The Exponential Function - Practice Problems with Solution | M 408C, Study notes of Mathematics

Material Type: Notes; Class: DIFFEREN AND INTEGRAL CALCULUS; Subject: Mathematics; University: University of Texas - Austin; Term: Fall 2008;

Typology: Study notes

Pre 2010

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M408C: The Exponential Function
November 13, 2008
We define the natural exponential function as the inverse of the natural logarithm function:
We can do this since lnxis an increasing function, so it is one-to-one, and thus has an inverse. The
two functions undo each other, i.e.
The domain of the exp is the range of ln, i.e. (−∞,). The range of exp is the domain of ln, i.e.
(0,). Since ln(ex) = xln(e) = xand exp is the inverse of ln, we have that ex= exp(x). This is
the notation we will typically use for exp(x). The cancellation laws then become eln x=xfor x > 0
and ln(ex) = xfor all x. The limiting behavior of exis well understood:
We also have the laws of exponents which follow from the laws of logarithms: ex+y=exey,
exy=ex
ey, and (ex)r=exr. Finally, differentiating and integrating the exponential is straightfor-
ward:
For the general exponential function, we build on top of our previous work. (We will discuss the
general logarithm function on Tuesday.) So if a > 0 and ris any number, then ar= (eln a)r=erln a.
Thus we can define ax=exlna. This is the exponential function with base a. The laws of
exponents hold for axas well: ax+y=axay,axy=ax
ay, (ax)y=axy, and (ab)x=axbx. We also
have the derivative and integral formulas:
1.
2.
1
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M408C: The Exponential Function

November 13, 2008

We define the natural exponential function as the inverse of the natural logarithm function:

We can do this since ln x is an increasing function, so it is one-to-one, and thus has an inverse. The two functions undo each other, i.e.

The domain of the exp is the range of ln, i.e. (−∞, ∞). The range of exp is the domain of ln, i.e. (0, ∞). Since ln(ex) = x ln(e) = x and exp is the inverse of ln, we have that ex^ = exp(x). This is the notation we will typically use for exp(x). The cancellation laws then become eln^ x^ = x for x > 0 and ln(ex) = x for all x. The limiting behavior of ex^ is well understood:

We also have the laws of exponents which follow from the laws of logarithms: ex+y^ = exey, ex−y^ = e

x ey^ , and (e

x)r (^) = exr. Finally, differentiating and integrating the exponential is straightfor-

ward:

For the general exponential function, we build on top of our previous work. (We will discuss the general logarithm function on Tuesday.) So if a > 0 and r is any number, then ar^ = (eln^ a)r^ = er^ ln^ a. Thus we can define ax^ = ex^ ln^ a. This is the exponential function with base a. The laws of exponents hold for ax^ as well: ax+y^ = axay, ax−y^ = a

x ay^ , (a

x)y (^) = axy, and (ab)x (^) = axbx. We also

have the derivative and integral formulas:

  1. (7.3*.48) Differentiate the function f (t) = sin^2 (esin

(^2) t ). Solution: We apply the chain rule along multiple times to get

f ′(t) = 2 sin(esin

(^2) t ) ·

[

sin(esin

(^2) t )

]′

= 2 sin(esin

(^2) t ) cos(esin

(^2) t ) ·

[

esin

(^2) t]′

= 2 sin(esin

(^2) t ) cos(esin

(^2) t )esin

(^2) t ·

[

sin^2 t

]′

= 2 sin(esin

(^2) t ) cos(esin

(^2) t )esin

(^2) t · 2 sin t cos t = 4 sin(esin

(^2) t ) cos(esin

(^2) t )esin

(^2) t sin t cos t

  1. (7.3*.82) Evaluate the integral

∫ (^) e 1 /x x^2 dx. Solution: We do a u-substitution by setting u = 1/x = x−^1 , so du = −x−^2 dx = − dxx 2 : ∫ e^1 /x x^2

dx = −

eudu = −eu^ + C = −e^1 /x^ + C.

  1. (7.4*.42) Differentiate the function y = (ln x)cos^ x.

Solution: This is a tricky problem. Although we know how to differentiate a number raised to a function – i.e. ax^ – we don’t know how to differentiate a function raised to a function. Instead, let’s try logarithmic differentiation – it will take the cos x and turn it from an exponent to a factor.

ln y = ln ((ln x)cos^ x) = cos x · ln (ln x).

Implicitly differentiating both sides, we get

y′ y

= − sin x · ln (ln x) + cos x ·

[ln x]′ ln x

= − sin x · ln (ln x) + cos x ·

1 /x ln x

= − sin x · ln (ln x) +

cos x x ln x

Solving for y′^ and substituting in for y, we get

y′^ = (ln x)cos^ x

cos x x ln x

− sin x · ln (ln x)

  1. (7.4*.50) Evaluate the integral

∫ (^2) x 2 x+1 dx. Solution: We use u-substitution with u = 2x^ + 1, so du = 2x^ ln 2 dx: ∫ 2 x 2 x^ + 1

dx =

u

du ln 2

ln 2

du u

ln 2

(ln |u| + C) =

ln 2

(ln | 2 x^ + 1| + C).

Since 2x^ + 1 > 0 for all x, | 2 x^ + 1| = 2x^ + 1. We can also multiply through by (^) ln 2^1 and rename (^) ln 2C as just C (in the end, it’s just a constant):

∫ 2 x 2 x^ + 1

dx =

ln(2x^ + 1) ln 2

+ C.