arsech}\,x | ln ⁣(LB1+1x2RB◆◆LBxRB)\ln\!\left(\dfrac◆LB◆1+\sqrt{1-x^2}◆RB◆◆LB◆x◆RB◆\right) | 0<x10 < x \leq 1 | | arcschx\operatorname{arcsch}\,x | ln ⁣(1x+LB1x2+1RB)\ln\!\left(\dfrac{1}{x}+\sqrt◆LB◆\dfrac{1}{x^2}+1◆RB◆\right) | x0x \neq 0 |

16.4 Hyperbolic functions and catenary applications

The catenary y=acosh(x/a)y = a\cosh(x/a) appears in:

  • Suspension bridges (cables hang in a catenary)
  • Arch shapes (the inverted catenary is the strongest arch)
  • Power lines between poles

17. Further Exam-Style Questions

Question 19

Solve the equation 2coshxsinhx=32\cosh x - \sinh x = 3.

Solution

2ex+ex2exex2=32\cdot\dfrac{e^x+e^{-x}}{2} - \dfrac{e^x-e^{-x}}{2} = 3.

ex+exex2+ex2=3e^x+e^{-x} - \dfrac{e^x}{2} + \dfrac{e^{-x}}{2} = 3.

ex2+3ex2=3    ex+3ex=6\dfrac{e^x}{2} + \dfrac{3e^{-x}}{2} = 3 \implies e^x + 3e^{-x} = 6.

e2x6ex+3=0e^{2x} - 6e^x + 3 = 0.

ex=LB6±3612RB◆◆LB2RB=3±6e^x = \dfrac◆LB◆6 \pm \sqrt{36-12}◆RB◆◆LB◆2◆RB◆ = 3 \pm \sqrt{6}.

x=ln(3+6)x = \ln(3+\sqrt{6}) or x=ln(36)x = \ln(3-\sqrt{6}).

Since 36>03-\sqrt{6} > 0, both are valid.

Question 20

Prove that arcoshx=ln(x+x21)\operatorname{arcosh}\,x = \ln(x+\sqrt{x^2-1}) for x1x \geq 1.

Solution

Let y=arcoshxy = \operatorname{arcosh}\,x, so x=coshy=ey+ey2x = \cosh y = \dfrac{e^y+e^{-y}}{2}.

2x=ey+ey    e2y2xey+1=02x = e^y + e^{-y} \implies e^{2y} - 2xe^y + 1 = 0.

ey=LB2x±4x24RB◆◆LB2RB=x±x21e^y = \dfrac◆LB◆2x \pm \sqrt{4x^2-4}◆RB◆◆LB◆2◆RB◆ = x \pm \sqrt{x^2-1}.

Since ey1e^y \geq 1 and x1x \geq 1: ey=x+x21e^y = x + \sqrt{x^2-1} (the positive root, since xx211x-\sqrt{x^2-1} \leq 1).

y=ln(x+x21)y = \ln(x+\sqrt{x^2-1}). \blacksquare


17. Further Advanced Topics

17.1 Hyperbolic substitutions in integration

Standard substitutions:

  • x2+a2\sqrt{x^2+a^2}: use x=acoshtx = a\cosh t
  • x2a2\sqrt{x^2-a^2}: use x=acoshtx = a\cosh t (for xax \geq a)
  • a2x2\sqrt{a^2-x^2}: use x=acostx = a\cos t (circular, not hyperbolic)

Example: LBdxRB◆◆LBx24RB\displaystyle\int \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2-4}◆RB◆ with x=2coshtx = 2\cosh t:

dx=2sinhtdtdx = 2\sinh t\,dt, x24=2sinht\sqrt{x^2-4} = 2\sinh t.

LB2sinhtRB◆◆LB2sinhtRBdt=t=arcosh ⁣(x2)+C\displaystyle\int \frac◆LB◆2\sinh t◆RB◆◆LB◆2\sinh t◆RB◆\,dt = t = \operatorname{arcosh}\!\left(\frac{x}{2}\right) + C.

17.2 Gudermannian function

The Gudermannian function relates circular and hyperbolic functions without complex numbers:

gd(x)=0xsechtdt=2arctan(ex)LBπRB◆◆LB2RB\operatorname{gd}(x) = \int_0^x \operatorname{sech} t\,dt = 2\arctan(e^x) - \frac◆LB◆\pi◆RB◆◆LB◆2◆RB◆

Key identities:

  • sin(gdx)=tanhx\sin(\operatorname{gd}\,x) = \tanh x
  • cos(gdx)=sechx\cos(\operatorname{gd}\,x) = \operatorname{sech} x
  • tan(gdx)=sinhx\tan(\operatorname{gd}\,x) = \sinh x

17.3 Hyperbolic functions and catenary

The catenary curve y=acosh ⁣(xa)y = a\cosh\!\left(\dfrac{x}{a}\right) describes a hanging chain.

Arc length from the vertex: s=asinh ⁣(xa)s = a\sinh\!\left(\dfrac{x}{a}\right).


18. Further Exam-Style Questions

Question 16

Prove that arsinhx=ln(x+x2+1)\operatorname{arsinh}\,x = \ln(x+\sqrt{x^2+1}).

Solution

Let y=arsinhxy = \operatorname{arsinh}\,x, so x=sinhy=eyey2x = \sinh y = \dfrac{e^y-e^{-y}}{2}.

2x=eyey    e2y2xey1=02x = e^y - e^{-y} \implies e^{2y} - 2xe^y - 1 = 0.

ey=LB2x+4x2+4RB◆◆LB2RB=x+x2+1e^y = \dfrac◆LB◆2x + \sqrt{4x^2+4}◆RB◆◆LB◆2◆RB◆ = x + \sqrt{x^2+1} (positive root since ey>0e^y > 0).

y=ln(x+x2+1)y = \ln(x+\sqrt{x^2+1}). \blacksquare

Question 17

Use the substitution x=3sinhtx = 3\sinh t to evaluate 0arsinh(4/3)x2+9dx\displaystyle\int_0^{\operatorname{arsinh}(4/3)} \sqrt{x^2+9}\,dx.

Solution

dx=3coshtdtdx = 3\cosh t\,dt, x2+9=3cosht\sqrt{x^2+9} = 3\cosh t.

=0arsinh(4/3)9cosh2tdt=920arsinh(4/3)(1+cosh2t)dt= \displaystyle\int_0^{\operatorname{arsinh}(4/3)} 9\cosh^2 t\,dt = \frac{9}{2}\int_0^{\operatorname{arsinh}(4/3)} (1+\cosh 2t)\,dt

=92 ⁣[t+LBsinh2tRB◆◆LB2RB]0arsinh(4/3)= \frac{9}{2}\!\left[t + \frac◆LB◆\sinh 2t◆RB◆◆LB◆2◆RB◆\right]_0^{\operatorname{arsinh}(4/3)}.

At t=arsinh(4/3)t = \operatorname{arsinh}(4/3): sinht=4/3\sinh t = 4/3, cosht=5/3\cosh t = 5/3, sinh2t=24353=409\sinh 2t = 2\cdot\dfrac{4}{3}\cdot\dfrac{5}{3} = \dfrac{40}{9}.

=92 ⁣(arsinh ⁣43+209)=92arsinh ⁣43+10= \frac{9}{2}\!\left(\operatorname{arsinh}\!\frac{4}{3} + \frac{20}{9}\right) = \boxed{\frac{9}{2}\operatorname{arsinh}\!\frac{4}{3} + 10}.