Hyperbolic Functions: sinh, cosh, tanh Explained

#Calculus
TL;DR
Hyperbolic Functions are built from the exponential exe^x: 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}, and tanh⁡x=sinh⁡xcosh⁡x\tanh x = \frac{\sinh x}{\cosh x}. They obey the fundamental identity cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1, which parametrizes the hyperbola x2−y2=1x^2 - y^2 = 1 the way sine and cosine parametrize the circle. Their derivatives are clean: ddx[sinh⁡x]=cosh⁡x\frac{d}{dx}[\sinh x] = \cosh x, ddx[cosh⁡x]=sinh⁡x\frac{d}{dx}[\cosh x] = \sinh x, and ddx[tanh⁡x]=sech⁡2x\frac{d}{dx}[\tanh x] = \operatorname{sech}^2 x.
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Bhanzu TeamLast updated on September 22, 202613 min read

What Are Hyperbolic Functions?

Hyperbolic Functions are a family of functions built from the exponential exe^x, defined so that they relate to the hyperbola x2−y2=1x^2 - y^2 = 1 in the same way the ordinary trigonometric functions relate to the circle x2+y2=1x^2 + y^2 = 1. The three core functions are the hyperbolic sine, the hyperbolic cosine, and the hyperbolic tangent, written sinh⁡\sinh, cosh⁡\cosh, and tanh⁡\tanh and pronounced "sinch," "cosh," and "tanch."

Their definitions are exact and short:

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

The three reciprocals complete the set. Each is defined wherever its denominator is non-zero:

csch⁡x=1sinh⁡x,sech⁡x=1cosh⁡x,coth⁡x=cosh⁡xsinh⁡x\operatorname{csch} x = \frac{1}{\sinh x}, \qquad \operatorname{sech} x = \frac{1}{\cosh x}, \qquad \coth x = \frac{\cosh x}{\sinh x}

Because cosh⁡x≥1\cosh x \geq 1 for every real xx, the functions tanh⁡x\tanh x and sech⁡x\operatorname{sech} x are defined for all real numbers, while coth⁡x\coth x and csch⁡x\operatorname{csch} x are undefined only at x=0x = 0, where sinh⁡x=0\sinh x = 0.

How Are Hyperbolic Functions Defined From e To The x?

To evaluate a hyperbolic function, substitute the value into its exponential formula. The two building blocks exe^x and e−xe^{-x} do all the work: adding them and halving gives cosh⁡x\cosh x, subtracting them and halving gives sinh⁡x\sinh x.

Example 1: Evaluate sinh⁡(ln⁡2)\sinh(\ln 2) and cosh⁡(ln⁡2)\cosh(\ln 2).

Use eln⁡2=2e^{\ln 2} = 2 and e−ln⁡2=12e^{-\ln 2} = \tfrac{1}{2}:

sinh⁡(ln⁡2)=2−122=322=34=0.7500\sinh(\ln 2) = \frac{2 - \tfrac{1}{2}}{2} = \frac{\tfrac{3}{2}}{2} = \frac{3}{4} = 0.7500

cosh⁡(ln⁡2)=2+122=522=54=1.2500\cosh(\ln 2) = \frac{2 + \tfrac{1}{2}}{2} = \frac{\tfrac{5}{2}}{2} = \frac{5}{4} = 1.2500

Final answer: sinh⁡(ln⁡2)=0.7500\sinh(\ln 2) = 0.7500 and cosh⁡(ln⁡2)=1.2500\cosh(\ln 2) = 1.2500. As a check, cosh⁡2−sinh⁡2=2516−916=1616=1\cosh^2 - \sinh^2 = \tfrac{25}{16} - \tfrac{9}{16} = \tfrac{16}{16} = 1, exactly the identity proved in the next section.

Two symmetry facts drop straight out of the definitions:

  • sinh⁡(−x)=−sinh⁡x\sinh(-x) = -\sinh x, so sinh⁡\sinh is an odd function, and its graph passes through the origin.

  • cosh⁡(−x)=cosh⁡x\cosh(-x) = \cosh x, so cosh⁡\cosh is an even function, symmetric about the vertical axis, with a lowest point cosh⁡0=1\cosh 0 = 1.

Why Does cosh Squared Minus sinh Squared Equal 1?

The single most important identity is cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1. Every hyperbolic identity descends from it, and it is the reason the word "hyperbolic" appears in the name. Here is the full derivation from the definitions, which the ranking pages state but never show.

Square each definition:

cosh⁡2x=(ex+e−x2)2=e2x+2+e−2x4\cosh^2 x = \left(\frac{e^x + e^{-x}}{2}\right)^2 = \frac{e^{2x} + 2 + e^{-2x}}{4}

sinh⁡2x=(ex−e−x2)2=e2x−2+e−2x4\sinh^2 x = \left(\frac{e^x - e^{-x}}{2}\right)^2 = \frac{e^{2x} - 2 + e^{-2x}}{4}

Subtract the second from the first. The e2xe^{2x} and e−2xe^{-2x} terms cancel, leaving only the constants:

cosh⁡2x−sinh⁡2x=(e2x+2+e−2x)−(e2x−2+e−2x)4=44=1\cosh^2 x - \sinh^2 x = \frac{(e^{2x} + 2 + e^{-2x}) - (e^{2x} - 2 + e^{-2x})}{4} = \frac{4}{4} = 1

The geometric meaning. Set xcoord=cosh⁡tx_{\text{coord}} = \cosh t and ycoord=sinh⁡ty_{\text{coord}} = \sinh t. Then xcoord2−ycoord2=cosh⁡2t−sinh⁡2t=1x_{\text{coord}}^2 - y_{\text{coord}}^2 = \cosh^2 t - \sinh^2 t = 1, so the point (cosh⁡t,sinh⁡t)(\cosh t, \sinh t) always lands on the hyperbola x2−y2=1x^2 - y^2 = 1. As tt runs over all real numbers, the point traces the right branch of that curve, because cosh⁡t≥1\cosh t \geq 1 is never negative.

This is the exact hyperbolic mirror of the circle: (cos⁡t,sin⁡t)(\cos t, \sin t) satisfies cos⁡2t+sin⁡2t=1\cos^2 t + \sin^2 t = 1 and rides the unit circle. The only change is a single sign, plus becoming minus.

How Do You Differentiate Hyperbolic Functions?

Differentiating sinh⁡\sinh and cosh⁡\cosh takes one line each, because ddx[ex]=ex\frac{d}{dx}[e^x] = e^x and ddx[e−x]=−e−x\frac{d}{dx}[e^{-x}] = -e^{-x}:

ddx[sinh⁡x]=ddx[ex−e−x2]=ex+e−x2=cosh⁡x\frac{d}{dx}[\sinh x] = \frac{d}{dx}\left[\frac{e^x - e^{-x}}{2}\right] = \frac{e^x + e^{-x}}{2} = \cosh x

ddx[cosh⁡x]=ddx[ex+e−x2]=ex−e−x2=sinh⁡x\frac{d}{dx}[\cosh x] = \frac{d}{dx}\left[\frac{e^x + e^{-x}}{2}\right] = \frac{e^x - e^{-x}}{2} = \sinh x

Notice what did not happen: no minus sign appeared. This is the sharpest break from circular trig, where ddx[cos⁡x]=−sin⁡x\frac{d}{dx}[\cos x] = -\sin x. For hyperbolic cosine there is no sign flip.

The hyperbolic tangent derivative is worth deriving in full, since the result sech⁡2x\operatorname{sech}^2 x is easy to misremember. Apply the quotient rule to tanh⁡x=sinh⁡xcosh⁡x\tanh x = \frac{\sinh x}{\cosh x} and use the two derivatives above:

ddx[tanh⁡x]=cosh⁡x⋅cosh⁡x−sinh⁡x⋅sinh⁡xcosh⁡2x=cosh⁡2x−sinh⁡2xcosh⁡2x=1cosh⁡2x=sech⁡2x\frac{d}{dx}[\tanh x] = \frac{\cosh x \cdot \cosh x - \sinh x \cdot \sinh x}{\cosh^2 x} = \frac{\cosh^2 x - \sinh^2 x}{\cosh^2 x} = \frac{1}{\cosh^2 x} = \operatorname{sech}^2 x

The numerator collapses to 11 by the fundamental identity, which is why the answer is so clean.

The geometric interpretation. Each derivative is still a slope of a tangent line. At x=0x = 0, for instance, ddx[sinh⁡x]=cosh⁡0=1\frac{d}{dx}[\sinh x] = \cosh 0 = 1, so the graph of sinh⁡x\sinh x crosses the origin at slope 11, matching the slope of y=xy = x there. And because ddx[tanh⁡x]=sech⁡2x\frac{d}{dx}[\tanh x] = \operatorname{sech}^2 x is always positive but shrinks toward 00 for large xx, the tanh⁡\tanh curve rises everywhere yet flattens toward its horizontal asymptotes at y=±1y = \pm 1.

The full first-derivative set, all consistent with the derivative rules of exponentials:

Table: Derivatives of the six hyperbolic functions.

Function

Derivative

sinh⁡x\sinh x

cosh⁡x\cosh x

cosh⁡x\cosh x

sinh⁡x\sinh x

tanh⁡x\tanh x

sech⁡2x\operatorname{sech}^2 x

coth⁡x\coth x

−csch⁡2x-\operatorname{csch}^2 x

sech⁡x\operatorname{sech} x

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

csch⁡x\operatorname{csch} x

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

Reading the table backwards gives the matching integrals: ∫cosh⁡x,dx=sinh⁡x+C\int \cosh x , dx = \sinh x + C and ∫sinh⁡x,dx=cosh⁡x+C\int \sinh x , dx = \cosh x + C, each with its constant of integration.

Example 2: Differentiate y=sinh⁡(3x)y = \sinh(3x) and integrate ∫cosh⁡(2x),dx\int \cosh(2x), dx.

For the derivative, apply the chain rule, the inner function is 3x3x with inner derivative 33:

ddx[sinh⁡(3x)]=cosh⁡(3x)⋅3=3cosh⁡(3x)\frac{d}{dx}[\sinh(3x)] = \cosh(3x) \cdot 3 = 3\cosh(3x)

For the integral, reverse the chain rule and divide by the inner derivative 22:

∫cosh⁡(2x),dx=12sinh⁡(2x)+C\int \cosh(2x), dx = \frac{1}{2}\sinh(2x) + C

Verify by differentiating the antiderivative back: ddx[12sinh⁡(2x)+C]=12⋅2cosh⁡(2x)=cosh⁡(2x)\frac{d}{dx}\left[\tfrac{1}{2}\sinh(2x) + C\right] = \tfrac{1}{2}\cdot 2\cosh(2x) = \cosh(2x), which is the original integrand.

Final answer: ddx[sinh⁡(3x)]=3cosh⁡(3x)\frac{d}{dx}[\sinh(3x)] = 3\cosh(3x) and ∫cosh⁡(2x),dx=12sinh⁡(2x)+C\int \cosh(2x), dx = \frac{1}{2}\sinh(2x) + C.

What Are The Key Hyperbolic Identities?

Because every hyperbolic function is an exponential in disguise, the identities look like the trigonometric ones with a handful of sign changes. The table pairs each hyperbolic identity with its circular cousin so the differences are visible at a glance.

Table: Hyperbolic identities and their circular counterparts.

Hyperbolic identity

Circular counterpart

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

cos⁡2x+sin⁡2x=1\cos^2 x + \sin^2 x = 1

1−tanh⁡2x=sech⁡2x1 - \tanh^2 x = \operatorname{sech}^2 x

1+tan⁡2x=sec⁡2x1 + \tan^2 x = \sec^2 x

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

sin⁡(x+y)=sin⁡xcos⁡y+cos⁡xsin⁡y\sin(x+y) = \sin x \cos y + \cos x \sin y

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

cos⁡(x+y)=cos⁡xcos⁡y−sin⁡xsin⁡y\cos(x+y) = \cos x \cos y - \sin x \sin y

sinh⁡(2x)=2sinh⁡xcosh⁡x\sinh(2x) = 2\sinh x \cosh x

sin⁡(2x)=2sin⁡xcos⁡x\sin(2x) = 2\sin x \cos x

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

cos⁡(2x)=cos⁡2x−sin⁡2x\cos(2x) = \cos^2 x - \sin^2 x

The identity 1−tanh⁡2x=sech⁡2x1 - \tanh^2 x = \operatorname{sech}^2 x follows from the fundamental one by dividing cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1 through by cosh⁡2x\cosh^2 x. The pattern to remember: wherever a product of two sines appears, the hyperbolic version flips the sign relative to the circular version. That single rule reproduces the whole table.

What Are Inverse Hyperbolic Functions?

Each hyperbolic function has an inverse that undoes it, and because the originals are made of exponentials, the inverses are made of logarithms. Solving y=sinh⁡xy = \sinh x for xx leads to a quadratic in exe^x, and the positive root gives a closed form:

sinh⁡−1x=ln⁡(x+x2+1),valid for all real x\sinh^{-1} x = \ln\left(x + \sqrt{x^2 + 1}\right), \quad \text{valid for all real } x

cosh⁡−1x=ln⁡(x+x2−1),x≥1\cosh^{-1} x = \ln\left(x + \sqrt{x^2 - 1}\right), \quad x \geq 1

tanh⁡−1x=12ln⁡(1+x1−x),∣x∣<1\tanh^{-1} x = \frac{1}{2}\ln\left(\frac{1 + x}{1 - x}\right), \quad |x| < 1

The restriction on cosh⁡−1x\cosh^{-1} x (only x≥1x \geq 1) exists because cosh⁡\cosh never outputs a value below 11, and the restriction ∣x∣<1|x| < 1 on tanh⁡−1x\tanh^{-1} x exists because tanh⁡\tanh only ever outputs values strictly between −1-1 and 11. These are ordinary inverse functions, restricted to the ranges the originals actually reach.

Their derivatives are the reason hyperbolic functions matter in integration: for example, ddx[sinh⁡−1x]=1x2+1\frac{d}{dx}[\sinh^{-1} x] = \frac{1}{\sqrt{x^2 + 1}}, so ∫dxx2+1=sinh⁡−1x+C\int \frac{dx}{\sqrt{x^2 + 1}} = \sinh^{-1} x + C, an antiderivative that would otherwise need an awkward substitution.

Why Do Hyperbolic Functions Work?

Hyperbolic functions are not a second, unrelated copy of trigonometry. They are what the same algebra produces when the underlying curve is a hyperbola instead of a circle.

  • They come from splitting exe^x. Any function can be broken into an even part and an odd part. For exe^x, the even part is cosh⁡x\cosh x and the odd part is sinh⁡x\sinh x, and adding them recovers cosh⁡x+sinh⁡x=ex\cosh x + \sinh x = e^x. The functions are simply the two halves of the exponential.

  • They ride the hyperbola. The point (cosh⁡t,sinh⁡t)(\cosh t, \sinh t) satisfies x2−y2=1x^2 - y^2 = 1, so it lives on the conic section called a hyperbola, the same way (cos⁡t,sin⁡t)(\cos t, \sin t) lives on the circle.

  • The parameter is an area, not an angle. For the circle, the parameter tt equals twice the area of the swept sector. For the hyperbola, tt again equals twice the area of the hyperbolic sector. This is the deep reason the two families mirror each other, and why tt is not measured in degrees.

  • The sign change is geometry, not accident. A circle has x2+y2=1x^2 + y^2 = 1 with a plus; a hyperbola has x2−y2=1x^2 - y^2 = 1 with a minus. Every "flipped sign" in the identity table traces back to that one difference in the defining curve.

Seen this way, sine and cosine and sinh⁡\sinh and cosh⁡\cosh are two readings of one idea. The trigonometric functions measure circular motion; the hyperbolic functions measure motion along a hyperbola.

Who Discovered Hyperbolic Functions?

For a long time the hyperbola and the circle were treated as distant relatives. The insight that they carry a matching pair of functions came in the mid-1700s, from two mathematicians working just after Euler had shown how deeply the exponential runs through all of analysis.

Two figures shaped the subject into its modern form:

  • Vincenzo Riccati (1707–1775, Italy) introduced the hyperbolic sine and cosine as geometric quantities and established their basic identity.

  • Johann Heinrich Lambert (1728–1777, Switzerland and Germany) developed the notation and the connection to the exponential, and popularized the functions so widely that they entered the standard toolkit of analysis.

Where Are Hyperbolic Functions Used In The Real World?

The clean derivatives and the exponential core make hyperbolic functions appear wherever growth, hanging, or steady-state behavior is modeled.

  • Engineering and architecture: a chain, rope, or power line hanging under its own weight forms a catenary, y=acosh⁡(x/a)y = a\cosh(x/a). Suspension-bridge cables, overhead transmission lines, and the shape of the Gateway Arch in St. Louis are all designed around this curve.

  • Physics: the velocity of an object falling with air resistance approaches its terminal speed along a tanh⁡\tanh curve, and the shape of a relativistic "rapidity" adds using tanh⁡\tanh rather than ordinary addition.

  • Machine learning: tanh⁡x\tanh x is a classic activation function inside neural networks, chosen because it squashes any input smoothly into the range (−1,1)(-1, 1).

  • Signal processing and heat flow: solutions to many differential equations that describe cooling, cable signals, and vibrations are written with cosh⁡\cosh and sinh⁡\sinh.

  • Special relativity: a boost between reference frames is a "hyperbolic rotation," using cosh⁡\cosh and sinh⁡\sinh exactly where a spatial rotation would use cos⁡\cos and sin⁡\sin.

One curve, the humble hanging chain, connects a child's swing set to a suspension bridge to the mathematics of moving reference frames. The hyperbola is quietly holding all of them up.

What Are The Most Common Mistakes With Hyperbolic Functions?

These four errors account for most lost marks on hyperbolic functions, verified against the mathcentre workbook, the Cuyamaca College M280 handout, and the "derivative of tanh" and "no sign flip" points surfaced in real search queries.

Using the wrong sign in the fundamental identity.

Where it slips in:

A student writes sinh⁡2x+cosh⁡2x=1\sinh^2 x + \cosh^2 x = 1 by copying the circular identity sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1 out of habit.

Don't do this:

Do not carry the plus sign over from circular trig. That equation is false, since cosh⁡x≥1\cosh x \geq 1 already makes cosh⁡2x≥1\cosh^2 x \geq 1 on its own.

The correct way:

Use a minus and put cosh⁡\cosh first: cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1. The minus is the fingerprint of the hyperbola x2−y2=1x^2 - y^2 = 1.

Adding a minus sign to the derivative of cosh.

Where it slips in:

A student writes ddx[cosh⁡x]=−sinh⁡x\frac{d}{dx}[\cosh x] = -\sinh x, reasoning by analogy with ddx[cos⁡x]=−sin⁡x\frac{d}{dx}[\cos x] = -\sin x.

Don't do this:

Do not import the sign flip from circular trig. There is no negative sign in the hyperbolic cosine derivative.

The correct way:

Differentiate from the definition: ddx[cosh⁡x]=ex−e−x2=sinh⁡x\frac{d}{dx}[\cosh x] = \frac{e^x - e^{-x}}{2} = \sinh x, with no minus. Both sinh⁡\sinh and cosh⁡\cosh differentiate to the other with a plus.

Forgetting the chain-rule inner derivative (or the +C+C).

Where it slips in:

A student writes ddx[sinh⁡(3x)]=cosh⁡(3x)\frac{d}{dx}[\sinh(3x)] = \cosh(3x), dropping the factor of 33, or writes ∫sinh⁡x,dx=cosh⁡x\int \sinh x , dx = \cosh x with no constant.

Don't do this:

Do not treat the inside as if it were a bare xx, and do not omit the constant of integration on an indefinite integral.

The correct way:

Multiply by the inner derivative: ddx[sinh⁡(3x)]=3cosh⁡(3x)\frac{d}{dx}[\sinh(3x)] = 3\cosh(3x). And close every indefinite integral with +C+C: ∫sinh⁡x,dx=cosh⁡x+C\int \sinh x , dx = \cosh x + C.

Confusing hyperbolic functions with circular ones.

Where it slips in:

Because the names sinh⁡\sinh and sin⁡\sin look almost identical, a student reads cosh⁡\cosh off a unit circle or expects tanh⁡x\tanh x to be periodic.

Don't do this:

Do not treat sinh⁡\sinh, cosh⁡\cosh, tanh⁡\tanh as periodic wave functions. They do not repeat, and cosh⁡x\cosh x never dips below 11.

The correct way:

Anchor them to the hyperbola, not the circle: cosh⁡\cosh grows without bound, sinh⁡\sinh passes once through the origin, and tanh⁡\tanh levels off toward ±1\pm 1. None of them cycles.

Practice Problems On Hyperbolic Functions

Work each one, then check against the verified answer.

  1. Simplify cosh⁡2(5)−sinh⁡2(5)\cosh^2(5) - \sinh^2(5).
    (Answer: 11, by the fundamental identity.)

  2. Find ddx[cosh⁡(4x)]\frac{d}{dx}[\cosh(4x)].
    (Answer: 4sinh⁡(4x)4\sinh(4x), by the chain rule.)

  3. Evaluate sinh⁡0\sinh 0 and cosh⁡0\cosh 0.
    (Answer: sinh⁡0=1−12=0\sinh 0 = \frac{1-1}{2} = 0 and cosh⁡0=1+12=1\cosh 0 = \frac{1+1}{2} = 1.)

  4. Compute ∫sinh⁡x,dx\int \sinh x , dx.
    (Answer: cosh⁡x+C\cosh x + C; differentiate back to recover sinh⁡x\sinh x.)

  5. Find ddx[tanh⁡(x2)]\frac{d}{dx}[\tanh(x^2)].
    (Answer: 2x,sech⁡2(x2)2x,\operatorname{sech}^2(x^2), chain rule with ddx[tanh⁡u]=sech⁡2u\frac{d}{dx}[\tanh u] = \operatorname{sech}^2 u.)

  6. Evaluate tanh⁡−1(0)\tanh^{-1}(0).
    (Answer: 12ln⁡1+01−0=12ln⁡1=0\frac{1}{2}\ln\frac{1+0}{1-0} = \frac{1}{2}\ln 1 = 0.)

Where Should You Go Next After Hyperbolic Functions?

Hyperbolic functions sit at the crossroads of exponentials, geometry, and calculus, and several natural doors open from here.

  1. The hyperbola. Meet the curve x2−y2=1x^2 - y^2 = 1 that gives these functions their name, and see why its two branches and asymptotes shape the graphs of cosh⁡\cosh and sinh⁡\sinh.

  2. Trigonometric functions. Revisit the circular originals side by side with their hyperbolic twins, so the matching identities and the sign differences click into place.

  3. The derivative. Firm up the differentiation rules that make ddx[sinh⁡x]=cosh⁡x\frac{d}{dx}[\sinh x] = \cosh x and ddx[tanh⁡x]=sech⁡2x\frac{d}{dx}[\tanh x] = \operatorname{sech}^2 x feel automatic.

If your child is building toward calculus, a live Bhanzu trainer teaches hyperbolic functions starting from the "why" (the hyperbola and the split of exe^x) rather than a memorized table, in the Bhanzu math program.

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Frequently Asked Questions

What are hyperbolic functions in simple terms?
Hyperbolic Functions are the functions sinh⁡\sinh, cosh⁡\cosh, and tanh⁡\tanh (plus their reciprocals) built from exe^x. They behave like sine, cosine, and tangent, but they are tied to the hyperbola x2−y2=1x^2 - y^2 = 1 instead of the circle.
What is the difference between hyperbolic and trigonometric functions?
Trigonometric functions parametrize the circle x2+y2=1x^2 + y^2 = 1 and are periodic waves. Hyperbolic Functions parametrize the hyperbola x2−y2=1x^2 - y^2 = 1, do not repeat, and are built directly from the exponential. The identities match with a few sign changes, most importantly cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1 versus cos⁡2x+sin⁡2x=1\cos^2 x + \sin^2 x = 1.
What is the derivative of tanh x?
The derivative of tanh⁡x\tanh x is sech⁡2x\operatorname{sech}^2 x, equivalently 1−tanh⁡2x1 - \tanh^2 x. It follows from the quotient rule applied to sinh⁡xcosh⁡x\frac{\sinh x}{\cosh x}, where the numerator collapses to 11 by the fundamental identity.
Why is a hanging chain a cosh curve?
A flexible chain hanging under gravity balances tension and weight at every point, and solving that balance gives the catenary equation y=acosh⁡(x/a)y = a\cosh(x/a). The cosh⁡\cosh shape is the unique curve where those forces stay in equilibrium along the whole chain.
Do hyperbolic functions have inverses?
Yes. Because they are made of exponentials, their inverses are logarithms, for example sinh⁡−1x=ln⁡(x+x2+1)\sinh^{-1} x = \ln(x + \sqrt{x^2 + 1}). The inverse of cosh⁡\cosh needs x≥1x \geq 1 and the inverse of tanh⁡\tanh needs ∣x∣<1|x| < 1, because those are the only values the originals produce.
Which curricula include hyperbolic functions?
Hyperbolic functions appear in India's NCERT and JEE calculus material, in the AP Calculus BC and university calculus sequence in the United States, and in UK A-Level Further Mathematics. They typically follow the study of exponentials, logarithms, and differentiation.
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