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 sinh x = e x − e − x 2 \sinh x = \frac{e^x - e^{-x}}{2} sinh x = 2 e x − e − x
cosh x = e x + e − x 2 \cosh x = \frac{e^x + e^{-x}}{2} cosh x = 2 e x + e − x
tanh x = ◆ L B ◆ sinh x ◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = e x − e − x e x + e − x \tanh x = \frac◆LB◆\sinh x◆RB◆◆LB◆\cosh x◆RB◆ = \frac{e^x - e^{-x}}{e^x + e^{-x}} tanh x = L ◆ B ◆ sinh x ◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = e x + e − x e x − e − x
1.2 Reciprocal functions c o s e c h x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ sinh x ◆ R B ◆ = 2 e x − e − x , x ≠ 0 \mathrm{cosech}\,x = \frac◆LB◆1◆RB◆◆LB◆\sinh x◆RB◆ = \frac{2}{e^x - e^{-x}}, \quad x \neq 0 cosech x = L ◆ B ◆1◆ R B ◆◆ L B ◆ sinh x ◆ R B ◆ = e x − e − x 2 , x = 0
s e c h x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = 2 e x + e − x \mathrm{sech}\,x = \frac◆LB◆1◆RB◆◆LB◆\cosh x◆RB◆ = \frac{2}{e^x + e^{-x}} sech x = L ◆ B ◆1◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = e x + e − x 2
coth x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ tanh x ◆ R B ◆ = e x + e − x e x − e − x , x ≠ 0 \coth x = \frac◆LB◆1◆RB◆◆LB◆\tanh x◆RB◆ = \frac{e^x + e^{-x}}{e^x - e^{-x}}, \quad x \neq 0 coth x = L ◆ B ◆1◆ R B ◆◆ L B ◆ tanh x ◆ R B ◆ = e x − e − x e x + e − x , x = 0
1.3 Basic properties
sinh 0 = 0 \sinh 0 = 0 sinh 0 = 0 , cosh 0 = 1 \cosh 0 = 1 cosh 0 = 1 , tanh 0 = 0 \tanh 0 = 0 tanh 0 = 0 .
sinh x \sinh x sinh x is odd : sinh ( − x ) = − sinh x \sinh(-x) = -\sinh x sinh ( − x ) = − sinh x .
cosh x \cosh x cosh x is even : cosh ( − x ) = cosh x \cosh(-x) = \cosh x cosh ( − x ) = cosh x .
tanh x \tanh x tanh x is odd .
As x → + ∞ x \to +\infty x → + ∞ : sinh x → + ∞ \sinh x \to +\infty sinh x → + ∞ , cosh x → + ∞ \cosh x \to +\infty cosh x → + ∞ , tanh x → 1 \tanh x \to 1 tanh x → 1 .
As x → − ∞ x \to -\infty x → − ∞ : sinh x → − ∞ \sinh x \to -\infty sinh x → − ∞ , cosh x → + ∞ \cosh x \to +\infty cosh x → + ∞ , tanh x → − 1 \tanh x \to -1 tanh x → − 1 .
cosh x = cos ( i x ) , sinh x = − i sin ( i x ) \cosh x = \cos(ix), \qquad \sinh x = -i\sin(ix) cosh x = cos ( i x ) , sinh x = − i sin ( i x )
Proof. cos ( i x ) = e i ( i x ) + e − i ( i x ) 2 = e − x + e x 2 = cosh x \cos(ix) = \dfrac{e^{i(ix)} + e^{-i(ix)}}{2} = \dfrac{e^{-x} + e^{x}}{2} = \cosh x cos ( i x ) = 2 e i ( i x ) + e − i ( i x ) = 2 e − x + e x = cosh x .
− i sin ( i x ) = − i ⋅ e i ( i x ) − e − i ( i x ) 2 i = e − x − e x − 2 = e x − e − x 2 = 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 − i sin ( i x ) = − i ⋅ 2 i e i ( i x ) − e − i ( i x ) = − 2 e − x − e x = 2 e x − e − x = sinh x .
■ \blacksquare ■
1.5 Graphs
sinh x \sinh x sinh x : passes through the origin, increasing, resembles y = x / 2 y = x/2 y = x /2 near the origin and
y = e x / 2 y = e^x/2 y = e x /2 for large positive x x x .
cosh x \cosh x cosh x : minimum at ( 0 , 1 ) (0, 1) ( 0 , 1 ) , symmetric about the y y y -axis, resembles y = 1 + x 2 / 2 y = 1 + x^2/2 y = 1 + x 2 /2 near
the origin and y = e x / 2 y = e^x/2 y = e x /2 for large positive x x x .
tanh x \tanh x tanh x : S-shaped curve with horizontal asymptotes at y = ± 1 y = \pm 1 y = ± 1 , passing through the
origin with gradient 1.
2. Hyperbolic Identities 2.1 Fundamental identity cosh 2 x − sinh 2 x = 1 \boxed{\cosh^2 x - \sinh^2 x = 1} cosh 2 x − sinh 2 x = 1
Proof.
cosh 2 x − sinh 2 x = ( e x + e − x ) 2 4 − ( e x − e − x ) 2 4 \cosh^2 x - \sinh^2 x = \frac{(e^x + e^{-x})^2}{4} - \frac{(e^x - e^{-x})^2}{4} cosh 2 x − sinh 2 x = 4 ( e x + e − x ) 2 − 4 ( e x − e − x ) 2
= e 2 x + 2 + e − 2 x − ( e 2 x − 2 + e − 2 x ) 4 = 4 4 = 1 ■ = \frac{e^{2x} + 2 + e^{-2x} - (e^{2x} - 2 + e^{-2x})}{4} = \frac{4}{4} = 1 \quad \blacksquare = 4 e 2 x + 2 + e − 2 x − ( e 2 x − 2 + e − 2 x ) = 4 4 = 1 ■
2.2 Identity for tanh \tanh tanh 1 − tanh 2 x = s e c h 2 x \boxed{1 - \tanh^2 x = \mathrm{sech}^2\,x} 1 − tanh 2 x = sech 2 x
Proof. Divide the fundamental identity by cosh 2 x \cosh^2 x cosh 2 x :
1 − tanh 2 x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ cosh 2 x ◆ R B ◆ = s e c h 2 x ■ 1 - \tanh^2 x = \frac◆LB◆1◆RB◆◆LB◆\cosh^2 x◆RB◆ = \mathrm{sech}^2\,x \quad \blacksquare 1 − tanh 2 x = L ◆ B ◆1◆ R B ◆◆ L B ◆ cosh 2 x ◆ R B ◆ = sech 2 x ■
2.3 Osborne's rule Every trigonometric identity has a corresponding hyperbolic identity, obtained by:
Replacing cos \cos cos with cosh \cosh cosh .
Replacing sin \sin sin with sinh \sinh sinh .
Negating every product (or power of 2 or more) of sinh \sinh sinh .
Example: cos 2 x + sin 2 x = 1 \cos^2 x + \sin^2 x = 1 cos 2 x + sin 2 x = 1 becomes cosh 2 x − sinh 2 x = 1 \cosh^2 x - \sinh^2 x = 1 cosh 2 x − sinh 2 x = 1 (the sinh 2 \sinh^2 sinh 2 term is
negated).
Example: sin 2 x = 2 sin x cos x \sin 2x = 2\sin x\cos x sin 2 x = 2 sin x cos x becomes sinh 2 x = 2 sinh x cosh x \sinh 2x = 2\sinh x\cosh x sinh 2 x = 2 sinh x cosh x (the product
sinh x cosh x \sinh x \cosh x sinh x cosh x is negated since it contains sinh \sinh sinh , but sinh 2 x \sinh 2x sinh 2 x on the left is not a product,
so the overall sign changes on both sides cancel).
sinh 2 x = 2 sinh x cosh x \sinh 2x = 2\sinh x\cosh x sinh 2 x = 2 sinh x cosh x
cosh 2 x = cosh 2 x + sinh 2 x = 2 cosh 2 x − 1 = 1 + 2 sinh 2 x \cosh 2x = \cosh^2 x + \sinh^2 x = 2\cosh^2 x - 1 = 1 + 2\sinh^2 x cosh 2 x = cosh 2 x + sinh 2 x = 2 cosh 2 x − 1 = 1 + 2 sinh 2 x
Proof of cosh 2 x = 2 cosh 2 x − 1 \cosh 2x = 2\cosh^2 x - 1 cosh 2 x = 2 cosh 2 x − 1 :
cosh 2 x = e 2 x + e − 2 x 2 = ( e x + e − x ) 2 − 2 2 = ◆ L B ◆ 4 cosh 2 x − 2 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = 2 cosh 2 x − 1 ■ \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 cosh 2 x = 2 e 2 x + e − 2 x = 2 ( e x + e − x ) 2 − 2 = L ◆ B ◆4 cosh 2 x − 2◆ R B ◆◆ L B ◆2◆ R B ◆ = 2 cosh 2 x − 1 ■
sinh ( A ± B ) = sinh A cosh B ± cosh A sinh B \sinh(A \pm B) = \sinh A\cosh B \pm \cosh A\sinh B sinh ( A ± B ) = sinh A cosh B ± cosh A sinh B
cosh ( A ± B ) = cosh A cosh B ± sinh A sinh B \cosh(A \pm B) = \cosh A\cosh B \pm \sinh A\sinh B cosh ( A ± B ) = cosh A cosh B ± sinh A sinh B
Proof of the addition formula for sinh \sinh sinh :
sinh ( A + B ) = e A + B − e − ( A + B ) 2 = e A e B − e − A e − B 2 \sinh(A + B) = \frac{e^{A+B} - e^{-(A+B)}}{2} = \frac{e^A e^B - e^{-A}e^{-B}}{2} sinh ( A + B ) = 2 e A + B − e − ( A + B ) = 2 e A e B − e − A e − B
= ( e A − e − A ) ( e B + e − B ) + ( e A + e − A ) ( e B − e − B ) 4 = \frac{(e^A - e^{-A})(e^B + e^{-B}) + (e^A + e^{-A})(e^B - e^{-B})}{4} = 4 ( e A − e − A ) ( e B + e − B ) + ( e A + e − A ) ( e B − e − B )
= sinh A cosh B + cosh A sinh B ■ = \sinh A\cosh B + \cosh A\sinh B \quad \blacksquare = sinh A cosh B + cosh A sinh B ■
2.6 Worked example Problem. Given sinh x = 3 \sinh x = 3 sinh x = 3 , find cosh x \cosh x cosh x and tanh x \tanh x tanh x without finding x x x .
From cosh 2 x − sinh 2 x = 1 \cosh^2 x - \sinh^2 x = 1 cosh 2 x − sinh 2 x = 1 :
cosh 2 x = 1 + 9 = 10 ⟹ cosh x = 10 \cosh^2 x = 1 + 9 = 10 \implies \cosh x = \sqrt{10} cosh 2 x = 1 + 9 = 10 ⟹ cosh x = 10
(We take the positive root since cosh x ≥ 1 \cosh x \geq 1 cosh x ≥ 1 for all x x x .)
tanh x = ◆ L B ◆ sinh x ◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = ◆ L B ◆ 3 ◆ R B ◆◆ L B ◆ 10 ◆ R B ◆ = ◆ L B ◆ 3 10 ◆ R B ◆◆ L B ◆ 10 ◆ R B ◆ \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◆ tanh x = L ◆ B ◆ sinh x ◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = L ◆ B ◆3◆ R B ◆◆ L B ◆ 10 ◆ R B ◆ = L ◆ B ◆3 10 ◆ R B ◆◆ L B ◆10◆ R B ◆
3. Inverse Hyperbolic Functions arsinh x = ln ( x + x 2 + 1 ) , x ∈ R \operatorname{arsinh}\,x = \ln\!\left(x + \sqrt{x^2 + 1}\right), \quad x \in \mathbb{R} arsinh x = ln ( x + x 2 + 1 ) , x ∈ R
arcosh x = ln ( x + x 2 − 1 ) , x ≥ 1 \operatorname{arcosh}\,x = \ln\!\left(x + \sqrt{x^2 - 1}\right), \quad x \geq 1 arcosh x = ln ( x + x 2 − 1 ) , x ≥ 1
artanh x = 1 2 ln ( 1 + x 1 − x ) , − 1 < x < 1 \operatorname{artanh}\,x = \frac{1}{2}\ln\!\left(\frac{1 + x}{1 - x}\right), \quad -1 \lt x \lt 1 artanh x = 2 1 ln ( 1 − x 1 + x ) , − 1 < x < 1
3.2 Derivation of arsinh x = ln ( x + x 2 + 1 ) \operatorname{arsinh}\,x = \ln(x + \sqrt{x^2 + 1}) arsinh x = ln ( x + x 2 + 1 ) Let y = arsinh x y = \operatorname{arsinh}\,x y = arsinh x , so x = sinh y = e y − e − y 2 x = \sinh y = \dfrac{e^y - e^{-y}}{2} x = sinh y = 2 e y − e − y .
2 x = e y − e − y ⟹ e 2 y − 2 x e y − 1 = 0 2x = e^y - e^{-y} \implies e^{2y} - 2xe^y - 1 = 0 2 x = e y − e − y ⟹ e 2 y − 2 x e y − 1 = 0
This is a quadratic in e y e^y e y :
e y = ◆ L B ◆ 2 x ± 4 x 2 + 4 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = x ± x 2 + 1 e^y = \frac◆LB◆2x \pm \sqrt{4x^2 + 4}◆RB◆◆LB◆2◆RB◆ = x \pm \sqrt{x^2 + 1} e y = L ◆ B ◆2 x ± 4 x 2 + 4 ◆ R B ◆◆ L B ◆2◆ R B ◆ = x ± x 2 + 1
Since e y > 0 e^y \gt 0 e y > 0 and x 2 + 1 > ∣ x ∣ \sqrt{x^2 + 1} \gt |x| x 2 + 1 > ∣ x ∣ , we take the positive root:
e y = x + x 2 + 1 ⟹ y = ln ( x + x 2 + 1 ) ■ e^y = x + \sqrt{x^2 + 1} \implies y = \ln\!\left(x + \sqrt{x^2 + 1}\right) \quad \blacksquare e y = x + x 2 + 1 ⟹ y = ln ( x + x 2 + 1 ) ■
3.3 Derivation of arcosh x = ln ( x + x 2 − 1 ) \operatorname{arcosh}\,x = \ln(x + \sqrt{x^2 - 1}) arcosh x = ln ( x + x 2 − 1 ) Let y = arcosh x y = \operatorname{arcosh}\,x y = arcosh x , so x = cosh y = e y + e − y 2 x = \cosh y = \dfrac{e^y + e^{-y}}{2} x = cosh y = 2 e y + e − y .
2 x = e y + e − y ⟹ e 2 y − 2 x e y + 1 = 0 2x = e^y + e^{-y} \implies e^{2y} - 2xe^y + 1 = 0 2 x = e y + e − y ⟹ e 2 y − 2 x e y + 1 = 0
e y = ◆ L B ◆ 2 x ± 4 x 2 − 4 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = x ± x 2 − 1 e^y = \frac◆LB◆2x \pm \sqrt{4x^2 - 4}◆RB◆◆LB◆2◆RB◆ = x \pm \sqrt{x^2 - 1} e y = L ◆ B ◆2 x ± 4 x 2 − 4 ◆ R B ◆◆ L B ◆2◆ R B ◆ = x ± x 2 − 1
Since e y ≥ 1 e^y \geq 1 e y ≥ 1 and x ≥ 1 x \geq 1 x ≥ 1 , we need e y ≥ 1 e^y \geq 1 e y ≥ 1 . Both roots are positive when x ≥ 1 x \geq 1 x ≥ 1 .
The convention is to take e y = x + x 2 − 1 e^y = x + \sqrt{x^2 - 1} e y = x + x 2 − 1 (which gives y ≥ 0 y \geq 0 y ≥ 0 ):
y = ln ( x + x 2 − 1 ) ■ y = \ln\!\left(x + \sqrt{x^2 - 1}\right) \quad \blacksquare y = ln ( x + x 2 − 1 ) ■
3.4 Derivation of artanh x \operatorname{artanh}\,x artanh x Let y = artanh x y = \operatorname{artanh}\,x y = artanh x , so x = tanh y x = \tanh y x = tanh y .
x = e y − e − y e y + e − y = e 2 y − 1 e 2 y + 1 x = \frac{e^y - e^{-y}}{e^y + e^{-y}} = \frac{e^{2y} - 1}{e^{2y} + 1} x = e y + e − y e y − e − y = e 2 y + 1 e 2 y − 1
x ( e 2 y + 1 ) = e 2 y − 1 ⟹ e 2 y ( 1 − x ) = 1 + x x(e^{2y} + 1) = e^{2y} - 1 \implies e^{2y}(1 - x) = 1 + x x ( e 2 y + 1 ) = e 2 y − 1 ⟹ e 2 y ( 1 − x ) = 1 + x
e 2 y = 1 + x 1 − x ⟹ 2 y = ln ( 1 + x 1 − x ) e^{2y} = \frac{1 + x}{1 - x} \implies 2y = \ln\!\left(\frac{1 + x}{1 - x}\right) e 2 y = 1 − x 1 + x ⟹ 2 y = ln ( 1 − x 1 + x )
y = 1 2 ln ( 1 + x 1 − x ) ■ y = \frac{1}{2}\ln\!\left(\frac{1 + x}{1 - x}\right) \quad \blacksquare y = 2 1 ln ( 1 − x 1 + x ) ■
3.5 Worked example Problem. Evaluate arsinh 2 \operatorname{arsinh}\,2 arsinh 2 and artanh 1 3 \operatorname{artanh}\,\dfrac{1}{3} artanh 3 1 in exact
logarithmic form.
arsinh 2 = ln ( 2 + 5 ) \operatorname{arsinh}\,2 = \ln(2 + \sqrt{5}) arsinh 2 = ln ( 2 + 5 )
artanh 1 3 = 1 2 ln ( 4 / 3 2 / 3 ) = 1 2 ln 2 \operatorname{artanh}\,\frac{1}{3} = \frac{1}{2}\ln\!\left(\frac{4/3}{2/3}\right) = \frac{1}{2}\ln 2 artanh 3 1 = 2 1 ln ( 2/3 4/3 ) = 2 1 ln 2
3.6 Domains and ranges Function Domain Range arsinh x \operatorname{arsinh}\,x arsinh x R \mathbb{R} R R \mathbb{R} R arcosh x \operatorname{arcosh}\,x arcosh x x ≥ 1 x \geq 1 x ≥ 1 y ≥ 0 y \geq 0 y ≥ 0 artanh x \operatorname{artanh}\,x artanh x − 1 < x < 1 -1 \lt x \lt 1 − 1 < x < 1 R \mathbb{R} R
4. Calculus of Hyperbolic Functions 4.1 Differentiation d d x ( sinh x ) = cosh x \frac{d}{dx}(\sinh x) = \cosh x d x d ( sinh x ) = cosh x
d d x ( cosh x ) = sinh x \frac{d}{dx}(\cosh x) = \sinh x d x d ( cosh x ) = sinh x
d d x ( tanh x ) = s e c h 2 x \frac{d}{dx}(\tanh x) = \mathrm{sech}^2\,x d x d ( tanh x ) = sech 2 x
Proof of d d x sinh x = cosh x \dfrac{d}{dx}\sinh x = \cosh x d x d sinh x = cosh x :
d d x ( e x − e − x 2 ) = e x + e − x 2 = cosh x ■ \frac{d}{dx}\!\left(\frac{e^x - e^{-x}}{2}\right) = \frac{e^x + e^{-x}}{2} = \cosh x \quad \blacksquare d x d ( 2 e x − e − x ) = 2 e x + e − x = cosh x ■
4.2 Differentiation of inverse hyperbolic functions d d x ( arsinh x ) = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 + 1 ◆ R B ◆ \frac{d}{dx}(\operatorname{arsinh}\,x) = \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 + 1}◆RB◆ d x d ( arsinh x ) = L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 + 1 ◆ R B ◆
d d x ( arcosh x ) = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ , x > 1 \frac{d}{dx}(\operatorname{arcosh}\,x) = \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆, \quad x \gt 1 d x d ( arcosh x ) = L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ , x > 1
d d x ( artanh x ) = 1 1 − x 2 , ∣ x ∣ < 1 \frac{d}{dx}(\operatorname{artanh}\,x) = \frac{1}{1 - x^2}, \quad |x| \lt 1 d x d ( artanh x ) = 1 − x 2 1 , ∣ x ∣ < 1
Proof for arsinh x \operatorname{arsinh}\,x arsinh x . Let y = arsinh x y = \operatorname{arsinh}\,x y = arsinh x , so x = sinh y x = \sinh y x = sinh y .
d y d x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ d x d y ◆ R B ◆ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ cosh y ◆ R B ◆ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ ◆ L B ◆ 1 + sinh 2 y ◆ R B ◆◆ R B ◆ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ 1 + x 2 ◆ R B ◆ ■ \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 d x d y = L ◆ B ◆1◆ R B ◆◆ L B ◆ d y d x ◆ R B ◆ = L ◆ B ◆1◆ R B ◆◆ L B ◆ cosh y ◆ R B ◆ = L ◆ B ◆1◆ R B ◆◆ L B ◆ ◆ L B ◆1 + sinh 2 y ◆ R B ◆◆ R B ◆ = L ◆ B ◆1◆ R B ◆◆ L B ◆ 1 + x 2 ◆ R B ◆ ■
Proof for artanh x \operatorname{artanh}\,x artanh x . Let y = artanh x y = \operatorname{artanh}\,x y = artanh x , so x = tanh y x = \tanh y x = tanh y .
d y d x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ s e c h 2 y ◆ R B ◆ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ 1 − tanh 2 y ◆ R B ◆ = 1 1 − x 2 ■ \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 d x d y = L ◆ B ◆1◆ R B ◆◆ L B ◆ sech 2 y ◆ R B ◆ = L ◆ B ◆1◆ R B ◆◆ L B ◆1 − tanh 2 y ◆ R B ◆ = 1 − x 2 1 ■
4.3 Integration The differentiation results give standard integrals:
∫ cosh x d x = sinh x + C \int \cosh x\,dx = \sinh x + C ∫ cosh x d x = sinh x + C
∫ sinh x d x = cosh x + C \int \sinh x\,dx = \cosh x + C ∫ sinh x d x = cosh x + C
∫ s e c h 2 x d x = tanh x + C \int \mathrm{sech}^2\,x\,dx = \tanh x + C ∫ sech 2 x d x = tanh x + C
4.4 Integrals leading to inverse hyperbolic functions ∫ ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 + a 2 ◆ R B ◆ d x = arsinh ( x a ) + C \int \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 + a^2}◆RB◆\,dx = \operatorname{arsinh}\!\left(\frac{x}{a}\right) + C ∫ L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 + a 2 ◆ R B ◆ d x = arsinh ( a x ) + C
∫ ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − a 2 ◆ R B ◆ d x = arcosh ( x a ) + 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 ∫ L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − a 2 ◆ R B ◆ d x = arcosh ( a x ) + C , x > a
∫ 1 a 2 − x 2 d x = 1 a artanh ( x a ) + 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 ∫ a 2 − x 2 1 d x = a 1 artanh ( a x ) + C , ∣ x ∣ < a
Proof of the first formula. Let u = x / a u = x/a u = x / a :
∫ ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + a 2 ◆ R B ◆ = ∫ ◆ L B ◆ a d u ◆ R B ◆◆ L B ◆ a u 2 + 1 ◆ R B ◆ = arsinh u + C = arsinh ( x a ) + 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 ∫ L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + a 2 ◆ R B ◆ = ∫ L ◆ B ◆ a d u ◆ R B ◆◆ L B ◆ a u 2 + 1 ◆ R B ◆ = arsinh u + C = arsinh ( a x ) + C ■
4.5 Worked example: differentiation Problem. Differentiate f ( x ) = sinh ( 3 x 2 ) f(x) = \sinh(3x^2) f ( x ) = sinh ( 3 x 2 ) .
f ′ ( x ) = 6 x cosh ( 3 x 2 ) f'(x) = 6x\cosh(3x^2) f ′ ( x ) = 6 x cosh ( 3 x 2 )
4.6 Worked example: integration Problem. Evaluate ∫ ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ 4 x 2 + 9 ◆ R B ◆ d x \displaystyle\int \frac◆LB◆1◆RB◆◆LB◆\sqrt{4x^2 + 9}◆RB◆\,dx ∫ L ◆ B ◆1◆ R B ◆◆ L B ◆ 4 x 2 + 9 ◆ R B ◆ d x .
∫ ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ 4 x 2 + 9 ◆ R B ◆ = 1 2 ∫ ◆ L B ◆ d ( 2 x ) ◆ R B ◆◆ L B ◆ ( 2 x ) 2 + 9 ◆ R B ◆ = 1 2 arsinh ( 2 x 3 ) + 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 ∫ L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ 4 x 2 + 9 ◆ R B ◆ = 2 1 ∫ L ◆ B ◆ d ( 2 x ) ◆ R B ◆◆ L B ◆ ( 2 x ) 2 + 9 ◆ R B ◆ = 2 1 arsinh ( 3 2 x ) + C
4.7 Worked example: definite integral Problem. Evaluate ∫ 0 1 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + 1 ◆ R B ◆ \displaystyle\int_0^1 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 + 1}◆RB◆ ∫ 0 1 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + 1 ◆ R B ◆ .
= [ arsinh x ] 0 1 = 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}) = [ arsinh x ] 0 1 = arsinh 1 − arsinh 0 = ln ( 1 + 2 ) − 0 = ln ( 1 + 2 )
4.8 Worked example: integration by substitution with hyperbolic functions Problem. Evaluate ∫ x 2 + 4 d x \displaystyle\int \sqrt{x^2 + 4}\,dx ∫ x 2 + 4 d x .
Use the substitution x = 2 sinh u x = 2\sinh u x = 2 sinh u , d x = 2 cosh u d u dx = 2\cosh u\,du d x = 2 cosh u d u :
∫ ◆ L B ◆ 4 sinh 2 u + 4 ◆ R B ◆ ⋅ 2 cosh u d u = ∫ 2 cosh u ⋅ 2 cosh u d u = 4 ∫ cosh 2 u d u \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 ∫ ◆ L B ◆4 sinh 2 u + 4◆ R B ◆ ⋅ 2 cosh u d u = ∫ 2 cosh u ⋅ 2 cosh u d u = 4 ∫ cosh 2 u d u
Using cosh 2 u = ◆ L B ◆ 1 + cosh 2 u ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \cosh^2 u = \dfrac◆LB◆1 + \cosh 2u◆RB◆◆LB◆2◆RB◆ cosh 2 u = L ◆ B ◆1 + cosh 2 u ◆ R B ◆◆ L B ◆2◆ R B ◆ :
= 4 ∫ ◆ L B ◆ 1 + cosh 2 u ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ d u = 2 u + sinh 2 u + C = 4\int \frac◆LB◆1 + \cosh 2u◆RB◆◆LB◆2◆RB◆\,du = 2u + \sinh 2u + C = 4 ∫ L ◆ B ◆1 + cosh 2 u ◆ R B ◆◆ L B ◆2◆ R B ◆ d u = 2 u + sinh 2 u + C
= 2 u + 2 sinh u cosh u + C = 2u + 2\sinh u\cosh u + C = 2 u + 2 sinh u cosh u + C
Since x = 2 sinh u x = 2\sinh u x = 2 sinh u : sinh u = x 2 \sinh u = \dfrac{x}{2} sinh u = 2 x ,
cosh u = ◆ L B ◆ 1 + x 2 4 ◆ R B ◆ = ◆ L B ◆ x 2 + 4 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \cosh u = \sqrt◆LB◆1 + \dfrac{x^2}{4}◆RB◆ = \dfrac◆LB◆\sqrt{x^2 + 4}◆RB◆◆LB◆2◆RB◆ cosh u = ◆ L B ◆1 + 4 x 2 ◆ R B ◆ = L ◆ B ◆ x 2 + 4 ◆ R B ◆◆ L B ◆2◆ R B ◆ ,
u = arsinh ( x 2 ) u = \operatorname{arsinh}\!\left(\dfrac{x}{2}\right) u = arsinh ( 2 x ) .
= 2 arsinh ( x 2 ) + ◆ L B ◆ x x 2 + 4 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ + C = 2\operatorname{arsinh}\!\left(\frac{x}{2}\right) + \frac◆LB◆x\sqrt{x^2 + 4}◆RB◆◆LB◆2◆RB◆ + C = 2 arsinh ( 2 x ) + L ◆ B ◆ x x 2 + 4 ◆ R B ◆◆ L B ◆2◆ R B ◆ + C
Common Pitfall The substitution
x = a sinh u x = a\sinh u x = a sinh u is a powerful technique for integrals
involving x 2 + a 2 \sqrt{x^2 + a^2} x 2 + a 2 . Similarly, x = a cosh u x = a\cosh u x = a cosh u handles x 2 − a 2 \sqrt{x^2 - a^2} x 2 − a 2 and
x = a tanh u x = a\tanh u x = a tanh u handles expressions with a 2 − x 2 a^2 - x^2 a 2 − x 2 . The choice of substitution mirrors the
trigonometric substitutions but is often simpler algebraically. :::
5. Practice Problems Problem 1 Solve the equation 4 sinh x − 3 cosh x = 0 4\sinh x - 3\cosh x = 0 4 sinh x − 3 cosh x = 0 .
Solution 4 sinh x = 3 cosh x ⟹ tanh x = 3 4 4\sinh x = 3\cosh x \implies \tanh x = \dfrac{3}{4} 4 sinh x = 3 cosh x ⟹ tanh x = 4 3 .
x = artanh ( 3 4 ) = 1 2 ln ( 1 + 3 / 4 1 − 3 / 4 ) = 1 2 ln 7 x = \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 x = artanh ( 4 3 ) = 2 1 ln ( 1 − 3/4 1 + 3/4 ) = 2 1 ln 7 .
Problem 2 Prove that sinh 3 x = 3 sinh x + 4 sinh 3 x \sinh 3x = 3\sinh x + 4\sinh^3 x sinh 3 x = 3 sinh x + 4 sinh 3 x .
Solution sinh 3 x = sinh ( 2 x + x ) = sinh 2 x cosh x + cosh 2 x sinh x \sinh 3x = \sinh(2x + x) = \sinh 2x\cosh x + \cosh 2x\sinh x sinh 3 x = sinh ( 2 x + x ) = sinh 2 x cosh x + cosh 2 x sinh x
= 2 sinh x cosh 2 x + ( 1 + 2 sinh 2 x ) sinh x = 2\sinh x\cosh^2 x + (1 + 2\sinh^2 x)\sinh x = 2 sinh x cosh 2 x + ( 1 + 2 sinh 2 x ) sinh x
= 2 sinh x ( 1 + sinh 2 x ) + sinh x + 2 sinh 3 x = 2\sinh x(1 + \sinh^2 x) + \sinh x + 2\sinh^3 x = 2 sinh x ( 1 + sinh 2 x ) + sinh x + 2 sinh 3 x
= 2 sinh x + 2 sinh 3 x + sinh x + 2 sinh 3 x = 3 sinh x + 4 sinh 3 x = 2\sinh x + 2\sinh^3 x + \sinh x + 2\sinh^3 x = 3\sinh x + 4\sinh^3 x = 2 sinh x + 2 sinh 3 x + sinh x + 2 sinh 3 x = 3 sinh x + 4 sinh 3 x .
Problem 3 Evaluate ∫ 0 2 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + 16 ◆ R B ◆ \displaystyle\int_0^2 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 + 16}◆RB◆ ∫ 0 2 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + 16 ◆ R B ◆ .
Solution = [ arsinh ( x 4 ) ] 0 2 = arsinh ( 1 2 ) = ln ( 1 2 + ◆ L B ◆ 5 4 ◆ R B ◆ ) = ln ( ◆ L B ◆ 1 + 5 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ) = \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) = [ arsinh ( 4 x ) ] 0 2 = arsinh ( 2 1 ) = ln ( 2 1 + ◆ L B ◆ 4 5 ◆ R B ◆ ) = ln ( L ◆ B ◆1 + 5 ◆ R B ◆◆ L B ◆2◆ R B ◆ ) .
Problem 4 Differentiate f ( x ) = x arcosh x f(x) = x\,\operatorname{arcosh}\,x f ( x ) = x arcosh x for x > 1 x \gt 1 x > 1 .
Solution Using the product rule:
f ′ ( x ) = arcosh x + x ⋅ ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ = arcosh x + ◆ L B ◆ x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ f'(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◆ f ′ ( x ) = arcosh x + x ⋅ L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ = arcosh x + L ◆ B ◆ x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ .
6. Further Proofs and Key Results 6.1 Proof: ∫ ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − a 2 ◆ R B ◆ d x = arcosh ( x a ) + C \int \frac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - a^2}◆RB◆\,dx = \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C ∫ L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − a 2 ◆ R B ◆ d x = arcosh ( a x ) + C Proof. Let u = x / a u = x/a u = x / a , so d x = a d u dx = a\,du d x = a d u :
∫ ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − a 2 ◆ R B ◆ = ∫ ◆ L B ◆ a d u ◆ R B ◆◆ L B ◆ a u 2 − 1 ◆ R B ◆ = ∫ ◆ L B ◆ d u ◆ R B ◆◆ L B ◆ u 2 − 1 ◆ R B ◆ \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◆ ∫ L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − a 2 ◆ R B ◆ = ∫ L ◆ B ◆ a d u ◆ R B ◆◆ L B ◆ a u 2 − 1 ◆ R B ◆ = ∫ L ◆ B ◆ d u ◆ R B ◆◆ L B ◆ u 2 − 1 ◆ R B ◆
Now let u = cosh t u = \cosh t u = cosh t , so d u = sinh t d t du = \sinh t\,dt d u = sinh t d t :
= ∫ ◆ L B ◆ sinh t d t ◆ R B ◆◆ L B ◆ ◆ L B ◆ cosh 2 t − 1 ◆ R B ◆◆ R B ◆ = ∫ ◆ L B ◆ sinh t d t ◆ R B ◆◆ L B ◆ sinh t ◆ R B ◆ = ∫ 1 d t = t + C = arcosh u + 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 = ∫ L ◆ B ◆ sinh t d t ◆ R B ◆◆ L B ◆ ◆ L B ◆ cosh 2 t − 1◆ R B ◆◆ R B ◆ = ∫ L ◆ B ◆ sinh t d t ◆ R B ◆◆ L B ◆ sinh t ◆ R B ◆ = ∫ 1 d t = t + C = arcosh u + C
= arcosh ( x a ) + C ■ = \operatorname{arcosh}\!\left(\frac{x}{a}\right) + C \quad \blacksquare = arcosh ( a x ) + C ■
6.2 Proof: ∫ 1 a 2 − x 2 d x = 1 a artanh ( x a ) + C \int \frac{1}{a^2 - x^2}\,dx = \frac{1}{a}\operatorname{artanh}\!\left(\frac{x}{a}\right) + C ∫ a 2 − x 2 1 d x = a 1 artanh ( a x ) + C Proof. Let u = x / a u = x/a u = x / a , so d x = a d u dx = a\,du d x = a d u :
∫ d x a 2 − x 2 = 1 a ∫ d u 1 − u 2 = 1 a artanh u + C = 1 a artanh ( x a ) + 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 ∫ a 2 − x 2 d x = a 1 ∫ 1 − u 2 d u = a 1 artanh u + C = a 1 artanh ( a x ) + C ■
6.3 Proof: the catenary equation Theorem. A uniform chain hanging under gravity takes the shape
y = a cosh ( x a ) + c y = a\cosh\!\left(\dfrac{x}{a}\right) + c y = a cosh ( a x ) + c .
Proof (sketch). Consider a small element of the chain between horizontal positions x x x and
x + δ x x + \delta x x + δ x . Let the tension at position x x x be T T T , making angle θ \theta θ with the horizontal.
Horizontal equilibrium: T cos θ = T 0 T\cos\theta = T_0 T cos θ = T 0 (constant).
Vertical equilibrium: d d x ( T sin θ ) = w \dfrac{d}{dx}(T\sin\theta) = w d x d ( T sin θ ) = w where w w w is the weight per unit length.
Since T = T 0 sec θ T = T_0\sec\theta T = T 0 sec θ and T sin θ = T 0 tan θ T\sin\theta = T_0\tan\theta T sin θ = T 0 tan θ :
d d x ( T 0 tan θ ) = w ⟹ T 0 sec 2 θ ◆ L B ◆ d θ ◆ R B ◆◆ L B ◆ d x ◆ R B ◆ = w \frac{d}{dx}(T_0\tan\theta) = w \implies T_0\sec^2\theta\,\frac◆LB◆d\theta◆RB◆◆LB◆dx◆RB◆ = w d x d ( T 0 tan θ ) = w ⟹ T 0 sec 2 θ L ◆ B ◆ d θ ◆ R B ◆◆ L B ◆ d x ◆ R B ◆ = w
Let y ′ = tan θ y' = \tan\theta y ′ = tan θ , so
d y ′ d x = sec 2 θ ◆ L B ◆ d θ ◆ R B ◆◆ L B ◆ d x ◆ R B ◆ = w T 0 \dfrac{dy'}{dx} = \sec^2\theta\,\dfrac◆LB◆d\theta◆RB◆◆LB◆dx◆RB◆ = \dfrac{w}{T_0} d x d y ′ = sec 2 θ L ◆ B ◆ d θ ◆ R B ◆◆ L B ◆ d x ◆ R B ◆ = T 0 w .
Integrating: y ′ = w T 0 x + C 1 y' = \dfrac{w}{T_0}\,x + C_1 y ′ = T 0 w x + C 1 . Taking C 1 = 0 C_1 = 0 C 1 = 0 by symmetry:
y ′ = x a where a = T 0 w y' = \frac{x}{a} \quad \text{where } a = \frac{T_0}{w} y ′ = a x where a = w T 0
Integrating again: y = a cosh ( x a ) + C y = a\cosh\!\left(\dfrac{x}{a}\right) + C y = a cosh ( a x ) + C . ■ \blacksquare ■
7. Common Pitfalls
Sign in the fundamental identity: Unlike cos 2 x + sin 2 x = 1 \cos^2 x + \sin^2 x = 1 cos 2 x + sin 2 x = 1 , the hyperbolic identity
is cosh 2 x − sinh 2 x = 1 \cosh^2 x - \sinh^2 x = 1 cosh 2 x − sinh 2 x = 1 . The minus sign is crucial and is the source of many errors.
Domain of arcosh \operatorname{arcosh} arcosh : The domain is x ≥ 1 x \geq 1 x ≥ 1 (not x > 0 x > 0 x > 0 ). Attempting to
evaluate arcosh ( 0.5 ) \operatorname{arcosh}(0.5) arcosh ( 0.5 ) is undefined.
cosh x ≥ 1 \cosh x \geq 1 cosh x ≥ 1 always: When solving cosh 2 x = k \cosh^2 x = k cosh 2 x = k and taking the square root, always take
the positive root cosh x = + k \cosh x = +\sqrt{k} cosh x = + k since cosh x ≥ 1 > 0 \cosh x \geq 1 > 0 cosh x ≥ 1 > 0 for all real x x x .
Integration: artanh vs ln: When ∣ x ∣ > a |x| > a ∣ x ∣ > a in ∫ d x a 2 − x 2 \displaystyle\int \frac{dx}{a^2 - x^2} ∫ a 2 − x 2 d x , the
result involves arcoth \operatorname{arcoth} arcoth (or an alternative logarithmic form), not
artanh \operatorname{artanh} artanh . Check the domain of the integrand carefully. :::
8. Additional Exam-Style Questions Question 5 (a) Solve the equation cosh x = 2.5 \cosh x = 2.5 cosh x = 2.5 , giving your answer in exact logarithmic form.
(b) Hence solve cosh 2 x = 2.5 \cosh 2x = 2.5 cosh 2 x = 2.5 .
Solution (a) cosh x = e x + e − x 2 = 2.5 \cosh x = \dfrac{e^x + e^{-x}}{2} = 2.5 cosh x = 2 e x + e − x = 2.5
e x + e − x = 5 ⟹ e 2 x − 5 e x + 1 = 0 e^x + e^{-x} = 5 \implies e^{2x} - 5e^x + 1 = 0 e x + e − x = 5 ⟹ e 2 x − 5 e x + 1 = 0
e x = ◆ L B ◆ 5 ± 25 − 4 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = ◆ L B ◆ 5 ± 21 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ e^x = \dfrac◆LB◆5 \pm \sqrt{25 - 4}◆RB◆◆LB◆2◆RB◆ = \dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆ e x = L ◆ B ◆5 ± 25 − 4 ◆ R B ◆◆ L B ◆2◆ R B ◆ = L ◆ B ◆5 ± 21 ◆ R B ◆◆ L B ◆2◆ R B ◆
x = ln ( ◆ L B ◆ 5 ± 21 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ) x = \ln\!\left(\dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆\right) x = ln ( L ◆ B ◆5 ± 21 ◆ R B ◆◆ L B ◆2◆ R B ◆ )
Since cosh \cosh cosh is even, both ± \pm ± give valid solutions (one positive, one negative).
(b) cosh 2 x = 2.5 ⟹ 2 x = ln ( ◆ L B ◆ 5 ± 21 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ) \cosh 2x = 2.5 \implies 2x = \ln\!\left(\dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆\right) cosh 2 x = 2.5 ⟹ 2 x = ln ( L ◆ B ◆5 ± 21 ◆ R B ◆◆ L B ◆2◆ R B ◆ )
x = 1 2 ln ( ◆ L B ◆ 5 ± 21 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ) x = \dfrac{1}{2}\ln\!\left(\dfrac◆LB◆5 \pm \sqrt{21}◆RB◆◆LB◆2◆RB◆\right) x = 2 1 ln ( L ◆ B ◆5 ± 21 ◆ R B ◆◆ L B ◆2◆ R B ◆ )
Alternatively, using cosh 2 x = 2 cosh 2 x − 1 = 2.5 ⟹ cosh 2 x = 1.75 \cosh 2x = 2\cosh^2 x - 1 = 2.5 \implies \cosh^2 x = 1.75 cosh 2 x = 2 cosh 2 x − 1 = 2.5 ⟹ cosh 2 x = 1.75 , which gives the
same result.
Question 6 (a) Prove that d d x ( arcosh x ) = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ \dfrac{d}{dx}(\operatorname{arcosh}\,x) = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ d x d ( arcosh x ) = L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆
for x > 1 x > 1 x > 1 .
(b) Evaluate ∫ 2 3 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ \displaystyle\int_2^3 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ ∫ 2 3 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ in exact form.
Solution (a) Let y = arcosh x y = \operatorname{arcosh}\,x y = arcosh x , so x = cosh y x = \cosh y x = cosh y .
d x d y = sinh y \dfrac{dx}{dy} = \sinh y d y d x = sinh y , so d y d x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ sinh y ◆ R B ◆ \dfrac{dy}{dx} = \dfrac◆LB◆1◆RB◆◆LB◆\sinh y◆RB◆ d x d y = L ◆ B ◆1◆ R B ◆◆ L B ◆ sinh y ◆ R B ◆ .
Since cosh 2 y − sinh 2 y = 1 \cosh^2 y - \sinh^2 y = 1 cosh 2 y − sinh 2 y = 1 : sinh y = ◆ L B ◆ cosh 2 y − 1 ◆ R B ◆ = x 2 − 1 \sinh y = \sqrt◆LB◆\cosh^2 y - 1◆RB◆ = \sqrt{x^2 - 1} sinh y = ◆ L B ◆ cosh 2 y − 1◆ R B ◆ = x 2 − 1 .
d y d x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ ■ \dfrac{dy}{dx} = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ \quad \blacksquare d x d y = L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ ■
(b)
∫ 2 3 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ = [ arcosh x ] 2 3 \displaystyle\int_2^3 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ = \bigl[\operatorname{arcosh}\,x\bigr]_2^3 ∫ 2 3 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ = [ arcosh x ] 2 3
= ln ( 3 + 8 ) − ln ( 2 + 3 ) = ln ( 3 + 2 2 ) − ln ( 2 + 3 ) = \ln(3 + \sqrt{8}) - \ln(2 + \sqrt{3}) = \ln(3 + 2\sqrt{2}) - \ln(2 + \sqrt{3}) = ln ( 3 + 8 ) − ln ( 2 + 3 ) = ln ( 3 + 2 2 ) − ln ( 2 + 3 )
= ln ( ◆ L B ◆ 3 + 2 2 ◆ R B ◆◆ L B ◆ 2 + 3 ◆ R B ◆ ) = \ln\!\left(\dfrac◆LB◆3 + 2\sqrt{2}◆RB◆◆LB◆2 + \sqrt{3}◆RB◆\right) = ln ( L ◆ B ◆3 + 2 2 ◆ R B ◆◆ L B ◆2 + 3 ◆ R B ◆ ) .
Question 7 A curve C C C has equation y = sinh − 1 ( 2 x − 1 ) y = \sinh^{-1}(2x - 1) y = sinh − 1 ( 2 x − 1 ) .
(a) Find d y d x \dfrac{dy}{dx} d x d y .
(b) Find the equation of the tangent to C C C at the point where x = 1 x = 1 x = 1 .
Solution (a) y = arsinh ( 2 x − 1 ) y = \operatorname{arsinh}(2x - 1) y = arsinh ( 2 x − 1 ) .
d y d x = ◆ L B ◆ 2 ◆ R B ◆◆ L B ◆ ( 2 x − 1 ) 2 + 1 ◆ R B ◆ = ◆ L B ◆ 2 ◆ R B ◆◆ L B ◆ 4 x 2 − 4 x + 2 ◆ R B ◆ \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◆ d x d y = L ◆ B ◆2◆ R B ◆◆ L B ◆ ( 2 x − 1 ) 2 + 1 ◆ R B ◆ = L ◆ B ◆2◆ R B ◆◆ L B ◆ 4 x 2 − 4 x + 2 ◆ R B ◆ .
(b) At x = 1 x = 1 x = 1 : y = arsinh ( 1 ) = ln ( 1 + 2 ) y = \operatorname{arsinh}(1) = \ln(1 + \sqrt{2}) y = arsinh ( 1 ) = ln ( 1 + 2 ) .
d y d x ∣ x = 1 = ◆ L B ◆ 2 ◆ R B ◆◆ L B ◆ 4 − 4 + 2 ◆ R B ◆ = ◆ L B ◆ 2 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = 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} d x d y x = 1 = L ◆ B ◆2◆ R B ◆◆ L B ◆ 4 − 4 + 2 ◆ R B ◆ = L ◆ B ◆2◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = 2 .
Equation of tangent: y − ln ( 1 + 2 ) = 2 ( x − 1 ) y - \ln(1 + \sqrt{2}) = \sqrt{2}(x - 1) y − ln ( 1 + 2 ) = 2 ( x − 1 ) , i.e.
y = 2 x − 2 + ln ( 1 + 2 ) y = \sqrt{2}\,x - \sqrt{2} + \ln(1 + \sqrt{2}) y = 2 x − 2 + ln ( 1 + 2 ) .
9. Advanced Worked Examples Example 9.1: Solving hyperbolic equations Problem. Solve 3 sinh x + 4 cosh x = 5 3\sinh x + 4\cosh x = 5 3 sinh x + 4 cosh x = 5 , giving your answer in exact logarithmic form.
Solution. Using the exponential definitions:
3 ⋅ e x − e − x 2 + 4 ⋅ e x + e − x 2 = 5 3\cdot\frac{e^x - e^{-x}}{2} + 4\cdot\frac{e^x + e^{-x}}{2} = 5 3 ⋅ 2 e x − e − x + 4 ⋅ 2 e x + e − x = 5
3 e x − 3 e − x + 4 e x + 4 e − x = 10 3e^x - 3e^{-x} + 4e^x + 4e^{-x} = 10 3 e x − 3 e − x + 4 e x + 4 e − x = 10
7 e x + e − x = 10 7e^x + e^{-x} = 10 7 e x + e − x = 10
Multiplying by e x e^x e x : 7 e 2 x + 1 = 10 e x 7e^{2x} + 1 = 10e^x 7 e 2 x + 1 = 10 e x
7 e 2 x − 10 e x + 1 = 0 7e^{2x} - 10e^x + 1 = 0 7 e 2 x − 10 e x + 1 = 0
This is a quadratic in e x e^x e x :
e x = ◆ L B ◆ 10 ± 100 − 28 ◆ R B ◆◆ L B ◆ 14 ◆ R B ◆ = ◆ L B ◆ 10 ± 72 ◆ R B ◆◆ L B ◆ 14 ◆ R B ◆ = ◆ L B ◆ 10 ± 6 2 ◆ R B ◆◆ L B ◆ 14 ◆ R B ◆ = ◆ L B ◆ 5 ± 3 2 ◆ R B ◆◆ L B ◆ 7 ◆ R B ◆ e^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◆ e x = L ◆ B ◆10 ± 100 − 28 ◆ R B ◆◆ L B ◆14◆ R B ◆ = L ◆ B ◆10 ± 72 ◆ R B ◆◆ L B ◆14◆ R B ◆ = L ◆ B ◆10 ± 6 2 ◆ R B ◆◆ L B ◆14◆ R B ◆ = L ◆ B ◆5 ± 3 2 ◆ R B ◆◆ L B ◆7◆ R B ◆
x = ln ( ◆ L B ◆ 5 + 3 2 ◆ R B ◆◆ L B ◆ 7 ◆ R B ◆ ) or x = ln ( ◆ L B ◆ 5 − 3 2 ◆ R B ◆◆ L B ◆ 7 ◆ R B ◆ ) 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) x = ln ( L ◆ B ◆5 + 3 2 ◆ R B ◆◆ L B ◆7◆ R B ◆ ) or x = ln ( L ◆ B ◆5 − 3 2 ◆ R B ◆◆ L B ◆7◆ R B ◆ )
Since ◆ L B ◆ 5 − 3 2 ◆ R B ◆◆ L B ◆ 7 ◆ R B ◆ ≈ 0.109 > 0 \dfrac◆LB◆5 - 3\sqrt{2}◆RB◆◆LB◆7◆RB◆ \approx 0.109 > 0 L ◆ B ◆5 − 3 2 ◆ R B ◆◆ L B ◆7◆ R B ◆ ≈ 0.109 > 0 , both solutions are valid.
Example 9.2: Integration using hyperbolic substitution Problem. Evaluate ∫ x 2 − 9 d x \displaystyle\int \sqrt{x^2 - 9}\,dx ∫ x 2 − 9 d x for x ≥ 3 x \geq 3 x ≥ 3 .
Solution. Use the substitution x = 3 cosh u x = 3\cosh u x = 3 cosh u , d x = 3 sinh u d u dx = 3\sinh u\,du d x = 3 sinh u d u :
∫ ◆ L B ◆ 9 cosh 2 u − 9 ◆ R B ◆ ⋅ 3 sinh u d u = ∫ 3 sinh u ⋅ 3 sinh u d u = 9 ∫ sinh 2 u d u \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 ∫ ◆ L B ◆9 cosh 2 u − 9◆ R B ◆ ⋅ 3 sinh u d u = ∫ 3 sinh u ⋅ 3 sinh u d u = 9 ∫ sinh 2 u d u
Using sinh 2 u = ◆ L B ◆ cosh 2 u − 1 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \sinh^2 u = \dfrac◆LB◆\cosh 2u - 1◆RB◆◆LB◆2◆RB◆ sinh 2 u = L ◆ B ◆ cosh 2 u − 1◆ R B ◆◆ L B ◆2◆ R B ◆ :
= 9 ∫ ◆ L B ◆ cosh 2 u − 1 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ d u = 9 2 ( ◆ L B ◆ sinh 2 u ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ − u ) + C = 9 4 sinh 2 u − 9 2 u + 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 = 9 ∫ L ◆ B ◆ cosh 2 u − 1◆ R B ◆◆ L B ◆2◆ R B ◆ d u = 2 9 ( L ◆ B ◆ sinh 2 u ◆ R B ◆◆ L B ◆2◆ R B ◆ − u ) + C = 4 9 sinh 2 u − 2 9 u + C
Since x = 3 cosh u x = 3\cosh u x = 3 cosh u : cosh u = x 3 \cosh u = \dfrac{x}{3} cosh u = 3 x ,
sinh u = ◆ L B ◆ x 2 9 − 1 ◆ R B ◆ = ◆ L B ◆ x 2 − 9 ◆ R B ◆◆ L B ◆ 3 ◆ R B ◆ \sinh u = \sqrt◆LB◆\dfrac{x^2}{9} - 1◆RB◆ = \dfrac◆LB◆\sqrt{x^2 - 9}◆RB◆◆LB◆3◆RB◆ sinh u = ◆ L B ◆ 9 x 2 − 1◆ R B ◆ = L ◆ B ◆ x 2 − 9 ◆ R B ◆◆ L B ◆3◆ R B ◆ .
sinh 2 u = 2 sinh u cosh u = ◆ L B ◆ 2 x x 2 − 9 ◆ R B ◆◆ L B ◆ 9 ◆ R B ◆ \sinh 2u = 2\sinh u\cosh u = \dfrac◆LB◆2x\sqrt{x^2 - 9}◆RB◆◆LB◆9◆RB◆ sinh 2 u = 2 sinh u cosh u = L ◆ B ◆2 x x 2 − 9 ◆ R B ◆◆ L B ◆9◆ R B ◆ .
u = arcosh ( x 3 ) = ln ( x 3 + ◆ L B ◆ x 2 9 − 1 ◆ R B ◆ ) u = \operatorname{arcosh}\!\left(\dfrac{x}{3}\right) = \ln\!\left(\dfrac{x}{3} + \sqrt◆LB◆\dfrac{x^2}{9} - 1◆RB◆\right) u = arcosh ( 3 x ) = ln ( 3 x + ◆ L B ◆ 9 x 2 − 1◆ R B ◆ ) .
= ◆ L B ◆ x x 2 − 9 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ − 9 2 arcosh ( x 3 ) + C = \frac◆LB◆x\sqrt{x^2 - 9}◆RB◆◆LB◆2◆RB◆ - \frac{9}{2}\operatorname{arcosh}\!\left(\frac{x}{3}\right) + C = L ◆ B ◆ x x 2 − 9 ◆ R B ◆◆ L B ◆2◆ R B ◆ − 2 9 arcosh ( 3 x ) + C
Example 9.3: Proving an identity using Osborne's rule Problem. Prove that cosh 3 x = 4 cosh 3 x − 3 cosh x \cosh 3x = 4\cosh^3 x - 3\cosh x cosh 3 x = 4 cosh 3 x − 3 cosh x .
Solution. From the trigonometric identity cos 3 θ = 4 cos 3 θ − 3 cos θ \cos 3\theta = 4\cos^3\theta - 3\cos\theta cos 3 θ = 4 cos 3 θ − 3 cos θ , applying
Osborne's rule: since cos 3 θ \cos^3\theta cos 3 θ contains no products of sin \sin sin , it remains unchanged.
Therefore:
cosh 3 x = 4 cosh 3 x − 3 cosh x \cosh 3x = 4\cosh^3 x - 3\cosh x cosh 3 x = 4 cosh 3 x − 3 cosh x
Direct proof. Starting from cosh 3 x = cosh ( 2 x + x ) \cosh 3x = \cosh(2x + x) cosh 3 x = cosh ( 2 x + x ) :
= cosh 2 x cosh x + sinh 2 x sinh x = ( 2 cosh 2 x − 1 ) cosh x + 2 sinh 2 x cosh x = \cosh 2x\cosh x + \sinh 2x\sinh x = (2\cosh^2 x - 1)\cosh x + 2\sinh^2 x\cosh x = cosh 2 x cosh x + sinh 2 x sinh x = ( 2 cosh 2 x − 1 ) cosh x + 2 sinh 2 x cosh 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 = 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 = 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
= 4 cosh 3 x − 3 cosh x ■ = 4\cosh^3 x - 3\cosh x \quad \blacksquare = 4 cosh 3 x − 3 cosh x ■
Example 9.4: Differentiation involving multiple hyperbolic functions Problem. Find d y d x \dfrac{dy}{dx} d x d y where y = ◆ L B ◆ sinh x ◆ R B ◆◆ L B ◆ 1 + cosh x ◆ R B ◆ y = \dfrac◆LB◆\sinh x◆RB◆◆LB◆1 + \cosh x◆RB◆ y = L ◆ B ◆ sinh x ◆ R B ◆◆ L B ◆1 + cosh x ◆ R B ◆ and simplify
your answer.
Solution. Using the quotient rule:
d y d x = ◆ L B ◆ cosh x ( 1 + cosh x ) − sinh x ⋅ sinh x ◆ R B ◆◆ L B ◆ ( 1 + cosh x ) 2 ◆ R B ◆ = ◆ L B ◆ cosh x + cosh 2 x − sinh 2 x ◆ R B ◆◆ L B ◆ ( 1 + cosh x ) 2 ◆ R B ◆ \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◆ d x d y = L ◆ B ◆ cosh x ( 1 + cosh x ) − sinh x ⋅ sinh x ◆ R B ◆◆ L B ◆ ( 1 + cosh x ) 2 ◆ R B ◆ = L ◆ B ◆ cosh x + cosh 2 x − sinh 2 x ◆ R B ◆◆ L B ◆ ( 1 + cosh x ) 2 ◆ R B ◆
Using cosh 2 x − sinh 2 x = 1 \cosh^2 x - \sinh^2 x = 1 cosh 2 x − sinh 2 x = 1 :
= ◆ L B ◆ cosh x + 1 ◆ R B ◆◆ L B ◆ ( 1 + cosh x ) 2 ◆ R B ◆ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ 1 + cosh x ◆ R B ◆ = s e c h 2 ( x 2 ) = \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) = L ◆ B ◆ cosh x + 1◆ R B ◆◆ L B ◆ ( 1 + cosh x ) 2 ◆ R B ◆ = L ◆ B ◆1◆ R B ◆◆ L B ◆1 + cosh x ◆ R B ◆ = sech 2 ( 2 x )
The final simplification uses the identity 1 + cosh x = 2 cosh 2 ( x / 2 ) 1 + \cosh x = 2\cosh^2(x/2) 1 + cosh x = 2 cosh 2 ( x /2 ) .
Example 9.5: Definite integral with inverse hyperbolic functions Problem. Evaluate ∫ 0 1 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ 1 + 4 x 2 ◆ R B ◆ \displaystyle\int_0^1 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{1 + 4x^2}◆RB◆ ∫ 0 1 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ 1 + 4 x 2 ◆ R B ◆ .
Solution. Write 1 + 4 x 2 = 4 ( x 2 + 1 / 4 ) = 2 x 2 + ( 1 / 2 ) 2 \sqrt{1 + 4x^2} = \sqrt{4(x^2 + 1/4)} = 2\sqrt{x^2 + (1/2)^2} 1 + 4 x 2 = 4 ( x 2 + 1/4 ) = 2 x 2 + ( 1/2 ) 2 .
∫ 0 1 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ 1 + 4 x 2 ◆ R B ◆ = 1 2 ∫ 0 1 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + 1 / 4 ◆ R B ◆ = 1 2 [ arsinh ( x 1 / 2 ) ] 0 1 \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 ∫ 0 1 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ 1 + 4 x 2 ◆ R B ◆ = 2 1 ∫ 0 1 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 + 1/4 ◆ R B ◆ = 2 1 [ arsinh ( 1/2 x ) ] 0 1
= 1 2 [ arsinh 2 − arsinh 0 ] = 1 2 ln ( 2 + 5 ) = \frac{1}{2}\bigl[\operatorname{arsinh}\,2 - \operatorname{arsinh}\,0\bigr] = \frac{1}{2}\ln(2 + \sqrt{5}) = 2 1 [ arsinh 2 − arsinh 0 ] = 2 1 ln ( 2 + 5 )
Example 9.6: Parametric differentiation with hyperbolic functions Problem. A curve is given parametrically by x = 2 cosh t x = 2\cosh t x = 2 cosh t , y = 3 sinh t y = 3\sinh t y = 3 sinh t . Find the value of
d y d x \dfrac{dy}{dx} d x d y at t = ln 2 t = \ln 2 t = ln 2 .
Solution. d x d t = 2 sinh t \dfrac{dx}{dt} = 2\sinh t d t d x = 2 sinh t , d y d t = 3 cosh t \dfrac{dy}{dt} = 3\cosh t d t d y = 3 cosh t .
d y d x = ◆ L B ◆ 3 cosh t ◆ R B ◆◆ L B ◆ 2 sinh t ◆ R B ◆ = 3 2 coth t \frac{dy}{dx} = \frac◆LB◆3\cosh t◆RB◆◆LB◆2\sinh t◆RB◆ = \frac{3}{2}\coth t d x d y = L ◆ B ◆3 cosh t ◆ R B ◆◆ L B ◆2 sinh t ◆ R B ◆ = 2 3 coth t
At t = ln 2 t = \ln 2 t = ln 2 : cosh ( ln 2 ) = 2 + 1 / 2 2 = 5 4 \cosh(\ln 2) = \dfrac{2 + 1/2}{2} = \dfrac{5}{4} cosh ( ln 2 ) = 2 2 + 1/2 = 4 5 ,
sinh ( ln 2 ) = 2 − 1 / 2 2 = 3 4 \sinh(\ln 2) = \dfrac{2 - 1/2}{2} = \dfrac{3}{4} sinh ( ln 2 ) = 2 2 − 1/2 = 4 3 .
d y d x ∣ t = ln 2 = ◆ L B ◆ 3 ⋅ 5 / 4 ◆ R B ◆◆ L B ◆ 2 ⋅ 3 / 4 ◆ R B ◆ = 15 / 4 3 / 2 = 5 2 \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} d x d y t = l n 2 = L ◆ B ◆3 ⋅ 5/4◆ R B ◆◆ L B ◆2 ⋅ 3/4◆ R B ◆ = 3/2 15/4 = 2 5
Problem. Let I n = ∫ 0 π / 2 cosh n ( sin x ) d x I_n = \displaystyle\int_0^{\pi/2} \cosh^n(\sin x)\,dx I n = ∫ 0 π /2 cosh n ( sin x ) d x is not well-formed.
Instead, verify that
∫ tanh 3 x d x = ln ( cosh x ) − 1 2 s e c h 2 x tanh x + C \displaystyle\int \tanh^3 x\,dx = \ln(\cosh x) - \dfrac{1}{2}\mathrm{sech}^2\,x\tanh x + C ∫ tanh 3 x d x = ln ( cosh x ) − 2 1 sech 2 x tanh x + C is
incorrect, and find the correct integral.
Solution. Let us compute ∫ tanh 3 x d x \displaystyle\int \tanh^3 x\,dx ∫ tanh 3 x d x correctly.
Write
tanh 3 x = tanh x ⋅ tanh 2 x = tanh x ( 1 − s e c h 2 x ) = tanh x − tanh x s e c h 2 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 3 x = tanh x ⋅ tanh 2 x = tanh x ( 1 − sech 2 x ) = tanh x − tanh x sech 2 x .
∫ tanh 3 x d x = ∫ tanh x d x − ∫ tanh x s e c h 2 x d x \int \tanh^3 x\,dx = \int \tanh x\,dx - \int \tanh x\,\mathrm{sech}^2\,x\,dx ∫ tanh 3 x d x = ∫ tanh x d x − ∫ tanh x sech 2 x d x
The first integral: ∫ tanh x d x = ln ( cosh x ) + C \displaystyle\int\tanh x\,dx = \ln(\cosh x) + C ∫ tanh x d x = ln ( cosh x ) + C .
For the second integral, let u = tanh x u = \tanh x u = tanh x , d u = s e c h 2 x d x du = \mathrm{sech}^2\,x\,dx d u = sech 2 x d x :
∫ u d u = u 2 2 + C = ◆ L B ◆ tanh 2 x ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ + C \int u\,du = \frac{u^2}{2} + C = \frac◆LB◆\tanh^2 x◆RB◆◆LB◆2◆RB◆ + C ∫ u d u = 2 u 2 + C = L ◆ B ◆ tanh 2 x ◆ R B ◆◆ L B ◆2◆ R B ◆ + C
Therefore:
∫ tanh 3 x d x = ln ( cosh x ) − ◆ L B ◆ tanh 2 x ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ + C \boxed{\int \tanh^3 x\,dx = \ln(\cosh x) - \frac◆LB◆\tanh^2 x◆RB◆◆LB◆2◆RB◆ + C} ∫ tanh 3 x d x = ln ( cosh x ) − L ◆ B ◆ tanh 2 x ◆ R B ◆◆ L B ◆2◆ R B ◆ + C
Example 9.8: Arc length of a hyperbolic cosine curve Problem. Find the arc length of y = a cosh ( x / a ) y = a\cosh(x/a) y = a cosh ( x / a ) from x = 0 x = 0 x = 0 to x = b x = b x = b .
Solution. d y d x = sinh ( x / a ) \dfrac{dy}{dx} = \sinh(x/a) d x d y = sinh ( x / a ) .
s = ∫ 0 b ◆ L B ◆ 1 + sinh 2 ( x / a ) ◆ R B ◆ d x = ∫ 0 b cosh ( x / a ) d x = [ a sinh ( x / a ) ] 0 b = a sinh ( 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) s = ∫ 0 b ◆ L B ◆1 + sinh 2 ( x / a ) ◆ R B ◆ d x = ∫ 0 b cosh ( x / a ) d x = [ a sinh ( x / a ) ] 0 b = a sinh ( b / a )
10. Connections to Other Topics 10.1 Hyperbolic functions and differential equations The differential equation d 2 y d x 2 − y = 0 \dfrac{d^2y}{dx^2} - y = 0 d x 2 d 2 y − y = 0 has general solution
y = A cosh x + B sinh x y = A\cosh x + B\sinh x y = A cosh x + B sinh x , which can also be written y = C e x + D e − x y = Ce^x + De^{-x} y = C e x + D e − x . See
Differential Equations .
10.2 Hyperbolic functions and complex numbers The identities cosh x = cos ( i x ) \cosh x = \cos(ix) cosh x = cos ( i x ) and sinh x = − i sin ( i x ) \sinh x = -i\sin(ix) sinh x = − i sin ( i x ) connect the two topics. See
Complex Numbers .
10.3 Hyperbolic functions and integration techniques Hyperbolic substitutions (x = a sinh u x = a\sinh u x = a sinh u , x = a cosh u x = a\cosh u x = a cosh u ) are powerful alternatives to trigonometric
substitutions. See
Further Calculus .
10.4 The catenary and mechanics The shape y = a cosh ( x / a ) y = a\cosh(x/a) y = a cosh ( x / a ) describes a hanging chain. The arc length is s = a sinh ( x / a ) s = a\sinh(x/a) s = a sinh ( x / a ) . See
Further Mechanics .
11. Additional Exam-Style Questions Question 8 (a) Given sinh x = 12 5 \sinh x = \dfrac{12}{5} sinh x = 5 12 , find the exact value of cosh x \cosh x cosh x and tanh x \tanh x tanh x .
(b) Hence evaluate arcosh ( 13 5 ) \operatorname{arcosh}\!\left(\dfrac{13}{5}\right) arcosh ( 5 13 ) in exact logarithmic
form.
Solution (a) cosh 2 x = 1 + sinh 2 x = 1 + 144 25 = 169 25 \cosh^2 x = 1 + \sinh^2 x = 1 + \dfrac{144}{25} = \dfrac{169}{25} cosh 2 x = 1 + sinh 2 x = 1 + 25 144 = 25 169 , so
cosh x = 13 5 \cosh x = \dfrac{13}{5} cosh x = 5 13 (positive root).
tanh x = ◆ L B ◆ sinh x ◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = 12 / 5 13 / 5 = 12 13 \tanh x = \dfrac◆LB◆\sinh x◆RB◆◆LB◆\cosh x◆RB◆ = \dfrac{12/5}{13/5} = \dfrac{12}{13} tanh x = L ◆ B ◆ sinh x ◆ R B ◆◆ L B ◆ cosh x ◆ R B ◆ = 13/5 12/5 = 13 12 .
(b) Since cosh x = 13 5 \cosh x = \dfrac{13}{5} cosh x = 5 13 :
arcosh ( 13 5 ) = x = ln ( 13 5 + ◆ L B ◆ 169 25 − 1 ◆ R B ◆ ) = ln ( 13 5 + 12 5 ) = ln 5 \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 arcosh ( 5 13 ) = x = ln ( 5 13 + ◆ L B ◆ 25 169 − 1◆ R B ◆ ) = ln ( 5 13 + 5 12 ) = ln 5
Question 9 Find the exact value of ∫ 0 ln 2 cosh 2 x d x \displaystyle\int_0^{\ln 2} \cosh 2x\,dx ∫ 0 l n 2 cosh 2 x d x .
Solution ∫ 0 ln 2 cosh 2 x d x = [ ◆ L B ◆ sinh 2 x ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ] 0 ln 2 = ◆ L B ◆ sinh ( 2 ln 2 ) ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \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◆ ∫ 0 l n 2 cosh 2 x d x = [ L ◆ B ◆ sinh 2 x ◆ R B ◆◆ L B ◆2◆ R B ◆ ] 0 l n 2 = L ◆ B ◆ sinh ( 2 ln 2 ) ◆ R B ◆◆ L B ◆2◆ R B ◆
sinh ( 2 ln 2 ) = ◆ L B ◆ e 2 ln 2 − e − 2 ln 2 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = 4 − 1 / 4 2 = 15 8 \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} sinh ( 2 ln 2 ) = L ◆ B ◆ e 2 l n 2 − e − 2 l n 2 ◆ R B ◆◆ L B ◆2◆ R B ◆ = 2 4 − 1/4 = 8 15 .
∫ 0 ln 2 cosh 2 x d x = 15 16 \int_0^{\ln 2}\cosh 2x\,dx = \frac{15}{16} ∫ 0 l n 2 cosh 2 x d x = 16 15
Question 10 Prove by induction that d n d x n ( sinh x ) = sinh x \dfrac{d^n}{dx^n}(\sinh x) = \sinh x d x n d n ( sinh x ) = sinh x when n n n is even and
d n d x n ( sinh x ) = cosh x \dfrac{d^n}{dx^n}(\sinh x) = \cosh x d x n d n ( sinh x ) = cosh x when n n n is odd.
Solution Base case (n = 0 n = 0 n = 0 ): d 0 d x 0 ( sinh x ) = sinh x \dfrac{d^0}{dx^0}(\sinh x) = \sinh x d x 0 d 0 ( sinh x ) = sinh x . Correct for n = 0 n = 0 n = 0 (even).
Base case (n = 1 n = 1 n = 1 ): d d x ( sinh x ) = cosh x \dfrac{d}{dx}(\sinh x) = \cosh x d x d ( sinh x ) = cosh x . Correct for n = 1 n = 1 n = 1 (odd).
Inductive step. Assume the result holds for n = k n = k n = k .
If k k k is even: d k d x k ( sinh x ) = sinh x \dfrac{d^k}{dx^k}(\sinh x) = \sinh x d x k d k ( sinh x ) = sinh x . Then
d k + 1 d x k + 1 ( sinh x ) = d d x ( sinh x ) = cosh x \dfrac{d^{k+1}}{dx^{k+1}}(\sinh x) = \dfrac{d}{dx}(\sinh x) = \cosh x d x k + 1 d k + 1 ( sinh x ) = d x d ( sinh x ) = cosh x . Since k + 1 k + 1 k + 1 is odd, the
result holds.
If k k k is odd: d k d x k ( sinh x ) = cosh x \dfrac{d^k}{dx^k}(\sinh x) = \cosh x d x k d k ( sinh x ) = cosh x . Then
d k + 1 d x k + 1 ( sinh x ) = d d x ( cosh x ) = sinh x \dfrac{d^{k+1}}{dx^{k+1}}(\sinh x) = \dfrac{d}{dx}(\cosh x) = \sinh x d x k + 1 d k + 1 ( sinh x ) = d x d ( cosh x ) = sinh x . Since k + 1 k + 1 k + 1 is even, the
result holds. ■ \blacksquare ■
Question 11 Evaluate ∫ 3 / 2 2 ◆ L B ◆ 3 ◆ R B ◆◆ L B ◆ 4 x 2 − 9 ◆ R B ◆ d x \displaystyle\int_{3/2}^2 \frac◆LB◆3◆RB◆◆LB◆\sqrt{4x^2 - 9}◆RB◆\,dx ∫ 3/2 2 L ◆ B ◆3◆ R B ◆◆ L B ◆ 4 x 2 − 9 ◆ R B ◆ d x in exact form.
Solution ∫ 3 / 2 2 ◆ L B ◆ 3 ◆ R B ◆◆ L B ◆ 4 x 2 − 9 ◆ R B ◆ d x = 3 2 ∫ 3 / 2 2 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 9 / 4 ◆ R B ◆ = 3 2 [ arcosh ( 2 x 3 ) ] 3 / 2 2 \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 ∫ 3/2 2 L ◆ B ◆3◆ R B ◆◆ L B ◆ 4 x 2 − 9 ◆ R B ◆ d x = 2 3 ∫ 3/2 2 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 9/4 ◆ R B ◆ = 2 3 [ arcosh ( 3 2 x ) ] 3/2 2
= 3 2 [ arcosh ( 4 3 ) − arcosh ( 1 ) ] = 3 2 arcosh ( 4 3 ) = \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) = 2 3 [ arcosh ( 3 4 ) − arcosh ( 1 ) ] = 2 3 arcosh ( 3 4 )
= 3 2 ln ( 4 3 + ◆ L B ◆ 16 9 − 1 ◆ R B ◆ ) = 3 2 ln ( ◆ L B ◆ 4 + 7 ◆ R B ◆◆ L B ◆ 3 ◆ R B ◆ ) = \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) = 2 3 ln ( 3 4 + ◆ L B ◆ 9 16 − 1◆ R B ◆ ) = 2 3 ln ( L ◆ B ◆4 + 7 ◆ R B ◆◆ L B ◆3◆ R B ◆ )
Question 12 Given that y = ln ( sinh x ) y = \ln(\sinh x) y = ln ( sinh x ) , show that d 2 y d x 2 = − c o s e c h 2 x \dfrac{d^2y}{dx^2} = -\mathrm{cosech}^2\,x d x 2 d 2 y = − cosech 2 x .
Solution d y d x = ◆ L B ◆ cosh x ◆ R B ◆◆ L B ◆ sinh x ◆ R B ◆ = coth x \frac{dy}{dx} = \frac◆LB◆\cosh x◆RB◆◆LB◆\sinh x◆RB◆ = \coth x d x d y = L ◆ B ◆ cosh x ◆ R B ◆◆ L B ◆ sinh x ◆ R B ◆ = coth x
d 2 y d x 2 = d d x ( coth x ) = − c o s e c h 2 x = ◆ L B ◆ − 1 ◆ R B ◆◆ L B ◆ sinh 2 x ◆ R B ◆ ■ \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 d x 2 d 2 y = d x d ( coth x ) = − cosech 2 x = L ◆ B ◆ − 1◆ R B ◆◆ L B ◆ sinh 2 x ◆ R B ◆ ■
Question 13 (a) Express sinh ( 2 ln 3 ) \sinh(2\ln 3) sinh ( 2 ln 3 ) in the form a b \dfrac{a}{b} b a where a , b a, b a , b are integers.
(b) Hence find ln 3 − ln 2 \ln 3 - \ln 2 ln 3 − ln 2 in terms of inverse hyperbolic functions.
Solution (a) sinh ( 2 ln 3 ) = 2 sinh ( ln 3 ) cosh ( ln 3 ) \sinh(2\ln 3) = 2\sinh(\ln 3)\cosh(\ln 3) sinh ( 2 ln 3 ) = 2 sinh ( ln 3 ) cosh ( ln 3 ) .
sinh ( ln 3 ) = 3 − 1 / 3 2 = 4 3 \sinh(\ln 3) = \dfrac{3 - 1/3}{2} = \dfrac{4}{3} sinh ( ln 3 ) = 2 3 − 1/3 = 3 4 ,
cosh ( ln 3 ) = 3 + 1 / 3 2 = 5 3 \cosh(\ln 3) = \dfrac{3 + 1/3}{2} = \dfrac{5}{3} cosh ( ln 3 ) = 2 3 + 1/3 = 3 5 .
sinh ( 2 ln 3 ) = 2 ⋅ 4 3 ⋅ 5 3 = 40 9 \sinh(2\ln 3) = 2 \cdot \dfrac{4}{3} \cdot \dfrac{5}{3} = \dfrac{40}{9} sinh ( 2 ln 3 ) = 2 ⋅ 3 4 ⋅ 3 5 = 9 40 .
(b) ln 3 − ln 2 = ln ( 3 / 2 ) \ln 3 - \ln 2 = \ln(3/2) ln 3 − ln 2 = ln ( 3/2 ) . Since arsinh x = ln ( x + x 2 + 1 ) \operatorname{arsinh}\,x = \ln(x + \sqrt{x^2+1}) arsinh x = ln ( x + x 2 + 1 ) :
arsinh ( 3 4 ) = ln ( 3 4 + ◆ L B ◆ 9 16 + 1 ◆ R B ◆ ) = ln ( 3 4 + 5 4 ) = ln 2 \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 arsinh ( 4 3 ) = ln ( 4 3 + ◆ L B ◆ 16 9 + 1◆ R B ◆ ) = ln ( 4 3 + 4 5 ) = ln 2 .
Therefore ln 2 = arsinh ( 3 / 4 ) \ln 2 = \operatorname{arsinh}(3/4) ln 2 = 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) ln 3 = ln 2 + ln ( 3/2 ) = arsinh ( 3/4 ) + artanh ( 1/5 ) (using
artanh ( 1 / 5 ) = 1 2 ln ( 6 / 4 ) = 1 2 ln ( 3 / 2 ) \operatorname{artanh}(1/5) = \frac{1}{2}\ln(6/4) = \frac{1}{2}\ln(3/2) artanh ( 1/5 ) = 2 1 ln ( 6/4 ) = 2 1 ln ( 3/2 ) ).
So ln 3 − ln 2 = artanh ( 1 / 5 ) \ln 3 - \ln 2 = \operatorname{artanh}(1/5) ln 3 − ln 2 = artanh ( 1/5 ) .
12. Summary of Extended Results Identity Formula Triple angle sinh 3 x = 3 sinh x + 4 sinh 3 x \sinh 3x = 3\sinh x + 4\sinh^3 x sinh 3 x = 3 sinh x + 4 sinh 3 x Triple angle cosh 3 x = 4 cosh 3 x − 3 cosh x \cosh 3x = 4\cosh^3 x - 3\cosh x cosh 3 x = 4 cosh 3 x − 3 cosh x Half angle cosh 2 ( x 2 ) = ◆ L B ◆ 1 + cosh x ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \cosh^2\!\left(\dfrac{x}{2}\right) = \dfrac◆LB◆1 + \cosh x◆RB◆◆LB◆2◆RB◆ cosh 2 ( 2 x ) = L ◆ B ◆1 + cosh x ◆ R B ◆◆ L B ◆2◆ R B ◆ Half angle sinh 2 ( x 2 ) = ◆ L B ◆ cosh x − 1 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \sinh^2\!\left(\dfrac{x}{2}\right) = \dfrac◆LB◆\cosh x - 1◆RB◆◆LB◆2◆RB◆ sinh 2 ( 2 x ) = L ◆ B ◆ cosh x − 1◆ R B ◆◆ L B ◆2◆ R B ◆ Integral of tanh \tanh tanh ∫ tanh x d x = ln ( cosh x ) + C \displaystyle\int\tanh x\,dx = \ln(\cosh x) + C ∫ tanh x d x = ln ( cosh x ) + C Integral of coth \coth coth ∫ coth x d x = ln ( sinh x ) + C \displaystyle\int\coth x\,dx = \ln(\sinh x) + C ∫ coth x d x = ln ( sinh x ) + C Integral of tanh 3 \tanh^3 tanh 3 ∫ tanh 3 x d x = ln ( cosh x ) − ◆ L B ◆ tanh 2 x ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ + C \displaystyle\int\tanh^3 x\,dx = \ln(\cosh x) - \dfrac◆LB◆\tanh^2 x◆RB◆◆LB◆2◆RB◆ + C ∫ tanh 3 x d x = ln ( cosh x ) − L ◆ B ◆ tanh 2 x ◆ R B ◆◆ L B ◆2◆ R B ◆ + C Arc length of catenary s = a sinh ( b / a ) s = a\sinh(b/a) s = a sinh ( b / a ) for y = a cosh ( x / a ) y = a\cosh(x/a) y = a cosh ( x / a )
13. Further Common Pitfalls
Substitution domain errors: When using x = a cosh u x = a\cosh u x = a cosh u , the substitution requires x ≥ a x \geq a x ≥ a
(since cosh u ≥ 1 \cosh u \geq 1 cosh u ≥ 1 ). Attempting to use x = a cosh u x = a\cosh u x = a cosh u for x < a x < a x < a leads to an error. Use
x = a sinh u x = a\sinh u x = a sinh u for x 2 + a 2 \sqrt{x^2 + a^2} x 2 + a 2 and x = a cosh u x = a\cosh u x = a cosh u for x 2 − a 2 \sqrt{x^2 - a^2} x 2 − a 2 .
Confusing artanh \operatorname{artanh} artanh and ln \ln ln forms: The formula
∫ d x a 2 − x 2 = 1 2 a ln ∣ a + x a − x ∣ \displaystyle\int\frac{dx}{a^2 - x^2} = \frac{1}{2a}\ln\!\left|\frac{a+x}{a-x}\right| ∫ a 2 − x 2 d x = 2 a 1 ln a − x a + x is valid
for all ∣ x ∣ ≠ a |x| \neq a ∣ x ∣ = a , but 1 a artanh ( x / a ) \dfrac{1}{a}\operatorname{artanh}(x/a) a 1 artanh ( x / a ) is only valid for ∣ x ∣ < a |x| < a ∣ x ∣ < a .
For ∣ x ∣ > a |x| > a ∣ x ∣ > a , use the logarithmic form or arcoth \operatorname{arcoth} arcoth .
No absolute value needed for cosh \cosh cosh : Unlike ∣ cos x ∣ |\cos x| ∣ cos x ∣ , ◆ L B ◆ cosh 2 x ◆ R B ◆ = cosh x \sqrt◆LB◆\cosh^2 x◆RB◆ = \cosh x ◆ L B ◆ cosh 2 x ◆ R B ◆ = cosh x
(no absolute value needed) since cosh x ≥ 1 > 0 \cosh x \geq 1 > 0 cosh x ≥ 1 > 0 for all real x x x .
Differential equation solutions: The equation y ′ ′ − y = 0 y'' - y = 0 y ′′ − y = 0 has solutions in both exponential
and hyperbolic forms. When boundary conditions involve y ( 0 ) y(0) y ( 0 ) and y ′ ( 0 ) y'(0) y ′ ( 0 ) , the hyperbolic form
y = A cosh x + B sinh x y = A\cosh x + B\sinh x y = A cosh x + B sinh x is often more convenient since cosh 0 = 1 \cosh 0 = 1 cosh 0 = 1 and sinh 0 = 0 \sinh 0 = 0 sinh 0 = 0 . :::
14. Advanced Worked Examples Example 14.1: Integration using sinh \sinh sinh substitution Problem. Evaluate ∫ x 2 + 9 d x \displaystyle\int \sqrt{x^2 + 9}\,dx ∫ x 2 + 9 d x .
Solution. Let x = 3 sinh u x = 3\sinh u x = 3 sinh u , d x = 3 cosh u d u dx = 3\cosh u\,du d x = 3 cosh u d u .
∫ 3 cosh u ⋅ 3 cosh u d u = 9 ∫ cosh 2 u d u = 9 ∫ ◆ L B ◆ 1 + cosh 2 u ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ d u = 9 2 ( u + ◆ L B ◆ sinh 2 u ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ) \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) ∫ 3 cosh u ⋅ 3 cosh u d u = 9 ∫ cosh 2 u d u = 9 ∫ L ◆ B ◆1 + cosh 2 u ◆ R B ◆◆ L B ◆2◆ R B ◆ d u = 2 9 ( u + L ◆ B ◆ sinh 2 u ◆ R B ◆◆ L B ◆2◆ R B ◆ )
= 9 u 2 + ◆ L B ◆ 9 sinh u cosh u ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = 9 2 arsinh ( x 3 ) + ◆ L B ◆ x x 2 + 9 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ + 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 = 2 9 u + L ◆ B ◆9 sinh u cosh u ◆ R B ◆◆ L B ◆2◆ R B ◆ = 2 9 arsinh ( 3 x ) + L ◆ B ◆ x x 2 + 9 ◆ R B ◆◆ L B ◆2◆ R B ◆ + C
Example 14.2: Solving y ′ ′ − 4 y = 0 y'' - 4y = 0 y ′′ − 4 y = 0 with hyperbolic functions Problem. Solve y ′ ′ − 4 y = 0 y'' - 4y = 0 y ′′ − 4 y = 0 with y ( 0 ) = 3 y(0) = 3 y ( 0 ) = 3 and y ′ ( 0 ) = 8 y'(0) = 8 y ′ ( 0 ) = 8 .
Solution. Auxiliary: m 2 − 4 = 0 ⟹ m = ± 2 m^2 - 4 = 0 \implies m = \pm 2 m 2 − 4 = 0 ⟹ m = ± 2 .
y = A cosh 2 x + B sinh 2 x y = A\cosh 2x + B\sinh 2x y = A cosh 2 x + B sinh 2 x .
y ( 0 ) = A = 3 y(0) = A = 3 y ( 0 ) = A = 3 . y ′ ( 0 ) = 2 B = 8 ⟹ B = 4 y'(0) = 2B = 8 \implies B = 4 y ′ ( 0 ) = 2 B = 8 ⟹ B = 4 .
y = 3 cosh 2 x + 4 sinh 2 x \boxed{y = 3\cosh 2x + 4\sinh 2x} y = 3 cosh 2 x + 4 sinh 2 x
In exponential form:
y = 3 ⋅ e 2 x + e − 2 x 2 + 4 ⋅ e 2 x − e − 2 x 2 = 7 2 e 2 x − 1 2 e − 2 x y = 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} y = 3 ⋅ 2 e 2 x + e − 2 x + 4 ⋅ 2 e 2 x − e − 2 x = 2 7 e 2 x − 2 1 e − 2 x .
Example 14.3: Arc length of a catenary Problem. Find the arc length of y = cosh x y = \cosh x y = cosh x from x = 0 x = 0 x = 0 to x = 1 x = 1 x = 1 .
Solution. y ′ = sinh x y' = \sinh x y ′ = sinh x . d s = ◆ L B ◆ 1 + sinh 2 x ◆ R B ◆ d x = cosh x d x ds = \sqrt◆LB◆1 + \sinh^2 x◆RB◆\,dx = \cosh x\,dx d s = ◆ L B ◆1 + sinh 2 x ◆ R B ◆ d x = cosh x d x .
s = ∫ 0 1 cosh x d x = [ sinh x ] 0 1 = sinh 1 = e − e − 1 2 ≈ 1.175 s = \int_0^1 \cosh x\,dx = [\sinh x]_0^1 = \sinh 1 = \frac{e - e^{-1}}{2} \approx \boxed{1.175} s = ∫ 0 1 cosh x d x = [ sinh x ] 0 1 = sinh 1 = 2 e − e − 1 ≈ 1.175
Example 14.4: Osborn's rule applied to tan 2 x \tan 2x tan 2 x Problem. Using Osborn's rule, find tanh 2 x \tanh 2x tanh 2 x in terms of tanh x \tanh x tanh x .
Solution. tan 2 x = ◆ L B ◆ 2 tan x ◆ R B ◆◆ L B ◆ 1 − tan 2 x ◆ R B ◆ \tan 2x = \dfrac◆LB◆2\tan x◆RB◆◆LB◆1-\tan^2 x◆RB◆ tan 2 x = L ◆ B ◆2 tan x ◆ R B ◆◆ L B ◆1 − tan 2 x ◆ R B ◆ . Apply Osborn's rule (change
tan 2 x \tan^2 x tan 2 x to − tanh 2 x -\tanh^2 x − tanh 2 x ):
tanh 2 x = ◆ L B ◆ 2 tanh x ◆ R B ◆◆ L B ◆ 1 + tanh 2 x ◆ R B ◆ \boxed{\tanh 2x = \frac◆LB◆2\tanh x◆RB◆◆LB◆1+\tanh^2 x◆RB◆} tanh 2 x = L ◆ B ◆2 tanh x ◆ R B ◆◆ L B ◆1 + tanh 2 x ◆ R B ◆
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 sec θ = cosh u where u = gd − 1 ( θ ) u = \operatorname{gd}^{-1}(\theta) u = gd − 1 ( θ ) . Show that
◆ L B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = sech u \dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = \operatorname{sech}\, u L ◆ B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = sech u .
Solution. sec θ = cosh u ⟹ cos θ = sech u \sec\theta = \cosh u \implies \cos\theta = \operatorname{sech}\, u sec θ = cosh u ⟹ cos θ = sech u .
Differentiating implicitly with respect to u u u :
− sin θ ⋅ ◆ L B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = − sech u tanh u -\sin\theta \cdot \dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = -\operatorname{sech}\,u \tanh u − sin θ ⋅ L ◆ B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = − sech u tanh u .
◆ L B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = ◆ L B ◆ sech u tanh u ◆ R B ◆◆ L B ◆ sin θ ◆ R B ◆ \dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = \dfrac◆LB◆\operatorname{sech}\,u \tanh u◆RB◆◆LB◆\sin\theta◆RB◆ L ◆ B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = L ◆ B ◆ sech u tanh u ◆ R B ◆◆ L B ◆ sin θ ◆ R B ◆ .
Since cos θ = sech u \cos\theta = \operatorname{sech}\,u cos θ = sech u :
sin θ = ◆ L B ◆ 1 − sech 2 u ◆ R B ◆ = ◆ L B ◆ 1 − ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ cosh 2 u ◆ R B ◆◆ R B ◆ = ◆ L B ◆ ◆ L B ◆ cosh 2 u − 1 ◆ R B ◆◆ R B ◆◆ L B ◆ cosh u ◆ R B ◆ = ◆ L B ◆ sinh u ◆ R B ◆◆ L B ◆ cosh u ◆ R B ◆ = tanh u \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 sin θ = ◆ L B ◆1 − sech 2 u ◆ R B ◆ = ◆ L B ◆1 − L ◆ B ◆1◆ R B ◆◆ L B ◆ cosh 2 u ◆ R B ◆◆ R B ◆ = L ◆ B ◆ ◆ L B ◆ cosh 2 u − 1◆ R B ◆◆ R B ◆◆ L B ◆ cosh u ◆ R B ◆ = L ◆ B ◆ sinh u ◆ R B ◆◆ L B ◆ cosh u ◆ R B ◆ = tanh u .
◆ L B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = ◆ L B ◆ sech u tanh u ◆ R B ◆◆ L B ◆ tanh u ◆ R B ◆ = sech u \dfrac◆LB◆d\theta◆RB◆◆LB◆du◆RB◆ = \dfrac◆LB◆\operatorname{sech}\,u \tanh u◆RB◆◆LB◆\tanh u◆RB◆ = \boxed{\operatorname{sech}\,u} L ◆ B ◆ d θ ◆ R B ◆◆ L B ◆ d u ◆ R B ◆ = L ◆ B ◆ sech u tanh u ◆ R B ◆◆ L B ◆ tanh u ◆ R B ◆ = sech u .
■ \blacksquare ■
15. Additional Exam-Style Questions Question 16 Evaluate ∫ 1 2 ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ \displaystyle\int_1^2 \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2 - 1}◆RB◆ ∫ 1 2 L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ .
Solution = [ arcosh x ] 1 2 = ln ( 2 + 3 ) − ln 1 = ln ( 2 + 3 ) = [\operatorname{arcosh}\, x]_1^2 = \ln(2+\sqrt{3}) - \ln 1 = \boxed{\ln(2+\sqrt{3})} = [ arcosh x ] 1 2 = ln ( 2 + 3 ) − ln 1 = ln ( 2 + 3 ) .
Question 17 Prove that sinh ( x + y ) = sinh x cosh y + cosh x sinh y \sinh(x+y) = \sinh x\cosh y + \cosh x\sinh y sinh ( x + y ) = sinh x cosh y + cosh x sinh y .
Solution sinh x cosh y + cosh x sinh y = ( e x − e − x ) ( e y + e − y ) + ( e x + e − x ) ( e y − 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} sinh x cosh y + cosh x sinh y = 4 ( e x − e − x ) ( e y + e − y ) + ( e x + e − x ) ( e y − e − y )
= 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 = \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} = 4 e x + y + e x − y − e − x + y − e − x − y + e x + y − e x − y + e − x + y − e − x − y
= 2 e x + y − 2 e − ( x + y ) 4 = e x + 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) = 4 2 e x + y − 2 e − ( x + y ) = 2 e x + y − e − ( x + y ) = sinh ( x + y ) . ■ \blacksquare ■
Question 18 Find d d x [ arcosh x ] \dfrac{d}{dx}[\operatorname{arcosh}\, x] d x d [ arcosh x ] and state the domain.
Solution Let y = arcosh x y = \operatorname{arcosh}\, x y = arcosh x , so x = cosh y x = \cosh y x = cosh y and x ≥ 1 x \geq 1 x ≥ 1 .
1 = sinh y ⋅ d y d x 1 = \sinh y \cdot \dfrac{dy}{dx} 1 = sinh y ⋅ d x d y .
d y d x = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ sinh y ◆ R B ◆ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ ◆ L B ◆ cosh 2 y − 1 ◆ R B ◆◆ R B ◆ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ \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◆ d x d y = L ◆ B ◆1◆ R B ◆◆ L B ◆ sinh y ◆ R B ◆ = L ◆ B ◆1◆ R B ◆◆ L B ◆ ◆ L B ◆ cosh 2 y − 1◆ R B ◆◆ R B ◆ = L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ .
d d x [ arcosh x ] = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ \boxed{\dfrac{d}{dx}[\operatorname{arcosh}\, x] = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{x^2-1}◆RB◆} d x d [ arcosh x ] = L ◆ B ◆1◆ R B ◆◆ L B ◆ x 2 − 1 ◆ R B ◆ for
x > 1 x > 1 x > 1 .
16. Advanced Topics 16.1 The Gudermannian function The Gudermannian function g d ( x ) \mathrm{gd}(x) gd ( x ) relates circular and hyperbolic functions without complex
numbers:
sin ( g d x ) = tanh x \sin(\mathrm{gd}\,x) = \tanh x sin ( gd x ) = tanh x , cos ( g d x ) = s e c h x \cos(\mathrm{gd}\,x) = \mathrm{sech}\,x cos ( gd x ) = sech x ,
tan ( g d x ) = sinh x \tan(\mathrm{gd}\,x) = \sinh x tan ( gd x ) = sinh x .
d d x g d ( x ) = s e c h x \dfrac{d}{dx}\mathrm{gd}(x) = \mathrm{sech}\,x d x d gd ( x ) = sech x .
In special relativity, the Lorentz transformation uses hyperbolic functions. If β = v / c \beta = v/c β = v / c and
γ = ( 1 − β 2 ) − 1 / 2 = cosh ϕ \gamma = (1-\beta^2)^{-1/2} = \cosh\phi γ = ( 1 − β 2 ) − 1/2 = cosh ϕ where tanh ϕ = β \tanh\phi = \beta tanh ϕ = β , then:
t ′ = t cosh ϕ − x sinh ϕ / c t' = t\cosh\phi - x\sinh\phi/c t ′ = t cosh ϕ − x sinh ϕ / c , x ′ = x cosh ϕ − c t sinh ϕ x' = x\cosh\phi - ct\sinh\phi x ′ = x cosh ϕ − c t sinh ϕ .
| Function | Logarithmic Form | Domain |
| -------------------------- | -------------------------------------------------------------- | -------------- | --- | ---- |
| arsinh x \operatorname{arsinh}\,x arsinh x | ln ( x + x 2 + 1 ) \ln(x+\sqrt{x^2+1}) ln ( x + x 2 + 1 ) | all real x x x |
| arcosh x \operatorname{arcosh}\,x arcosh x | ln ( x + x 2 − 1 ) \ln(x+\sqrt{x^2-1}) ln ( x + x 2 − 1 ) | x ≥ 1 x \geq 1 x ≥ 1 |
| artanh x \operatorname{artanh}\,x artanh x | 1 2 ln ( 1 + x 1 − x ) \dfrac{1}{2}\ln\!\left(\dfrac{1+x}{1-x}\right) 2 1 ln ( 1 − x 1 + x ) | ∣ x ∣ < 1 | x | < 1 ∣ x ∣ < 1 |
| arcoth x \operatorname{arcoth}\,x arcoth x | 1 2 ln ( x + 1 x − 1 ) \dfrac{1}{2}\ln\!\left(\dfrac{x+1}{x-1}\right) 2 1 ln ( x − 1 x + 1 ) | ∣ x ∣ > 1 | x | > 1 ∣ x ∣ > 1 |
| arsech x \operatorname{arsech}\,x arsech x | ln ( ◆ L B ◆ 1 + 1 − x 2 ◆ R B ◆◆ L B ◆ x ◆ R B ◆ ) \ln\!\left(\dfrac◆LB◆1+\sqrt{1-x^2}◆RB◆◆LB◆x◆RB◆\right) ln ( L ◆ B ◆1 + 1 − x 2 ◆ R B ◆◆ L B ◆ x ◆ R B ◆ ) | 0 < x ≤ 1 0 < x \leq 1 0 < x ≤ 1 |
| arcsch x \operatorname{arcsch}\,x arcsch x | ln ( 1 x + ◆ L B ◆ 1 x 2 + 1 ◆ R B ◆ ) \ln\!\left(\dfrac{1}{x}+\sqrt◆LB◆\dfrac{1}{x^2}+1◆RB◆\right) ln ( x 1 + ◆ L B ◆ x 2 1 + 1◆ R B ◆ ) | x ≠ 0 x \neq 0 x = 0 |
16.4 Hyperbolic functions and catenary applications The catenary y = a cosh ( x / a ) y = a\cosh(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 2 cosh x − sinh x = 3 2\cosh x - \sinh x = 3 2 cosh x − sinh x = 3 .
Solution 2 ⋅ e x + e − x 2 − e x − e − x 2 = 3 2\cdot\dfrac{e^x+e^{-x}}{2} - \dfrac{e^x-e^{-x}}{2} = 3 2 ⋅ 2 e x + e − x − 2 e x − e − x = 3 .
e x + e − x − e x 2 + e − x 2 = 3 e^x+e^{-x} - \dfrac{e^x}{2} + \dfrac{e^{-x}}{2} = 3 e x + e − x − 2 e x + 2 e − x = 3 .
e x 2 + 3 e − x 2 = 3 ⟹ e x + 3 e − x = 6 \dfrac{e^x}{2} + \dfrac{3e^{-x}}{2} = 3 \implies e^x + 3e^{-x} = 6 2 e x + 2 3 e − x = 3 ⟹ e x + 3 e − x = 6 .
e 2 x − 6 e x + 3 = 0 e^{2x} - 6e^x + 3 = 0 e 2 x − 6 e x + 3 = 0 .
e x = ◆ L B ◆ 6 ± 36 − 12 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = 3 ± 6 e^x = \dfrac◆LB◆6 \pm \sqrt{36-12}◆RB◆◆LB◆2◆RB◆ = 3 \pm \sqrt{6} e x = L ◆ B ◆6 ± 36 − 12 ◆ R B ◆◆ L B ◆2◆ R B ◆ = 3 ± 6 .
x = ln ( 3 + 6 ) x = \ln(3+\sqrt{6}) x = ln ( 3 + 6 ) or x = ln ( 3 − 6 ) x = \ln(3-\sqrt{6}) x = ln ( 3 − 6 ) .
Since 3 − 6 > 0 3-\sqrt{6} > 0 3 − 6 > 0 , both are valid.
Question 20 Prove that arcosh x = ln ( x + x 2 − 1 ) \operatorname{arcosh}\,x = \ln(x+\sqrt{x^2-1}) arcosh x = ln ( x + x 2 − 1 ) for x ≥ 1 x \geq 1 x ≥ 1 .
Solution Let y = arcosh x y = \operatorname{arcosh}\,x y = arcosh x , so x = cosh y = e y + e − y 2 x = \cosh y = \dfrac{e^y+e^{-y}}{2} x = cosh y = 2 e y + e − y .
2 x = e y + e − y ⟹ e 2 y − 2 x e y + 1 = 0 2x = e^y + e^{-y} \implies e^{2y} - 2xe^y + 1 = 0 2 x = e y + e − y ⟹ e 2 y − 2 x e y + 1 = 0 .
e y = ◆ L B ◆ 2 x ± 4 x 2 − 4 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = x ± x 2 − 1 e^y = \dfrac◆LB◆2x \pm \sqrt{4x^2-4}◆RB◆◆LB◆2◆RB◆ = x \pm \sqrt{x^2-1} e y = L ◆ B ◆2 x ± 4 x 2 − 4 ◆ R B ◆◆ L B ◆2◆ R B ◆ = x ± x 2 − 1 .
Since e y ≥ 1 e^y \geq 1 e y ≥ 1 and x ≥ 1 x \geq 1 x ≥ 1 : e y = x + x 2 − 1 e^y = x + \sqrt{x^2-1} e y = x + x 2 − 1 (the positive root, since
x − x 2 − 1 ≤ 1 x-\sqrt{x^2-1} \leq 1 x − x 2 − 1 ≤ 1 ).
y = ln ( x + x 2 − 1 ) y = \ln(x+\sqrt{x^2-1}) y = ln ( x + x 2 − 1 ) . ■ \blacksquare ■
17. Further Advanced Topics 17.1 Hyperbolic substitutions in integration Standard substitutions:
x 2 + a 2 \sqrt{x^2+a^2} x 2 + a 2 : use x = a cosh t x = a\cosh t x = a cosh t
x 2 − a 2 \sqrt{x^2-a^2} x 2 − a 2 : use x = a cosh t x = a\cosh t x = a cosh t (for x ≥ a x \geq a x ≥ a )
a 2 − x 2 \sqrt{a^2-x^2} a 2 − x 2 : use x = a cos t x = a\cos t x = a cos t (circular, not hyperbolic)
Example: ∫ ◆ L B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 4 ◆ R B ◆ \displaystyle\int \frac◆LB◆dx◆RB◆◆LB◆\sqrt{x^2-4}◆RB◆ ∫ L ◆ B ◆ d x ◆ R B ◆◆ L B ◆ x 2 − 4 ◆ R B ◆ with x = 2 cosh t x = 2\cosh t x = 2 cosh t :
d x = 2 sinh t d t dx = 2\sinh t\,dt d x = 2 sinh t d t , x 2 − 4 = 2 sinh t \sqrt{x^2-4} = 2\sinh t x 2 − 4 = 2 sinh t .
∫ ◆ L B ◆ 2 sinh t ◆ R B ◆◆ L B ◆ 2 sinh t ◆ R B ◆ d t = t = arcosh ( x 2 ) + C \displaystyle\int \frac◆LB◆2\sinh t◆RB◆◆LB◆2\sinh t◆RB◆\,dt = t = \operatorname{arcosh}\!\left(\frac{x}{2}\right) + C ∫ L ◆ B ◆2 sinh t ◆ R B ◆◆ L B ◆2 sinh t ◆ R B ◆ d t = t = arcosh ( 2 x ) + C .
17.2 Gudermannian function The Gudermannian function relates circular and hyperbolic functions without complex numbers:
gd ( x ) = ∫ 0 x sech t d t = 2 arctan ( e x ) − ◆ L B ◆ π ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \operatorname{gd}(x) = \int_0^x \operatorname{sech} t\,dt = 2\arctan(e^x) - \frac◆LB◆\pi◆RB◆◆LB◆2◆RB◆ gd ( x ) = ∫ 0 x sech t d t = 2 arctan ( e x ) − L ◆ B ◆ π ◆ R B ◆◆ L B ◆2◆ R B ◆
Key identities:
sin ( gd x ) = tanh x \sin(\operatorname{gd}\,x) = \tanh x sin ( gd x ) = tanh x
cos ( gd x ) = sech x \cos(\operatorname{gd}\,x) = \operatorname{sech} x cos ( gd x ) = sech x
tan ( gd x ) = sinh x \tan(\operatorname{gd}\,x) = \sinh x tan ( gd x ) = sinh x
17.3 Hyperbolic functions and catenary The catenary curve y = a cosh ( x a ) y = a\cosh\!\left(\dfrac{x}{a}\right) y = a cosh ( a x ) describes a hanging chain.
Arc length from the vertex: s = a sinh ( x a ) s = a\sinh\!\left(\dfrac{x}{a}\right) s = a sinh ( a x ) .
18. Further Exam-Style Questions Question 16 Prove that arsinh x = ln ( x + x 2 + 1 ) \operatorname{arsinh}\,x = \ln(x+\sqrt{x^2+1}) arsinh x = ln ( x + x 2 + 1 ) .
Solution Let y = arsinh x y = \operatorname{arsinh}\,x y = arsinh x , so x = sinh y = e y − e − y 2 x = \sinh y = \dfrac{e^y-e^{-y}}{2} x = sinh y = 2 e y − e − y .
2 x = e y − e − y ⟹ e 2 y − 2 x e y − 1 = 0 2x = e^y - e^{-y} \implies e^{2y} - 2xe^y - 1 = 0 2 x = e y − e − y ⟹ e 2 y − 2 x e y − 1 = 0 .
e y = ◆ L B ◆ 2 x + 4 x 2 + 4 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = x + x 2 + 1 e^y = \dfrac◆LB◆2x + \sqrt{4x^2+4}◆RB◆◆LB◆2◆RB◆ = x + \sqrt{x^2+1} e y = L ◆ B ◆2 x + 4 x 2 + 4 ◆ R B ◆◆ L B ◆2◆ R B ◆ = x + x 2 + 1 (positive root since
e y > 0 e^y > 0 e y > 0 ).
y = ln ( x + x 2 + 1 ) y = \ln(x+\sqrt{x^2+1}) y = ln ( x + x 2 + 1 ) . ■ \blacksquare ■
Question 17 Use the substitution x = 3 sinh t x = 3\sinh t x = 3 sinh t to evaluate
∫ 0 arsinh ( 4 / 3 ) x 2 + 9 d x \displaystyle\int_0^{\operatorname{arsinh}(4/3)} \sqrt{x^2+9}\,dx ∫ 0 arsinh ( 4/3 ) x 2 + 9 d x .
Solution d x = 3 cosh t d t dx = 3\cosh t\,dt d x = 3 cosh t d t , x 2 + 9 = 3 cosh t \sqrt{x^2+9} = 3\cosh t x 2 + 9 = 3 cosh t .
= ∫ 0 arsinh ( 4 / 3 ) 9 cosh 2 t d t = 9 2 ∫ 0 arsinh ( 4 / 3 ) ( 1 + cosh 2 t ) d t = \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 = ∫ 0 arsinh ( 4/3 ) 9 cosh 2 t d t = 2 9 ∫ 0 arsinh ( 4/3 ) ( 1 + cosh 2 t ) d t
= 9 2 [ t + ◆ L B ◆ sinh 2 t ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ] 0 arsinh ( 4 / 3 ) = \frac{9}{2}\!\left[t + \frac◆LB◆\sinh 2t◆RB◆◆LB◆2◆RB◆\right]_0^{\operatorname{arsinh}(4/3)} = 2 9 [ t + L ◆ B ◆ sinh 2 t ◆ R B ◆◆ L B ◆2◆ R B ◆ ] 0 arsinh ( 4/3 ) .
At t = arsinh ( 4 / 3 ) t = \operatorname{arsinh}(4/3) t = arsinh ( 4/3 ) : sinh t = 4 / 3 \sinh t = 4/3 sinh t = 4/3 , cosh t = 5 / 3 \cosh t = 5/3 cosh t = 5/3 ,
sinh 2 t = 2 ⋅ 4 3 ⋅ 5 3 = 40 9 \sinh 2t = 2\cdot\dfrac{4}{3}\cdot\dfrac{5}{3} = \dfrac{40}{9} sinh 2 t = 2 ⋅ 3 4 ⋅ 3 5 = 9 40 .
= 9 2 ( arsinh 4 3 + 20 9 ) = 9 2 arsinh 4 3 + 10 = \frac{9}{2}\!\left(\operatorname{arsinh}\!\frac{4}{3} + \frac{20}{9}\right) = \boxed{\frac{9}{2}\operatorname{arsinh}\!\frac{4}{3} + 10} = 2 9 ( arsinh 3 4 + 9 20 ) = 2 9 arsinh 3 4 + 10 .