7.4 Hyperbolic Functions

The hyperbolic functions are functions that have many applications to mathematics, physics, and engineering. Among many other applications, they are used to describe the formation of satellite rings around planets, to describe the shape of a rope hanging from two points, and have application to the theory of special relativity. This section defines the hyperbolic functions and describes many of their properties, especially their usefulness to calculus.

††margin: (cos⁡θ,sin⁡θ)A=θ2x2+y2=1−11−11xy (cosh⁡θ,sinh⁡θ)A=θ2x2−y2=1−22−22xy Figure 7.4.1: Using trigonometric functions to define points on a circle and hyperbolic functions to define points on a hyperbola.

These functions are sometimes referred to as the “hyperbolic trigonometric functions” as there are many connections between them and the standard trigonometric functions. Figure 7.4.1 demonstrates one such connection. Just as cosine and sine are used to define points on the circle defined by x2+y2=1, the functions hyperbolic cosine and hyperbolic sine are used to define points on the hyperbola x2−y2=1.

We begin with their definitions.

Definition 7.4.1 Hyperbolic Functions


1. cosh⁡x=ex+e−x2 2. sinh⁡x=ex−e−x2 3. tanh⁡x=sinh⁡xcosh⁡x 4. sech⁡x=1cosh⁡x 5. csch⁡x=1sinh⁡x 6. coth⁡x=cosh⁡xsinh⁡x

The hyperbolic functions are graphed in Figure 7.4.2. In the graphs of cosh⁡x and sinh⁡x, graphs of ex/2 and e−x/2 are included with dashed lines. As x gets “large,” cosh⁡x and sinh⁡x each act like ex/2; when x is a large negative number, cosh⁡x acts like e−x/2 whereas sinh⁡x acts like −e−x/2.

††margin: Pronunciation Note:
“cosh” rhymes with “gosh,”
“sinh” rhymes with “pinch,” and
“tanh” rhymes with “ranch,”

Notice the domains of tanh⁡x and sech⁡x are (−∞,∞), whereas both coth⁡x and csch⁡x have vertical asymptotes at x=0. Also note the ranges of these functions, especially tanh⁡x: as x→∞, both sinh⁡x and cosh⁡x approach ex/2, hence tanh⁡x approaches 1.

f⁢(x)=cosh⁡x−3−2−1123−10−5510xyf⁢(x)=sinh⁡x−3−2−1123−10−5510xyf⁢(x)=tanh⁡xf⁢(x)=coth⁡x−3−2−1123−22xyf⁢(x)=sech⁡xf⁢(x)=csch⁡x−3−2−1123−3−2−1123xy
Figure 7.4.2: Graphs of the hyperbolic functions.

The following example explores some of the properties of these functions that bear remarkable resemblance to the properties of their trigonometric counterparts.

Example 7.4.1 Exploring properties of hyperbolic functions

Use Definition 7.4.1 to rewrite the following expressions.

  1. 1.

    cosh2⁡x−sinh2⁡x

  2. 2.

    tanh2⁡x+sech2⁡x

  3. 3.

    2⁢cosh⁡x⁢sinh⁡x

  4. 4.

    dd⁡x⁢(cosh⁡x)

  5. 5.

    dd⁡x⁢(sinh⁡x)

  6. 6.

    dd⁡x⁢(tanh⁡x)

Solution

  1. 1.

    cosh2⁡x−sinh2⁡x=(ex+e−x2)2−(ex−e−x2)2=e2⁢x+2⁢ex⁢e−x+e−2⁢x4−e2⁢x−2⁢ex⁢e−x+e−2⁢x4=44=1.
    So cosh2⁡x−sinh2⁡x=1.

  2. 2.

    tanh2⁡x+sech2⁡x=sinh2⁡xcosh2⁡x+1cosh2⁡x=sinh2⁡x+1cosh2⁡xNow use identity from #1.=cosh2⁡xcosh2⁡x=1.
    So tanh2⁡x+sech2⁡x=1.

  3. 3.

    2⁢cosh⁡x⁢sinh⁡x=2⁢(ex+e−x2)⁢(ex−e−x2)=2⋅e2⁢x−e−2⁢x4=e2⁢x−e−2⁢x2=sinh⁡(2⁢x).
    Thus 2⁢cosh⁡x⁢sinh⁡x=sinh⁡(2⁢x).

  4. 4.

    dd⁡x⁢(cosh⁡x)=dd⁡x⁢(ex+e−x2)=ex−e−x2=sinh⁡x.
    So dd⁡x⁢(cosh⁡x)=sinh⁡x.

  5. 5.

    dd⁡x⁢(sinh⁡x)=dd⁡x⁢(ex−e−x2)=ex+e−x2=cosh⁡x.
    So dd⁡x⁢(sinh⁡x)=cosh⁡x.

  6. 6.

    dd⁡x⁢(tanh⁡x)=dd⁡x⁢(sinh⁡xcosh⁡x)=cosh⁡x⁢cosh⁡x−sinh⁡x⁢sinh⁡xcosh2⁡x=1cosh2⁡x=sech2⁡x.
    So dd⁡x⁢(tanh⁡x)=sech2⁡x.

The following Key Idea summarizes many of the important identities relating to hyperbolic functions. Each can be verified by referring back to Definition 7.4.1.

Key Idea 7.4.1 Useful Hyperbolic Function Properties

Basic Identities

  1. 1.

    cosh2⁡x−sinh2⁡x=1

  2. 2.

    tanh2⁡x+sech2⁡x=1

  3. 3.

    coth2⁡x−csch2⁡x=1

  4. 4.

    cosh⁡2⁢x=cosh2⁡x+sinh2⁡x

  5. 5.

    sinh⁡2⁢x=2⁢sinh⁡x⁢cosh⁡x

  6. 6.

    cosh2⁡x=cosh⁡2⁢x+12

  7. 7.

    sinh2⁡x=cosh⁡2⁢x−12

Derivatives

  1. 1.

    dd⁡x⁢(cosh⁡x)=sinh⁡x

  2. 2.

    dd⁡x⁢(sinh⁡x)=cosh⁡x

  3. 3.

    dd⁡x⁢(tanh⁡x)=sech2⁡x

  4. 4.

    dd⁡x⁢(sech⁡x)=−sech⁡x⁢tanh⁡x

  5. 5.

    dd⁡x⁢(csch⁡x)=−csch⁡x⁢coth⁡x

  6. 6.

    dd⁡x⁢(coth⁡x)=−csch2⁡x

Integrals

  1. 1.

    ∫cosh⁡x⁢d⁡x=sinh⁡x+C

  2. 2.

    ∫sinh⁡x⁢d⁡x=cosh⁡x+C

  3. 3.

    ∫tanh⁡x⁢d⁡x=ln⁡(cosh⁡x)+C

  4. 4.

    ∫coth⁡x⁢d⁡x=ln⁡|sinh⁡x|+C

We practice using Key Idea 7.4.1.

Example 7.4.2 Derivatives and integrals of hyperbolic functions

Evaluate the following derivatives and integrals.
1. dd⁡x⁢(cosh⁡2⁢x) 2. ∫sech2⁡(7⁢t−3)⁢d⁡t 3. ∫0ln⁡2cosh⁡x⁢d⁡x

Solution

  1. 1.

    Using the Chain Rule directly, we have dd⁡x⁢(cosh⁡2⁢x)=2⁢sinh⁡2⁢x.

    Just to demonstrate that it works, let’s also use the Basic Identity found in Key Idea 7.4.1: cosh⁡2⁢x=cosh2⁡x+sinh2⁡x.

    dd⁡x⁢(cosh⁡2⁢x)=dd⁡x⁢(cosh2⁡x+sinh2⁡x) =2⁢cosh⁡x⁢sinh⁡x+2⁢sinh⁡x⁢cosh⁡x
    =4⁢cosh⁡x⁢sinh⁡x.

    Using another Basic Identity, we can see that 4⁢cosh⁡x⁢sinh⁡x=2⁢sinh⁡2⁢x. We get the same answer either way.

  2. 2.

    We employ substitution, with u=7⁢t−3 and d⁡u=7⁢d⁡t. Applying Key Idea 7.4.1 we have:

    ∫sech2⁡(7⁢t−3)⁢d⁡t=17⁢tanh⁡(7⁢t−3)+C.
  3. 3.
    ∫0ln⁡2cosh⁡x⁢d⁡x=sinh⁡x|0ln⁡2=sinh⁡(ln⁡2)−sinh⁡0=sinh⁡(ln⁡2).

    We can simplify this last expression as sinh⁡x is based on exponentials:

    sinh⁡(ln⁡2)=eln⁡2−e−ln⁡22=2−1/22=34.

Inverse Hyperbolic Functions

Just as the inverse trigonometric functions are useful in certain integrations, the inverse hyperbolic functions are useful with others. Figure 7.4.3 shows the restrictions on the domains to make each function one-to-one and the resulting domains and ranges of their inverse functions. Their graphs are shown in Figure 7.4.4.

Because the hyperbolic functions are defined in terms of exponential functions, their inverses can be expressed in terms of logarithms as shown in Key Idea 7.4.2. It is often more convenient to use sinh−1⁡x than ln⁡(x+x2+1), especially when one is working on theory and does not need to compute actual values. On the other hand, when computations are needed, technology is often helpful but many hand-held calculators lack a convenient sinh−1⁡x button. (Often it can be accessed under a menu system, but not conveniently.) In such a situation, the logarithmic representation is useful. The reader is not encouraged to memorize these, but rather know they exist and know how to use them when needed.

Function Domain Range Function Domain Range
cosh⁡x [0,∞) [1,∞) cosh−1⁡x [1,∞) [0,∞)
sinh⁡x (−∞,∞) (−∞,∞) sinh−1⁡x (−∞,∞) (−∞,∞)
tanh⁡x (−∞,∞) (−1,1) tanh−1⁡x (−1,1) (−∞,∞)
sech⁡x [0,∞) (0,1] sech−1⁡x (0,1] [0,∞)
csch⁡x (−∞,0)∪(0,∞) (−∞,0)∪(0,∞) csch−1⁡x (−∞,0)∪(0,∞) (−∞,0)∪(0,∞)
coth⁡x (−∞,0)∪(0,∞) (−∞,−1)∪(1,∞) coth−1⁡x (−∞,−1)∪(1,∞) (−∞,0)∪(0,∞)
Figure 7.4.3: Domains and ranges of the hyperbolic and inverse hyperbolic functions.
y=cosh−1⁡xy=cosh⁡x510510xy y=sinh⁡xy=sinh−1⁡x−1010−10−5510xy
y=coth−1⁡xy=tanh−1⁡x−22−22xy y=sech−1⁡xy=csch−1⁡x−3−2−1123−3−2−1123xy
Figure 7.4.4: Graphs of the hyperbolic functions and their inverses.

Now let’s consider the inverses of the hyperbolic functions. We begin with the function f⁢(x)=sinh⁡x. Since f′⁢(x)=cosh⁡x>0 for all real x, f is increasing and must be one-to-one.

y =ex−e−x2
2⁢y =ex−e−x(now multiply by ex)
2⁢y⁢ex =e2⁢x−1(a quadratic form )
(ex)2−2⁢y⁢ex−1 =0(use the quadratic formula)
ex =2⁢y±4⁢y2+42
ex =y±y2+1(use the fact that ex>0)
ex =y+y2+1
x =ln⁡(y+y2+1)

Finally, interchange the variable to find that

sinh−1⁡x=ln⁡(x+x2+1).

In a similar manner we find that the inverses of the other hyperbolic functions are given by:

Key Idea 7.4.2 Logarithmic definitions of Inverse Hyperbolic Functions


  1. 1.

    cosh−1⁡x=ln⁡(x+x2−1);
       x≥1

  2. 2.

    tanh−1⁡x=12⁢ln⁡(1+x1−x);
       |x|<1

  3. 3.

    sech−1⁡x=ln⁡(1+1−x2x);
       0<x≤1

  4. 4.

    sinh−1⁡x=ln⁡(x+x2+1)

  5. 5.

    coth−1⁡x=12⁢ln⁡(x+1x−1);
       |x|>1

  6. 6.

    csch−1⁡x=ln⁡(1x+1+x2|x|);
       x≠0

The following Key Ideas give the derivatives and integrals relating to the inverse hyperbolic functions. In Key Idea 7.4.4, both the inverse hyperbolic and logarithmic function representations of the antiderivative are given, based on Key Idea 7.4.2. Again, these latter functions are often more useful than the former.

Key Idea 7.4.3 Derivatives Involving Inverse Hyperbolic Functions


1. dd⁡x⁢(cosh−1⁡x)=1x2−1;
   x>1
2. dd⁡x⁢(sinh−1⁡x)=1x2+1
x≠0
3. dd⁡x⁢(tanh−1⁡x)=11−x2;
   |x|<1
4. dd⁡x⁢(sech−1⁡x)=−1x⁢1−x2;
   0<x<1
5. dd⁡x⁢(csch−1⁡x)=−1|x|⁢1+x2;
   x≠0
6. dd⁡x⁢(coth−1⁡x)=11−x2;
   |x|>1

Key Idea 7.4.4 Integrals Involving Inverse Hyperbolic Functions
1.⁢∫1x2−a2⁢d⁡x =cosh−1⁡(xa)+C; 0<a<x =ln⁡(x+x2−a2)+C
2.⁢∫1x2+a2⁢d⁡x =sinh−1⁡(xa)+C;a>0 =ln⁡(x+x2+a2)+C
3.⁢∫1a2−x2⁢d⁡x ={1a⁢tanh−1⁡(xa)+C|x|<|a|1a⁢coth−1⁡(xa)+C|a|<|x| =12⁢a⁢ln⁡|a+xa−x|+C
4.⁢∫1x⁢a2−x2⁢d⁡x =−1a⁢sech−1⁡|x|a+C; 0<|x|<a =1a⁢ln⁡|xa+a2−x2|+C
5.⁢∫1x⁢x2+a2⁢d⁡x =−1a⁢csch−1⁡|x|a+C;x≠0,a>0 =1a⁢ln⁡|xa+a2+x2|+C

We practice using the derivative and integral formulas in the following example.

Example 7.4.3 Derivatives and integrals involving inverse hyperbolic functions

Evaluate the following.

  1. 1.

    dd⁡x⁢[cosh−1⁡(3⁢x−25)]

  2. 2.

    ∫1x2−1⁢d⁡x

  3. 3.

    ∫19⁢x2+10⁢d⁡x

Solution

  1. 1.

    Applying Key Idea 7.4.3 with the Chain Rule gives:

    dd⁡x⁢[cosh−1⁡(3⁢x−25)]=1(3⁢x−25)2−1⋅35.
  2. 2.

    Multiplying the numerator and denominator by (−1) gives a second integral can be solved with a direct application of item #3 from Key Idea 7.4.4, with a=1. Thus

    ∫1x2−1⁢d⁡x =−∫11−x2⁢d⁡x
    ={−tanh−1⁡(x)+Cx2<1−coth−1⁡(x)+C1<x2
    =−12⁢ln⁡|x+1x−1|+C
    =12⁢ln⁡|x−1x+1|+C. (7.4.1)
  3. 3.

    This requires a substitution, then item #2 of Key Idea 7.4.4 can be applied.

    Let u=3⁢x, hence d⁡u=3⁢d⁡x. We have

    ∫19⁢x2+10⁢d⁡x =13⁢∫1u2+10⁢d⁡u.
    Note a2=10, hence a=10. Now apply the integral rule.
    =13⁢sinh−1⁡(3⁢x10)+C
    =13⁢ln⁡|3⁢x+9⁢x2+10|+C.

This section covers a lot of ground. New functions were introduced, along with some of their fundamental identities, their derivatives and antiderivatives, their inverses, and the derivatives and antiderivatives of these inverses. Four Key Ideas were presented, each including quite a bit of information.

Do not view this section as containing a source of information to be memorized, but rather as a reference for future problem solving. Key Idea 7.4.4 contains perhaps the most useful information. Know the integration forms it helps evaluate and understand how to use the inverse hyperbolic answer and the logarithmic answer.

The next section takes a brief break from demonstrating new integration techniques. It instead demonstrates a technique of evaluating limits that return indeterminate forms. This technique will be useful in Section 8.6, where limits will arise in the evaluation of certain definite integrals.

Exercises

 

Terms and Concepts

  1. 1.

    In Key Idea 7.4.1, the equation ∫tanh⁡x⁢d⁡x=ln⁡(cosh⁡x)+C is given. Why is “ln⁡|cosh⁡x|” not used — i.e., why are absolute values not necessary?

  2. 2.

    The hyperbolic functions are used to define points on the right hand portion of the hyperbola x2−y2=1, as shown in Figure 7.4.1. How can we use the hyperbolic functions to define points on the left hand portion of the hyperbola?

Problems

  1. 3.

    Suppose sinh⁡t=5/12. Find the values of the other five hyperbolic functions at t.

  2. 4.

    Suppose tanh⁡t=−3/5. Find the values of the other five hyperbolic functions at t.

In Exercises 3–12, verify the given identity using Definition 7.4.1, as done in Example 7.4.1.

  1. 5.

    coth2⁡x−csch2⁡x=1

  2. 6.

    cosh⁡2⁢x=cosh2⁡x+sinh2⁡x

  3. 7.

    cosh2⁡x=cosh⁡2⁢x+12

  4. 8.

    sinh2⁡x=cosh⁡2⁢x−12

  5. 9.

    dd⁡x⁢[sech⁡x]=−sech⁡x⁢tanh⁡x

  6. 10.

    dd⁡x⁢[coth⁡x]=−csch2⁡x

  7. 11.

    ∫tanh⁡x⁢d⁡x=ln⁡(cosh⁡x)+C

  8. 12.

    ∫coth⁡x⁢d⁡x=ln⁡|sinh⁡x|+C

In Exercises 13–24, find the derivative of the given function.

  1. 13.

    f⁢(x)=sinh⁡2⁢x

  2. 14.

    f⁢(x)=cosh2⁡x

  3. 15.

    f⁢(x)=tanh⁡(x2)

  4. 16.

    f⁢(x)=ln⁡(sinh⁡x)

  5. 17.

    f⁢(x)=sinh⁡x⁢cosh⁡x

  6. 18.

    f⁢(x)=x⁢sinh⁡x−cosh⁡x

  7. 19.

    f⁢(x)=sech−1⁡(x2)

  8. 20.

    f⁢(x)=sinh−1⁡(3⁢x)

  9. 21.

    f⁢(x)=cosh−1⁡(2⁢x2)

  10. 22.

    f⁢(x)=tanh−1⁡(x+5)

  11. 23.

    f⁢(x)=tanh−1⁡(cos⁡x)

  12. 24.

    f⁢(x)=cosh−1⁡(sec⁡x)

In Exercises 25–30, find the equation of the line tangent to the function at the given x-value.

  1. 25.

    f⁢(x)=sinh⁡x at x=0

  2. 26.

    f⁢(x)=cosh⁡x at x=ln⁡2

  3. 27.

    f⁢(x)=tanh⁡x at x=−ln⁡3

  4. 28.

    f⁢(x)=sech2⁡x at x=ln⁡3

  5. 29.

    f⁢(x)=sinh−1⁡x at x=0

  6. 30.

    f⁢(x)=cosh−1⁡x at x=2

In Exercises 31–38, evaluate the given indefinite integral.

  1. 31.

    ∫tanh⁡(2⁢x)⁢d⁡x

  2. 32.

    ∫cosh⁡(3⁢x−7)⁢d⁡x

  3. 33.

    ∫sinh⁡x⁢cosh⁡x⁢d⁡x

  4. 34.

    ∫19−x2⁢d⁡x

  5. 35.

    ∫2⁢xx4−4⁢d⁡x

  6. 36.

    ∫x1+x3⁢d⁡x

  7. 37.

    ∫exe2⁢x+1⁢d⁡x

  8. 38.

    ∫sech⁡x⁢d⁡x    (Hint: multiply by cosh⁡xcosh⁡x; set u=sinh⁡x.)

In Exercises 39–40, evaluate the given definite integral.

  1. 39.

    ∫−11sinh⁡x⁢d⁡x

  2. 40.

    ∫−ln⁡2ln⁡2cosh⁡x⁢d⁡x

  1. 41.

    In the bottom graph of Figure 7.4.1 (the hyperbola), it is stated that the shaded area is θ/2. Verify this claim by setting up and evaluating an appropriate integral (and note that θ is just a positive number, not an angle).

    Hint: Integrate with respect to y, and consult the table of Integration Rules in the Appendix if necessary.

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