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Hyperbolic Functions (Extended)

flowchart TD
A[Hyperbolic Functions] --> B[Key Concepts]
A --> C[Core Principles]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
C --> F[Design patterns]
D --> G[Real-world usage]

This topic explores fundamental concepts that shape our understanding of the world.

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


1.1 The three fundamental hyperbolic functions

Section titled “1.1 The three fundamental hyperbolic functions”
sinh⁡x=ex−e−x2\sinh x = \frac{e^x - e^{-x}}{2} cosh⁡x=ex+e−x2\cosh x = \frac{e^x + e^{-x}}{2} tanh⁡x=sinh⁡xcosh⁡x=ex−e−xex+e−x\tanh x = \frac{\sinh x}{\cosh x} = \frac{e^x - e^{-x}}{e^x + e^{-x}}cosech x=1sinh⁡x=2ex−e−x,x≠0\mathrm{cosech}\,x = \frac{1}{\sinh x} = \frac{2}{e^x - e^{-x}}, \quad x \neq 0 sech x=1cosh⁡x=2ex+e−x\mathrm{sech}\,x = \frac{1}{\cosh x} = \frac{2}{e^x + e^{-x}} coth⁡x=1tanh⁡x=ex+e−xex−e−x,x≠0\coth x = \frac{1}{\tanh x} = \frac{e^x + e^{-x}}{e^x - e^{-x}}, \quad x \neq 0
  • \sinh 0 = 0$$\cosh 0 = 1$$\tanh 0 = 0.
  • sinh⁡x\sinh x is odd: sinh⁡(−x)=−sinh⁡x\sinh(-x) = -\sinh x.
  • cosh⁡x\cosh x is even: cosh⁡(−x)=cosh⁡x\cosh(-x) = \cosh x.
  • tanh⁡x\tanh x is odd.
  • As x→+∞x \to +\infty: \sinh x \to +\infty$$\cosh x \to +\infty$$\tanh x \to 1.
  • As x→−∞x \to -\infty: \sinh x \to -\infty$$\cosh x \to +\infty$$\tanh x \to -1.
cosh⁡x=cos⁡(ix),sinh⁡x=−isin⁡(ix)\cosh x = \cos(ix), \qquad \sinh x = -i\sin(ix)

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

−isin⁡(ix)=−i⋅ei(ix)−e−i(ix)2i=e−x−ex−2=ex−e−x2=sinh⁡x-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

  • sinh⁡x\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.
  • cosh⁡x\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.
  • tanh⁡x\tanh x: S-shaped curve with horizontal asymptotes at y=±1y = \pm 1 Passing through the origin with gradient 1.

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

Proof.

cosh⁡2x−sinh⁡2x=(ex+e−x)24−(ex−e−x)24\cosh^2 x - \sinh^2 x = \frac{(e^x + e^{-x})^2}{4} - \frac{(e^x - e^{-x})^2}{4} =e2x+2+e−2x−(e2x−2+e−2x)4=44=1■= \frac{e^{2x} + 2 + e^{-2x} - (e^{2x} - 2 + e^{-2x})}{4} = \frac{4}{4} = 1 \quad \blacksquare1−tanh⁡2x=sech2 x\boxed{1 - \tanh^2 x = \mathrm{sech}^2\,x}

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

1−tanh⁡2x=1cosh⁡2x=sech2 x■1 - \tanh^2 x = \frac{1}{\cosh^2 x} = \mathrm{sech}^2\,x \quad \blacksquare

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: cos⁡2x+sin⁡2x=1\cos^2 x + \sin^2 x = 1 becomes cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1 (the sinh⁡2\sinh^2 term is Negated).

Example: sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x\cos x becomes sinh⁡2x=2sinh⁡xcosh⁡x\sinh 2x = 2\sinh x\cosh x (the product sinh⁡xcosh⁡x\sinh x \cosh x is negated since it contains sinh⁡\sinh But sinh⁡2x\sinh 2x on the left is not a product, So the overall sign changes on both sides cancel).

sinh⁡2x=2sinh⁡xcosh⁡x\sinh 2x = 2\sinh x\cosh x cosh⁡2x=cosh⁡2x+sinh⁡2x=2cosh⁡2x−1=1+2sinh⁡2x\cosh 2x = \cosh^2 x + \sinh^2 x = 2\cosh^2 x - 1 = 1 + 2\sinh^2 x

Proof of cosh⁡2x=2cosh⁡2x−1\cosh 2x = 2\cosh^2 x - 1:

cosh⁡2x=e2x+e−2x2=(ex+e−x)2−22=4cosh⁡2x−22=2cosh⁡2x−1■\cosh 2x = \frac{e^{2x} + e^{-2x}}{2} = \frac{(e^x + e^{-x})^2 - 2}{2} = \frac{4\cosh^2 x - 2}{2} = 2\cosh^2 x - 1 \quad \blacksquaresinh⁡(A±B)=sinh⁡Acosh⁡B±cosh⁡Asinh⁡B\sinh(A \pm B) = \sinh A\cosh B \pm \cosh A\sinh B cosh⁡(A±B)=cosh⁡Acosh⁡B±sinh⁡Asinh⁡B\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+B−e−(A+B)2=eAeB−e−Ae−B2\sinh(A + B) = \frac{e^{A+B} - e^{-(A+B)}}{2} = \frac{e^A e^B - e^{-A}e^{-B}}{2} =(eA−e−A)(eB+e−B)+(eA+e−A)(eB−e−B)4= \frac{(e^A - e^{-A})(e^B + e^{-B}) + (e^A + e^{-A})(e^B - e^{-B})}{4} =sinh⁡Acosh⁡B+cosh⁡Asinh⁡B■= \sinh A\cosh B + \cosh A\sinh B \quad \blacksquare

Problem. Given sinh⁡x=3\sinh x = 3 Find cosh⁡x\cosh x and tanh⁡x\tanh x without finding xx.

From cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1:

cosh⁡2x=1+9=10  ⟹  cosh⁡x=10\cosh^2 x = 1 + 9 = 10 \implies \cosh x = \sqrt{10}

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

tanh⁡x=sinh⁡xcosh⁡x=310=31010\tanh x = \frac{\sinh x}{\cosh x} = \frac{3}{\sqrt{10}} = \frac{3\sqrt{10}}{10}
arsinh⁡ x=ln⁡ ⁣(x+x2+1),x∈R\operatorname{arsinh}\,x = \ln\!\left(x + \sqrt{x^2 + 1}\right), \quad x \in \mathbb{R} arcosh⁡ x=ln⁡ ⁣(x+x2−1),x≥1\operatorname{arcosh}\,x = \ln\!\left(x + \sqrt{x^2 - 1}\right), \quad x \geq 1 artanh⁡ x=12ln⁡ ⁣(1+x1−x),−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 arsinh⁡ x=ln⁡(x+x2+1)\operatorname{arsinh}\,x = \ln(x + \sqrt{x^2 + 1})

Section titled “3.2 Derivation of arsinh⁡ x=ln⁡(x+x2+1)\operatorname{arsinh}\,x = \ln(x + \sqrt{x^2 + 1})arsinhx=ln(x+x2+1​)”

Let y=arsinh⁡ xy = \operatorname{arsinh}\,x So x=sinh⁡y=ey−e−y2x = \sinh y = \dfrac{e^y - e^{-y}}{2}.

2x=ey−e−y  ⟹  e2y−2xey−1=02x = e^y - e^{-y} \implies e^{2y} - 2xe^y - 1 = 0

This is a quadratic in eye^y:

ey=2x±4x2+42=x±x2+1e^y = \frac{2x \pm \sqrt{4x^2 + 4}}{2} = 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 arcosh⁡ x=ln⁡(x+x2−1)\operatorname{arcosh}\,x = \ln(x + \sqrt{x^2 - 1})

Section titled “3.3 Derivation of arcosh⁡ x=ln⁡(x+x2−1)\operatorname{arcosh}\,x = \ln(x + \sqrt{x^2 - 1})arcoshx=ln(x+x2−1​)”

Let y=arcosh⁡ xy = \operatorname{arcosh}\,x So x=cosh⁡y=ey+e−y2x = \cosh y = \dfrac{e^y + e^{-y}}{2}.

2x=ey+e−y  ⟹  e2y−2xey+1=02x = e^y + e^{-y} \implies e^{2y} - 2xe^y + 1 = 0 ey=2x±4x2−42=x±x2−1e^y = \frac{2x \pm \sqrt{4x^2 - 4}}{2} = x \pm \sqrt{x^2 - 1}

Since ey≥1e^y \geq 1 and x≥1x \geq 1 We need ey≥1e^y \geq 1. Both roots are positive when x≥1x \geq 1. The convention is to take ey=x+x2−1e^y = x + \sqrt{x^2 - 1} (which gives y≥0y \geq 0):

y=ln⁡ ⁣(x+x2−1)■y = \ln\!\left(x + \sqrt{x^2 - 1}\right) \quad \blacksquare

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

Section titled “3.4 Derivation of artanh⁡ x\operatorname{artanh}\,xartanhx”

Let y=artanh⁡ xy = \operatorname{artanh}\,x So x=tanh⁡yx = \tanh y.

x=ey−e−yey+e−y=e2y−1e2y+1x = \frac{e^y - e^{-y}}{e^y + e^{-y}} = \frac{e^{2y} - 1}{e^{2y} + 1} x(e2y+1)=e2y−1  ⟹  e2y(1−x)=1+xx(e^{2y} + 1) = e^{2y} - 1 \implies e^{2y}(1 - x) = 1 + x e2y=1+x1−x  ⟹  2y=ln⁡ ⁣(1+x1−x)e^{2y} = \frac{1 + x}{1 - x} \implies 2y = \ln\!\left(\frac{1 + x}{1 - x}\right) y=12ln⁡ ⁣(1+x1−x)■y = \frac{1}{2}\ln\!\left(\frac{1 + x}{1 - x}\right) \quad \blacksquare

Problem. Evaluate arsinh⁡ 2\operatorname{arsinh}\,2 and artanh⁡ 13\operatorname{artanh}\,\dfrac{1}{3} in exact Logarithmic form.

arsinh⁡ 2=ln⁡(2+5)\operatorname{arsinh}\,2 = \ln(2 + \sqrt{5}) artanh⁡ 13=12ln⁡ ⁣(4/32/3)=12ln⁡2\operatorname{artanh}\,\frac{1}{3} = \frac{1}{2}\ln\!\left(\frac{4/3}{2/3}\right) = \frac{1}{2}\ln 2
FunctionDomainRange
arsinh⁡ x\operatorname{arsinh}\,xR\mathbb{R}R\mathbb{R}
arcosh⁡ x\operatorname{arcosh}\,xx≥1x \geq 1y≥0y \geq 0
artanh⁡ x\operatorname{artanh}\,x−1<x<1-1 \lt x \lt 1R\mathbb{R}

ddx(sinh⁡x)=cosh⁡x\frac{d}{dx}(\sinh x) = \cosh x ddx(cosh⁡x)=sinh⁡x\frac{d}{dx}(\cosh x) = \sinh x ddx(tanh⁡x)=sech2 x\frac{d}{dx}(\tanh x) = \mathrm{sech}^2\,x

Proof of ddxsinh⁡x=cosh⁡x\dfrac{d}{dx}\sinh x = \cosh x:

ddx ⁣(ex−e−x2)=ex+e−x2=cosh⁡x■\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

Section titled “4.2 Differentiation of inverse hyperbolic functions”
ddx(arsinh⁡ x)=1x2+1\frac{d}{dx}(\operatorname{arsinh}\,x) = \frac{1}{\sqrt{x^2 + 1}} ddx(arcosh⁡ x)=1x2−1,x>1\frac{d}{dx}(\operatorname{arcosh}\,x) = \frac{1}{\sqrt{x^2 - 1}}, \quad x \gt 1 ddx(artanh⁡ x)=11−x2,∣x∣<1\frac{d}{dx}(\operatorname{artanh}\,x) = \frac{1}{1 - x^2}, \quad |x| \lt 1

Proof for arsinh⁡ x\operatorname{arsinh}\,x. Let y=arsinh⁡ xy = \operatorname{arsinh}\,x So x=sinh⁡yx = \sinh y.

dydx=1dxdy=1cosh⁡y=11+sinh⁡2y=11+x2■\frac{dy}{dx} = \frac{1}{\dfrac{dx}{dy}} = \frac{1}{\cosh y} = \frac{1}{\sqrt{1 + \sinh^2 y}} = \frac{1}{\sqrt{1 + x^2}} \quad \blacksquare

Proof for artanh⁡ x\operatorname{artanh}\,x. Let y=artanh⁡ xy = \operatorname{artanh}\,x So x=tanh⁡yx = \tanh y.

dydx=1sech2 y=11−tanh⁡2y=11−x2■\frac{dy}{dx} = \frac{1}{\mathrm{sech}^2\,y} = \frac{1}{1 - \tanh^2 y} = \frac{1}{1 - x^2} \quad \blacksquare

The differentiation results give standard integrals:

∫cosh⁡x dx=sinh⁡x+C\int \cosh x\,dx = \sinh x + C ∫sinh⁡x dx=cosh⁡x+C\int \sinh x\,dx = \cosh x + C ∫sech2 x dx=tanh⁡x+C\int \mathrm{sech}^2\,x\,dx = \tanh x + C

4.4 Integrals leading to inverse hyperbolic functions

Section titled “4.4 Integrals leading to inverse hyperbolic functions”
∫1x2+a2 dx=arsinh⁡ ⁣(xa)+C\int \frac{1}{\sqrt{x^2 + a^2}}\,dx = \operatorname{arsinh}\!\left(\frac{x}{a}\right) + C ∫1x2−a2 dx=arcosh⁡ ⁣(xa)+C,x>a\int \frac{1}{\sqrt{x^2 - a^2}}\,dx = \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C, \quad x \gt a ∫1a2−x2 dx=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:

∫dxx2+a2=∫a duau2+1=arsinh⁡ u+C=arsinh⁡ ⁣(xa)+C■\int \frac{dx}{\sqrt{x^2 + a^2}} = \int \frac{a\,du}{a\sqrt{u^2 + 1}} = \operatorname{arsinh}\,u + C = \operatorname{arsinh}\!\left(\frac{x}{a}\right) + C \quad \blacksquare

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

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

Problem. Evaluate ∫14x2+9 dx\displaystyle\int \frac{1}{\sqrt{4x^2 + 9}}\,dx.

∫dx4x2+9=12∫d(2x)(2x)2+9=12arsinh⁡ ⁣(2x3)+C\int \frac{dx}{\sqrt{4x^2 + 9}} = \frac{1}{2}\int \frac{d(2x)}{\sqrt{(2x)^2 + 9}} = \frac{1}{2}\operatorname{arsinh}\!\left(\frac{2x}{3}\right) + C

Problem. Evaluate ∫01dxx2+1\displaystyle\int_0^1 \frac{dx}{\sqrt{x^2 + 1}}.

=[arsinh⁡ x]01=arsinh⁡ 1−arsinh⁡ 0=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

Section titled “4.8 Worked example: integration by substitution with hyperbolic functions”

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

Use the substitution x=2sinh⁡ux = 2\sinh u, dx=2cosh⁡u dudx = 2\cosh u\,du:

∫4sinh⁡2u+4⋅2cosh⁡u du=∫2cosh⁡u⋅2cosh⁡u du=4∫cosh⁡2u du\int \sqrt{4\sinh^2 u + 4}\cdot 2\cosh u\,du = \int 2\cosh u \cdot 2\cosh u\,du = 4\int \cosh^2 u\,du

Using cosh⁡2u=1+cosh⁡2u2\cosh^2 u = \dfrac{1 + \cosh 2u}{2}:

=4∫1+cosh⁡2u2 du=2u+sinh⁡2u+C= 4\int \frac{1 + \cosh 2u}{2}\,du = 2u + \sinh 2u + C =2u+2sinh⁡ucosh⁡u+C= 2u + 2\sinh u\cosh u + C

Since x=2sinh⁡ux = 2\sinh u: sinh⁡u=x2\sinh u = \dfrac{x}{2} cosh⁡u=1+x24=x2+42\cosh u = \sqrt{1 + \dfrac{x^2}{4}} = \dfrac{\sqrt{x^2 + 4}}{2} u=arsinh⁡ ⁣(x2)u = \operatorname{arsinh}\!\left(\dfrac{x}{2}\right).

=2arsinh⁡ ⁣(x2)+xx2+42+C= 2\operatorname{arsinh}\!\left(\frac{x}{2}\right) + \frac{x\sqrt{x^2 + 4}}{2} + C

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

Solution

4sinh⁡x=3cosh⁡x  ⟹  tanh⁡x=344\sinh x = 3\cosh x \implies \tanh x = \dfrac{3}{4}.

x=artanh⁡ ⁣(34)=12ln⁡ ⁣(1+3/41−3/4)=12ln⁡7x = \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.

Prove that sinh⁡3x=3sinh⁡x+4sinh⁡3x\sinh 3x = 3\sinh x + 4\sinh^3 x.

Solution

sinh⁡3x=sinh⁡(2x+x)=sinh⁡2xcosh⁡x+cosh⁡2xsinh⁡x\sinh 3x = \sinh(2x + x) = \sinh 2x\cosh x + \cosh 2x\sinh x

=2sinh⁡xcosh⁡2x+(1+2sinh⁡2x)sinh⁡x= 2\sinh x\cosh^2 x + (1 + 2\sinh^2 x)\sinh x

=2sinh⁡x(1+sinh⁡2x)+sinh⁡x+2sinh⁡3x= 2\sinh x(1 + \sinh^2 x) + \sinh x + 2\sinh^3 x

=2sinh⁡x+2sinh⁡3x+sinh⁡x+2sinh⁡3x=3sinh⁡x+4sinh⁡3x= 2\sinh x + 2\sinh^3 x + \sinh x + 2\sinh^3 x = 3\sinh x + 4\sinh^3 x.

Evaluate ∫02dxx2+16\displaystyle\int_0^2 \frac{dx}{\sqrt{x^2 + 16}}.

Solution

=[arsinh⁡ ⁣(x4)]02=arsinh⁡ ⁣(12)=ln⁡ ⁣(12+54)=ln⁡ ⁣(1+52)= \left[\operatorname{arsinh}\!\left(\dfrac{x}{4}\right)\right]_0^2 = \operatorname{arsinh}\!\left(\dfrac{1}{2}\right) = \ln\!\left(\dfrac{1}{2} + \sqrt{\dfrac{5}{4}}\right) = \ln\!\left(\dfrac{1 + \sqrt{5}}{2}\right).

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

Solution

Using the product rule:

f′(x)=arcosh⁡ x+x⋅1x2−1=arcosh⁡ x+xx2−1f'(x) = \operatorname{arcosh}\,x + x \cdot \dfrac{1}{\sqrt{x^2 - 1}} = \operatorname{arcosh}\,x + \dfrac{x}{\sqrt{x^2 - 1}}.


6.1 Proof: ∫1x2−a2 dx=arcosh⁡ ⁣(xa)+C\int \frac{1}{\sqrt{x^2 - a^2}}\,dx = \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C

Section titled “6.1 Proof: ∫1x2−a2 dx=arcosh⁡ ⁣(xa)+C\int \frac{1}{\sqrt{x^2 - a^2}}\,dx = \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C∫x2−a2​1​dx=arcosh(ax​)+C”

Proof. Let u=x/au = x/a So dx=a dudx = a\,du:

∫dxx2−a2=∫a duau2−1=∫duu2−1\int \frac{dx}{\sqrt{x^2 - a^2}} = \int \frac{a\,du}{a\sqrt{u^2 - 1}} = \int \frac{du}{\sqrt{u^2 - 1}}

Now let u=cosh⁡tu = \cosh t So du=sinh⁡t dtdu = \sinh t\,dt:

=∫sinh⁡t dtcosh⁡2t−1=∫sinh⁡t dtsinh⁡t=∫1 dt=t+C=arcosh⁡ u+C= \int \frac{\sinh t\,dt}{\sqrt{\cosh^2 t - 1}} = \int \frac{\sinh t\,dt}{\sinh t} = \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: ∫1a2−x2 dx=1aartanh⁡ ⁣(xa)+C\int \frac{1}{a^2 - x^2}\,dx = \frac{1}{a}\operatorname{artanh}\!\left(\frac{x}{a}\right) + C

Section titled “6.2 Proof: ∫1a2−x2 dx=1aartanh⁡ ⁣(xa)+C\int \frac{1}{a^2 - x^2}\,dx = \frac{1}{a}\operatorname{artanh}\!\left(\frac{x}{a}\right) + C∫a2−x21​dx=a1​artanh(ax​)+C”

Proof. Let u=x/au = x/a So dx=a dudx = a\,du:

∫dxa2−x2=1a∫du1−u2=1aartanh⁡ u+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

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: Tcos⁡θ=T0T\cos\theta = T_0 (constant).

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

Since T=T0sec⁡θT = T_0\sec\theta and Tsin⁡θ=T0tan⁡θT\sin\theta = T_0\tan\theta:

ddx(T0tan⁡θ)=w  ⟹  T0sec⁡2θ dθdx=w\frac{d}{dx}(T_0\tan\theta) = w \implies T_0\sec^2\theta\,\frac{d\theta}{dx} = w

Let y′=tan⁡θy' = \tan\theta So dy′dx=sec⁡2θ dθdx=wT0\dfrac{dy'}{dx} = \sec^2\theta\,\dfrac{d\theta}{dx} = \dfrac{w}{T_0}.

Integrating: y′=wT0 x+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



(a) Solve the equation cosh⁡x=2.5\cosh x = 2.5 Giving your answer in exact logarithmic form.

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

Solution

(a) cosh⁡x=ex+e−x2=2.5\cosh x = \dfrac{e^x + e^{-x}}{2} = 2.5

ex+e−x=5  ⟹  e2x−5ex+1=0e^x + e^{-x} = 5 \implies e^{2x} - 5e^x + 1 = 0

ex=5±25−42=5±212e^x = \dfrac{5 \pm \sqrt{25 - 4}}{2} = \dfrac{5 \pm \sqrt{21}}{2}

x=ln⁡ ⁣(5±212)x = \ln\!\left(\dfrac{5 \pm \sqrt{21}}{2}\right)

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

(b) cosh⁡2x=2.5  ⟹  2x=ln⁡ ⁣(5±212)\cosh 2x = 2.5 \implies 2x = \ln\!\left(\dfrac{5 \pm \sqrt{21}}{2}\right)

x=12ln⁡ ⁣(5±212)x = \dfrac{1}{2}\ln\!\left(\dfrac{5 \pm \sqrt{21}}{2}\right)

Alternatively, using cosh⁡2x=2cosh⁡2x−1=2.5  ⟹  cosh⁡2x=1.75\cosh 2x = 2\cosh^2 x - 1 = 2.5 \implies \cosh^2 x = 1.75 Which gives the Same result.

(a) Prove that ddx(arcosh⁡ x)=1x2−1\dfrac{d}{dx}(\operatorname{arcosh}\,x) = \dfrac{1}{\sqrt{x^2 - 1}} for x>1x > 1.

(b) Evaluate ∫23dxx2−1\displaystyle\int_2^3 \frac{dx}{\sqrt{x^2 - 1}} in exact form.

Solution

(a) Let y=arcosh⁡ xy = \operatorname{arcosh}\,x So x=cosh⁡yx = \cosh y.

dxdy=sinh⁡y\dfrac{dx}{dy} = \sinh y So dydx=1sinh⁡y\dfrac{dy}{dx} = \dfrac{1}{\sinh y}.

Since cosh⁡2y−sinh⁡2y=1\cosh^2 y - \sinh^2 y = 1: sinh⁡y=cosh⁡2y−1=x2−1\sinh y = \sqrt{\cosh^2 y - 1} = \sqrt{x^2 - 1}.

dydx=1x2−1■\dfrac{dy}{dx} = \dfrac{1}{\sqrt{x^2 - 1}} \quad \blacksquare

(b) ∫23dxx2−1=[arcosh⁡ x]23\displaystyle\int_2^3 \frac{dx}{\sqrt{x^2 - 1}} = \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⁡ ⁣(3+222+3)= \ln\!\left(\dfrac{3 + 2\sqrt{2}}{2 + \sqrt{3}}\right).

A curve CC has equation y=sinh⁡−1(2x−1)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⁡(2x−1)y = \operatorname{arsinh}(2x - 1).

dydx=2(2x−1)2+1=24x2−4x+2\dfrac{dy}{dx} = \dfrac{2}{\sqrt{(2x - 1)^2 + 1}} = \dfrac{2}{\sqrt{4x^2 - 4x + 2}}.

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

dydx∣x=1=24−4+2=22=2\dfrac{dy}{dx}\bigg|_{x=1} = \dfrac{2}{\sqrt{4 - 4 + 2}} = \dfrac{2}{\sqrt{2}} = \sqrt{2}.

Equation of tangent: y−ln⁡(1+2)=2(x−1)y - \ln(1 + \sqrt{2}) = \sqrt{2}(x - 1) I.e.

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


Problem. Solve 3sinh⁡x+4cosh⁡x=53\sinh x + 4\cosh x = 5 Giving your answer in exact logarithmic form.

Solution. Using the exponential definitions:

3⋅ex−e−x2+4⋅ex+e−x2=53\cdot\frac{e^x - e^{-x}}{2} + 4\cdot\frac{e^x + e^{-x}}{2} = 5 3ex−3e−x+4ex+4e−x=103e^x - 3e^{-x} + 4e^x + 4e^{-x} = 10 7ex+e−x=107e^x + e^{-x} = 10

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

7e2x−10ex+1=07e^{2x} - 10e^x + 1 = 0

This is a quadratic in exe^x:

ex=10±100−2814=10±7214=10±6214=5±327e^x = \frac{10 \pm \sqrt{100 - 28}}{14} = \frac{10 \pm \sqrt{72}}{14} = \frac{10 \pm 6\sqrt{2}}{14} = \frac{5 \pm 3\sqrt{2}}{7} x=ln⁡ ⁣(5+327)orx=ln⁡ ⁣(5−327)x = \ln\!\left(\frac{5 + 3\sqrt{2}}{7}\right) \quad \text{or} \quad x = \ln\!\left(\frac{5 - 3\sqrt{2}}{7}\right)

Since 5−327≈0.109>0\dfrac{5 - 3\sqrt{2}}{7} \approx 0.109 > 0 Both solutions are valid.

Example 9.2: Integration using hyperbolic substitution

Section titled “Example 9.2: Integration using hyperbolic substitution”

Problem. Evaluate ∫x2−9 dx\displaystyle\int \sqrt{x^2 - 9}\,dx for x≥3x \geq 3.

Solution. Use the substitution x=3cosh⁡ux = 3\cosh u, dx=3sinh⁡u dudx = 3\sinh u\,du:

∫9cosh⁡2u−9⋅3sinh⁡u du=∫3sinh⁡u⋅3sinh⁡u du=9∫sinh⁡2u du\int \sqrt{9\cosh^2 u - 9}\cdot 3\sinh u\,du = \int 3\sinh u \cdot 3\sinh u\,du = 9\int \sinh^2 u\,du

Using sinh⁡2u=cosh⁡2u−12\sinh^2 u = \dfrac{\cosh 2u - 1}{2}:

=9∫cosh⁡2u−12 du=92(sinh⁡2u2−u)+C=94sinh⁡2u−92u+C= 9\int \frac{\cosh 2u - 1}{2}\,du = \frac{9}{2}\left(\frac{\sinh 2u}{2} - u\right) + C = \frac{9}{4}\sinh 2u - \frac{9}{2}u + C

Since x=3cosh⁡ux = 3\cosh u: cosh⁡u=x3\cosh u = \dfrac{x}{3} sinh⁡u=x29−1=x2−93\sinh u = \sqrt{\dfrac{x^2}{9} - 1} = \dfrac{\sqrt{x^2 - 9}}{3}.

sinh⁡2u=2sinh⁡ucosh⁡u=2xx2−99\sinh 2u = 2\sinh u\cosh u = \dfrac{2x\sqrt{x^2 - 9}}{9}.

u=arcosh⁡ ⁣(x3)=ln⁡ ⁣(x3+x29−1)u = \operatorname{arcosh}\!\left(\dfrac{x}{3}\right) = \ln\!\left(\dfrac{x}{3} + \sqrt{\dfrac{x^2}{9} - 1}\right).

=xx2−92−92arcosh⁡ ⁣(x3)+C= \frac{x\sqrt{x^2 - 9}}{2} - \frac{9}{2}\operatorname{arcosh}\!\left(\frac{x}{3}\right) + C

Example 9.3: Proving an identity using Osborne’s rule

Section titled “Example 9.3: Proving an identity using Osborne’s rule”

Problem. Prove that cosh⁡3x=4cosh⁡3x−3cosh⁡x\cosh 3x = 4\cosh^3 x - 3\cosh x.

Solution. From the trigonometric identity cos⁡3θ=4cos⁡3θ−3cos⁡θ\cos 3\theta = 4\cos^3\theta - 3\cos\theta Applying Osborne’s rule: since cos⁡3θ\cos^3\theta contains no products of sin⁡\sin It remains unchanged. Therefore:

cosh⁡3x=4cosh⁡3x−3cosh⁡x\cosh 3x = 4\cosh^3 x - 3\cosh x

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

=cosh⁡2xcosh⁡x+sinh⁡2xsinh⁡x=(2cosh⁡2x−1)cosh⁡x+2sinh⁡2xcosh⁡x= \cosh 2x\cosh x + \sinh 2x\sinh x = (2\cosh^2 x - 1)\cosh x + 2\sinh^2 x\cosh x =2cosh⁡3x−cosh⁡x+2(cosh⁡2x−1)cosh⁡x=2cosh⁡3x−cosh⁡x+2cosh⁡3x−2cosh⁡x= 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 =4cosh⁡3x−3cosh⁡x■= 4\cosh^3 x - 3\cosh x \quad \blacksquare

Example 9.4: Differentiation involving multiple hyperbolic functions

Section titled “Example 9.4: Differentiation involving multiple hyperbolic functions”

Problem. Find dydx\dfrac{dy}{dx} where y=sinh⁡x1+cosh⁡xy = \dfrac{\sinh x}{1 + \cosh x} and simplify Your answer.

Solution. Using the quotient rule:

dydx=cosh⁡x(1+cosh⁡x)−sinh⁡x⋅sinh⁡x(1+cosh⁡x)2=cosh⁡x+cosh⁡2x−sinh⁡2x(1+cosh⁡x)2\frac{dy}{dx} = \frac{\cosh x(1 + \cosh x) - \sinh x \cdot \sinh x}{(1 + \cosh x)^2} = \frac{\cosh x + \cosh^2 x - \sinh^2 x}{(1 + \cosh x)^2}

Using cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1:

=cosh⁡x+1(1+cosh⁡x)2=11+cosh⁡x=sech2 ⁣(x2)= \frac{\cosh x + 1}{(1 + \cosh x)^2} = \frac{1}{1 + \cosh x} = \mathrm{sech}^2\!\left(\frac{x}{2}\right)

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

Example 9.5: Definite integral with inverse hyperbolic functions

Section titled “Example 9.5: Definite integral with inverse hyperbolic functions”

Problem. Evaluate ∫01dx1+4x2\displaystyle\int_0^1 \frac{dx}{\sqrt{1 + 4x^2}}.

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}.

∫01dx1+4x2=12∫01dxx2+1/4=12[arsinh⁡ ⁣(x1/2)]01\int_0^1 \frac{dx}{\sqrt{1 + 4x^2}} = \frac{1}{2}\int_0^1 \frac{dx}{\sqrt{x^2 + 1/4}} = \frac{1}{2}\left[\operatorname{arsinh}\!\left(\frac{x}{1/2}\right)\right]_0^1 =12[arsinh⁡ 2−arsinh⁡ 0]=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

Section titled “Example 9.6: Parametric differentiation with hyperbolic functions”

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

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

dydx=3cosh⁡t2sinh⁡t=32coth⁡t\frac{dy}{dx} = \frac{3\cosh t}{2\sinh t} = \frac{3}{2}\coth t

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

dydx∣t=ln⁡2=3⋅5/42⋅3/4=15/43/2=52\frac{dy}{dx}\bigg|_{t = \ln 2} = \frac{3 \cdot 5/4}{2 \cdot 3/4} = \frac{15/4}{3/2} = \frac{5}{2}

Example 9.7: Verifying a reduction formula

Section titled “Example 9.7: Verifying a reduction formula”

Problem. Let In=∫0π/2cosh⁡n(sin⁡x) dxI_n = \displaystyle\int_0^{\pi/2} \cosh^n(\sin x)\,dx is not well-formed. Instead, verify that ∫tanh⁡3x dx=ln⁡(cosh⁡x)−12sech2 xtanh⁡x+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 ∫tanh⁡3x dx\displaystyle\int \tanh^3 x\,dx correctly.

Write tanh⁡3x=tanh⁡x⋅tanh⁡2x=tanh⁡x(1−sech2 x)=tanh⁡x−tanh⁡x sech2 x\tanh^3 x = \tanh x \cdot \tanh^2 x = \tanh x(1 - \mathrm{sech}^2\,x) = \tanh x - \tanh x\,\mathrm{sech}^2\,x.

∫tanh⁡3x dx=∫tanh⁡x dx−∫tanh⁡x sech2 x dx\int \tanh^3 x\,dx = \int \tanh x\,dx - \int \tanh x\,\mathrm{sech}^2\,x\,dx

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

For the second integral, let u=tanh⁡xu = \tanh x, du=sech2 x dxdu = \mathrm{sech}^2\,x\,dx:

∫u du=u22+C=tanh⁡2x2+C\int u\,du = \frac{u^2}{2} + C = \frac{\tanh^2 x}{2} + C

Therefore:

∫tanh⁡3x dx=ln⁡(cosh⁡x)−tanh⁡2x2+C\boxed{\int \tanh^3 x\,dx = \ln(\cosh x) - \frac{\tanh^2 x}{2} + C}

Example 9.8: Arc length of a hyperbolic cosine curve

Section titled “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=∫0b1+sinh⁡2(x/a) dx=∫0bcosh⁡(x/a) dx=[asinh⁡(x/a)]0b=asinh⁡(b/a)s = \int_0^b \sqrt{1 + \sinh^2(x/a)}\,dx = \int_0^b \cosh(x/a)\,dx = \bigl[a\sinh(x/a)\bigr]_0^b = a\sinh(b/a)

10.1 Hyperbolic functions and differential equations

Section titled “10.1 Hyperbolic functions and differential equations”

The differential equation d2ydx2−y=0\dfrac{d^2y}{dx^2} - y = 0 has general solution y=Acosh⁡x+Bsinh⁡xy = A\cosh x + B\sinh x Which can also be written y=Cex+De−xy = Ce^x + De^{-x}. See Differential Equations.

10.2 Hyperbolic functions and complex numbers

Section titled “10.2 Hyperbolic functions and complex numbers”

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

10.3 Hyperbolic functions and integration techniques

Section titled “10.3 Hyperbolic functions and integration techniques”

Hyperbolic substitutions (x=asinh⁡ux = a\sinh u, x=acosh⁡ux = a\cosh u) are powerful alternatives to trigonometric Substitutions. See Further Calculus.

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.


(a) Given sinh⁡x=125\sinh x = \dfrac{12}{5} Find the exact value of cosh⁡x\cosh x and tanh⁡x\tanh x.

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

Solution

(a) cosh⁡2x=1+sinh⁡2x=1+14425=16925\cosh^2 x = 1 + \sinh^2 x = 1 + \dfrac{144}{25} = \dfrac{169}{25} So cosh⁡x=135\cosh x = \dfrac{13}{5} (positive root).

tanh⁡x=sinh⁡xcosh⁡x=12/513/5=1213\tanh x = \dfrac{\sinh x}{\cosh x} = \dfrac{12/5}{13/5} = \dfrac{12}{13}.

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

arcosh⁡ ⁣(135)=x=ln⁡ ⁣(135+16925−1)=ln⁡ ⁣(135+125)=ln⁡5\operatorname{arcosh}\!\left(\frac{13}{5}\right) = x = \ln\!\left(\frac{13}{5} + \sqrt{\frac{169}{25} - 1}\right) = \ln\!\left(\frac{13}{5} + \frac{12}{5}\right) = \ln 5

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

Solution∫0ln⁡2cosh⁡2x dx=[sinh⁡2x2]0ln⁡2=sinh⁡(2ln⁡2)2\int_0^{\ln 2}\cosh 2x\,dx = \left[\frac{\sinh 2x}{2}\right]_0^{\ln 2} = \frac{\sinh(2\ln 2)}{2}

sinh⁡(2ln⁡2)=e2ln⁡2−e−2ln⁡22=4−1/42=158\sinh(2\ln 2) = \dfrac{e^{2\ln 2} - e^{-2\ln 2}}{2} = \dfrac{4 - 1/4}{2} = \dfrac{15}{8}.

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

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

Solution

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

Base case (n=1n = 1): ddx(sinh⁡x)=cosh⁡x\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(sinh⁡x)=sinh⁡x\dfrac{d^k}{dx^k}(\sinh x) = \sinh x. Then dk+1dxk+1(sinh⁡x)=ddx(sinh⁡x)=cosh⁡x\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(sinh⁡x)=cosh⁡x\dfrac{d^k}{dx^k}(\sinh x) = \cosh x. Then dk+1dxk+1(sinh⁡x)=ddx(cosh⁡x)=sinh⁡x\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

Evaluate ∫3/2234x2−9 dx\displaystyle\int_{3/2}^2 \frac{3}{\sqrt{4x^2 - 9}}\,dx in exact form.

Solution∫3/2234x2−9 dx=32∫3/22dxx2−9/4=32[arcosh⁡ ⁣(2x3)]3/22\int_{3/2}^2 \frac{3}{\sqrt{4x^2 - 9}}\,dx = \frac{3}{2}\int_{3/2}^2 \frac{dx}{\sqrt{x^2 - 9/4}} = \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+169−1)=32ln⁡ ⁣(4+73)= \frac{3}{2}\ln\!\left(\frac{4}{3} + \sqrt{\frac{16}{9} - 1}\right) = \frac{3}{2}\ln\!\left(\frac{4 + \sqrt{7}}{3}\right)

Given that y=ln⁡(sinh⁡x)y = \ln(\sinh x) Show that d2ydx2=−cosech2 x\dfrac{d^2y}{dx^2} = -\mathrm{cosech}^2\,x.

Solutiondydx=cosh⁡xsinh⁡x=coth⁡x\frac{dy}{dx} = \frac{\cosh x}{\sinh x} = \coth x d2ydx2=ddx(coth⁡x)=−cosech2 x=−1sinh⁡2x■\frac{d^2y}{dx^2} = \frac{d}{dx}(\coth x) = -\mathrm{cosech}^2\,x = \frac{-1}{\sinh^2 x} \quad \blacksquare

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

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

Solution

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

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

sinh⁡(2ln⁡3)=2⋅43⋅53=409\sinh(2\ln 3) = 2 \cdot \dfrac{4}{3} \cdot \dfrac{5}{3} = \dfrac{40}{9}.

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

arsinh⁡ ⁣(34)=ln⁡ ⁣(34+916+1)=ln⁡ ⁣(34+54)=ln⁡2\operatorname{arsinh}\!\left(\dfrac{3}{4}\right) = \ln\!\left(\dfrac{3}{4} + \sqrt{\dfrac{9}{16}+1}\right) = \ln\!\left(\dfrac{3}{4} + \dfrac{5}{4}\right) = \ln 2.

Therefore ln⁡2=arsinh⁡(3/4)\ln 2 = \operatorname{arsinh}(3/4) and ln⁡3=ln⁡2+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 ln⁡3−ln⁡2=artanh⁡(1/5)\ln 3 - \ln 2 = \operatorname{artanh}(1/5).


IdentityFormula
Triple anglesinh⁡3x=3sinh⁡x+4sinh⁡3x\sinh 3x = 3\sinh x + 4\sinh^3 x
Triple anglecosh⁡3x=4cosh⁡3x−3cosh⁡x\cosh 3x = 4\cosh^3 x - 3\cosh x
Half anglecosh⁡2 ⁣(x2)=1+cosh⁡x2\cosh^2\!\left(\dfrac{x}{2}\right) = \dfrac{1 + \cosh x}{2}
Half anglesinh⁡2 ⁣(x2)=cosh⁡x−12\sinh^2\!\left(\dfrac{x}{2}\right) = \dfrac{\cosh x - 1}{2}
Integral of tanh⁡\tanh∫tanh⁡x dx=ln⁡(cosh⁡x)+C\displaystyle\int\tanh x\,dx = \ln(\cosh x) + C
Integral of coth⁡\coth∫coth⁡x dx=ln⁡(sinh⁡x)+C\displaystyle\int\coth x\,dx = \ln(\sinh x) + C
Integral of tanh⁡3\tanh^3∫tanh⁡3x dx=ln⁡(cosh⁡x)−tanh⁡2x2+C\displaystyle\int\tanh^3 x\,dx = \ln(\cosh x) - \dfrac{\tanh^2 x}{2} + C
Arc length of catenarys=asinh⁡(b/a)s = a\sinh(b/a) for y=acosh⁡(x/a)y = a\cosh(x/a)


Example 14.1: Integration using sinh⁡\sinh substitution

Section titled “Example 14.1: Integration using sinh⁡\sinhsinh substitution”

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

Solution. Let x=3sinh⁡ux = 3\sinh u, dx=3cosh⁡u dudx = 3\cosh u\,du.

∫3cosh⁡u⋅3cosh⁡u du=9∫cosh⁡2u du=9∫1+cosh⁡2u2 du=92 ⁣(u+sinh⁡2u2)\int 3\cosh u \cdot 3\cosh u\,du = 9\int \cosh^2 u\,du = 9\int \frac{1+\cosh 2u}{2}\,du = \frac{9}{2}\!\left(u + \frac{\sinh 2u}{2}\right) =9u2+9sinh⁡ucosh⁡u2=92arsinh⁡ ⁣(x3)+xx2+92+C= \frac{9u}{2} + \frac{9\sinh u\cosh u}{2} = \frac{9}{2}\operatorname{arsinh}\!\left(\frac{x}{3}\right) + \frac{x\sqrt{x^2+9}}{2} + C

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

Section titled “Example 14.2: Solving y′′−4y=0y'' - 4y = 0y′′−4y=0 with hyperbolic functions”

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

Solution. Auxiliary: m2−4=0  ⟹  m=±2m^2 - 4 = 0 \implies m = \pm 2.

y=Acosh⁡2x+Bsinh⁡2xy = 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=3cosh⁡2x+4sinh⁡2x\boxed{y = 3\cosh 2x + 4\sinh 2x}

In exponential form: y=3⋅e2x+e−2x2+4⋅e2x−e−2x2=72e2x−12e−2xy = 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}.

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

Solution. y′=sinh⁡xy' = \sinh x. ds=1+sinh⁡2x dx=cosh⁡x dxds = \sqrt{1 + \sinh^2 x}\,dx = \cosh x\,dx.

s=∫01cosh⁡x dx=[sinh⁡x]01=sinh⁡1=e−e−12≈1.175s = \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 tan⁡2x\tan 2x

Section titled “Example 14.4: Osborn’s rule applied to tan⁡2x\tan 2xtan2x”

Problem. Using Osborn’s rule, find tanh⁡2x\tanh 2x in terms of tanh⁡x\tanh x.

Solution. tan⁡2x=2tan⁡x1−tan⁡2x\tan 2x = \dfrac{2\tan x}{1-\tan^2 x}. Apply Osborn’s rule (change tan⁡2x\tan^2 x to −tanh⁡2x-\tanh^2 x):

tanh⁡2x=2tanh⁡x1+tanh⁡2x\boxed{\tanh 2x = \frac{2\tanh x}{1+\tanh^2 x}}

Example 14.5: Deriving the Gudermannian function relationship

Section titled “Example 14.5: Deriving the Gudermannian function relationship”

Problem. The Gudermannian function relates circular and hyperbolic functions: sec⁡θ=cosh⁡u\sec\theta = \cosh u where u=gd⁡−1(θ)u = \operatorname{gd}^{-1}(\theta). Show that dθdu=sech⁡ u\dfrac{d\theta}{du} = \operatorname{sech}\, u.

Solution. sec⁡θ=cosh⁡u  ⟹  cos⁡θ=sech⁡ u\sec\theta = \cosh u \implies \cos\theta = \operatorname{sech}\, u.

Differentiating implicitly with respect to uu: −sin⁡θ⋅dθdu=−sech⁡ utanh⁡u-\sin\theta \cdot \dfrac{d\theta}{du} = -\operatorname{sech}\,u \tanh u.

dθdu=sech⁡ utanh⁡usin⁡θ\dfrac{d\theta}{du} = \dfrac{\operatorname{sech}\,u \tanh u}{\sin\theta}.

Since cos⁡θ=sech⁡ u\cos\theta = \operatorname{sech}\,u: sin⁡θ=1−sech⁡2u=1−1cosh⁡2u=cosh⁡2u−1cosh⁡u=sinh⁡ucosh⁡u=tanh⁡u\sin\theta = \sqrt{1-\operatorname{sech}^2 u} = \sqrt{1-\dfrac{1}{\cosh^2 u}} = \dfrac{\sqrt{\cosh^2 u - 1}}{\cosh u} = \dfrac{\sinh u}{\cosh u} = \tanh u.

dθdu=sech⁡ utanh⁡utanh⁡u=sech⁡ u\dfrac{d\theta}{du} = \dfrac{\operatorname{sech}\,u \tanh u}{\tanh u} = \boxed{\operatorname{sech}\,u}. ■\blacksquare


Evaluate ∫12dxx2−1\displaystyle\int_1^2 \frac{dx}{\sqrt{x^2 - 1}}.

Solution

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

Prove that sinh⁡(x+y)=sinh⁡xcosh⁡y+cosh⁡xsinh⁡y\sinh(x+y) = \sinh x\cosh y + \cosh x\sinh y.

Solution

sinh⁡xcosh⁡y+cosh⁡xsinh⁡y=(ex−e−x)(ey+e−y)+(ex+e−x)(ey−e−y)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+ex−y−e−x+y−e−x−y+ex+y−ex−y+e−x+y−e−x−y4= \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+y−2e−(x+y)4=ex+y−e−(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

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

Solution

Let y=arcosh⁡ xy = \operatorname{arcosh}\, x So x=cosh⁡yx = \cosh y and x≥1x \geq 1.

1=sinh⁡y⋅dydx1 = \sinh y \cdot \dfrac{dy}{dx}.

dydx=1sinh⁡y=1cosh⁡2y−1=1x2−1\dfrac{dy}{dx} = \dfrac{1}{\sinh y} = \dfrac{1}{\sqrt{\cosh^2 y - 1}} = \dfrac{1}{\sqrt{x^2-1}}.

ddx[arcosh⁡ x]=1x2−1\boxed{\dfrac{d}{dx}[\operatorname{arcosh}\, x] = \dfrac{1}{\sqrt{x^2-1}}} for x>1x > 1.


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

sin⁡(gd x)=tanh⁡x\sin(\mathrm{gd}\,x) = \tanh x, cos⁡(gd x)=sech x\cos(\mathrm{gd}\,x) = \mathrm{sech}\,x tan⁡(gd x)=sinh⁡x\tan(\mathrm{gd}\,x) = \sinh x.

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

16.2 Hyperbolic functions and the Lorentz transformation

Section titled “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=(1−β2)−1/2=cosh⁡ϕ\gamma = (1-\beta^2)^{-1/2} = \cosh\phi where tanh⁡ϕ=β\tanh\phi = \beta Then:

t′=tcosh⁡ϕ−xsinh⁡ϕ/ct' = t\cosh\phi - x\sinh\phi/c, x′=xcosh⁡ϕ−ctsinh⁡ϕx' = x\cosh\phi - ct\sinh\phi.

16.3 Inverse hyperbolic functions in logarithmic form

Section titled “16.3 Inverse hyperbolic functions in logarithmic form”
FunctionLogarithmic FormDomain
arsinh⁡ x\operatorname{arsinh}\,xln⁡(x+x2+1)\ln(x+\sqrt{x^2+1})all real xx
arcosh⁡ x\operatorname{arcosh}\,xln⁡(x+x2−1)\ln(x+\sqrt{x^2-1})x≥1x \geq 1
artanh⁡ x\operatorname{artanh}\,x12ln⁡ ⁣(1+x1−x)\dfrac{1}{2}\ln\!\left(\dfrac{1+x}{1-x}\right)∥x∥<1\| x \| < 1
arcoth⁡ x\operatorname{arcoth}\,x12ln⁡ ⁣(x+1x−1)\dfrac{1}{2}\ln\!\left(\dfrac{x+1}{x-1}\right)∥x∥>1\| x \| > 1
arsech⁡ x\operatorname{arsech}\,xln⁡ ⁣(1+1−x2x)\ln\!\left(\dfrac{1+\sqrt{1-x^2}}{x}\right)0<x≤10 < x \leq 1
arcsch⁡ x\operatorname{arcsch}\,xln⁡ ⁣(1x+1x2+1)\ln\!\left(\dfrac{1}{x}+\sqrt{\dfrac{1}{x^2}+1}\right)x≠0x \neq 0

16.4 Hyperbolic functions and catenary applications

Section titled “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

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

Solution

2⋅ex+e−x2−ex−e−x2=32\cdot\dfrac{e^x+e^{-x}}{2} - \dfrac{e^x-e^{-x}}{2} = 3.

ex+e−x−ex2+e−x2=3e^x+e^{-x} - \dfrac{e^x}{2} + \dfrac{e^{-x}}{2} = 3.

ex2+3e−x2=3  ⟹  ex+3e−x=6\dfrac{e^x}{2} + \dfrac{3e^{-x}}{2} = 3 \implies e^x + 3e^{-x} = 6.

e2x−6ex+3=0e^{2x} - 6e^x + 3 = 0.

ex=6±36−122=3±6e^x = \dfrac{6 \pm \sqrt{36-12}}{2} = 3 \pm \sqrt{6}.

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

Since 3−6>03-\sqrt{6} > 0 Both are valid.

Prove that arcosh⁡ x=ln⁡(x+x2−1)\operatorname{arcosh}\,x = \ln(x+\sqrt{x^2-1}) for x≥1x \geq 1.

Solution

Let y=arcosh⁡ xy = \operatorname{arcosh}\,x So x=cosh⁡y=ey+e−y2x = \cosh y = \dfrac{e^y+e^{-y}}{2}.

2x=ey+e−y  ⟹  e2y−2xey+1=02x = e^y + e^{-y} \implies e^{2y} - 2xe^y + 1 = 0.

ey=2x±4x2−42=x±x2−1e^y = \dfrac{2x \pm \sqrt{4x^2-4}}{2} = x \pm \sqrt{x^2-1}.

Since ey≥1e^y \geq 1 and x≥1x \geq 1: ey=x+x2−1e^y = x + \sqrt{x^2-1} (the positive root, since x−x2−1≤1x-\sqrt{x^2-1} \leq 1).

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


17.1 Hyperbolic substitutions in integration

Section titled “17.1 Hyperbolic substitutions in integration”

Standard substitutions:

  • x2+a2\sqrt{x^2+a^2}: use x=acosh⁡tx = a\cosh t
  • x2−a2\sqrt{x^2-a^2}: use x=acosh⁡tx = a\cosh t (for x≥ax \geq a)
  • a2−x2\sqrt{a^2-x^2}: use x=acos⁡tx = a\cos t (circular, not hyperbolic)

Example: ∫dxx2−4\displaystyle\int \frac{dx}{\sqrt{x^2-4}} with x=2cosh⁡tx = 2\cosh t:

dx=2sinh⁡t dtdx = 2\sinh t\,dt, x2−4=2sinh⁡t\sqrt{x^2-4} = 2\sinh t.

∫2sinh⁡t2sinh⁡t dt=t=arcosh⁡ ⁣(x2)+C\displaystyle\int \frac{2\sinh t}{2\sinh t}\,dt = t = \operatorname{arcosh}\!\left(\frac{x}{2}\right) + C.

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

gd⁡(x)=∫0xsech⁡t dt=2arctan⁡(ex)−π2\operatorname{gd}(x) = \int_0^x \operatorname{sech} t\,dt = 2\arctan(e^x) - \frac{\pi}{2}

Key identities:

  • sin⁡(gd⁡ x)=tanh⁡x\sin(\operatorname{gd}\,x) = \tanh x
  • cos⁡(gd⁡ x)=sech⁡x\cos(\operatorname{gd}\,x) = \operatorname{sech} x
  • tan⁡(gd⁡ x)=sinh⁡x\tan(\operatorname{gd}\,x) = \sinh x

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).


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

Solution

Let y=arsinh⁡ xy = \operatorname{arsinh}\,x So x=sinh⁡y=ey−e−y2x = \sinh y = \dfrac{e^y-e^{-y}}{2}.

2x=ey−e−y  ⟹  e2y−2xey−1=02x = e^y - e^{-y} \implies e^{2y} - 2xe^y - 1 = 0.

ey=2x+4x2+42=x+x2+1e^y = \dfrac{2x + \sqrt{4x^2+4}}{2} = 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

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

Solution

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

=∫0arsinh⁡(4/3)9cosh⁡2t dt=92∫0arsinh⁡(4/3)(1+cosh⁡2t) 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+sinh⁡2t2]0arsinh⁡(4/3)= \frac{9}{2}\!\left[t + \frac{\sinh 2t}{2}\right]_0^{\operatorname{arsinh}(4/3)}.

At t=arsinh⁡(4/3)t = \operatorname{arsinh}(4/3): sinh⁡t=4/3\sinh t = 4/3, cosh⁡t=5/3\cosh t = 5/3 sinh⁡2t=2⋅43⋅53=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}.