- •Functions
- •The Concept of a Function
- •Trigonometric Functions
- •Inverse Trigonometric Functions
- •Logarithmic, Exponential and Hyperbolic Functions
- •Limits and Continuity
- •Introductory Examples
- •Continuity Examples
- •Linear Function Approximations
- •Limits and Sequences
- •Properties of Continuous Functions
- •The Derivative
- •The Chain Rule
- •Higher Order Derivatives
- •Mathematical Applications
- •Antidifferentiation
- •Linear Second Order Homogeneous Differential Equations
- •Linear Non-Homogeneous Second Order Differential Equations
- •Area Approximation
- •Integration by Substitution
- •Integration by Parts
- •Logarithmic, Exponential and Hyperbolic Functions
- •The Riemann Integral
- •Volumes of Revolution
- •Arc Length and Surface Area
- •Techniques of Integration
- •Integration by formulae
- •Integration by Substitution
- •Integration by Parts
- •Trigonometric Integrals
- •Trigonometric Substitutions
- •Integration by Partial Fractions
- •Fractional Power Substitutions
- •Numerical Integration
- •Integrals over Unbounded Intervals
- •Discontinuities at End Points
- •Improper Integrals
- •Sequences
- •Monotone Sequences
- •Infinite Series
- •Series with Positive Terms
- •Alternating Series
- •Power Series
- •Taylor Polynomials and Series
- •Applications
- •Parabola
- •Ellipse
- •Hyperbola
- •Polar Coordinates
- •Graphs in Polar Coordinates
- •Areas in Polar Coordinates
- •Parametric Equations
4.2. ANTIDIFFERENTIATION |
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f(x) = |x − 1| + 2|x + 2|, [−4, 4] |
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f(x) = sin x − cos x, [0, 2π] |
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f(x) = x − cos x, [0, 2π] |
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x2 − 9 |
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f(x) = (x2 − 1)e−x2 , [−2, 2] |
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f(x) = 3 sin 2x + 4 cos 2x, [0, 2π] |
Evaluate each of the following limits by using the L’Hospital’s Rule.
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4.2Antidi erentiation
The process of finding a function g(x) such that g(x) = f(x), for a given f(x), is called antidi erentiation.
Definition 4.2.1 Let f and g be two continuous functions defined on an open interval (a, b). If g0(x) = f(x) for each x in (a, b), then g is called an antiderivative of f on (a, b).
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CHAPTER 4. APPLICATIONS OF DIFFERENTIATION |
Theorem 4.2.1 If g1(x) and g2(x) are any two antiderivatives of f(x) on (a, b), then there exists some constant C such that
g1(x) = g2(x) + C.
Proof. If h(x) = g1(x) − g2(x), then
h0(x) = g10 (x) − g20 (x)
=f(x) − f(x)
=0
for all x in (a, b). By Theorem 4.1.9, Part (iv), there exists some constant c such that for all x in (a, b),
C = h(x) = g1(x) − g2(x) g2(x) = g1(x) + C.
Definition 4.2.2 If g(x) is an antiderivative of f on (a, b), then the set {g(x)+C : C is a constant} is called a one-parameter family of antiderivatives of f. We called this one-parameter family of antiderivatives the indefinite integral of f(x) on (a, b) and write
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f(x)dx = g(x) + C.
R
The expression “ f(x)dx” is read as “the indefinite integral of f(x) with
R
respect to x.” The function “f(x)” is called the integrand, “ ” is called the integral sign and “x” is called the variable of integration. When dealing with indefinite integrals, we often use the terms antidi erentiation and integration interchangeably. By definition, we observe that
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Example 4.2.1 The following statements are true:
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4.2. ANTIDIFFERENTIATION
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3.x1 dx = ln |x| + c
5. Z sin(ax)dx = −a1 cos(ax) + c
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7.cos(ax)dx = a1 sin(ax) + c
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9.tan(ax)dx = a1 ln | sec(ax)| + c
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11.cot(ax)dx = a1 ln | sin(ax)| + c
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13.e−xdx = −e−x + c
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15.sinh xdx = cosh x + c
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17.tanh x dx = ln | cosh x| + c
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18.coth x dx = ln | sinh x| + c
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19.sinh(ax) = a1 cosh(ax) + c
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20.cosh(ax)dx = a1 sinh(ax) + c
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21.tanh(ax)dx = a1 ln | cosh ax| + c
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22. coth (ax)dx = a1 ln | sinh(ax)| + c
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4.sin x dx = − cos x + c
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6.cos x dx = sin x + c
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8.tan x dx = ln | sec x| + c
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10.cot x dx = ln | sin x| + c
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12.exdx = ex + c
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14.eaxdx = a1 eax + c
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16. cosh x dx = sinh x + c
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sec x dx = ln | sec x + tan x| + c |
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tan2 x dx = tan x − x + c |
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ANTIDIFFERENTIATION |
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csc x cot x dx = − csc x + c |
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Each of these indefinite integral formulas can be proved by di erentiating the right sides of the equation. We show some details in selected cases.
Part 3. Recall that
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CHAPTER 4. APPLICATIONS OF DIFFERENTIATION |
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Example 4.2.2 The following statements are true:
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4.2. ANTIDIFFERENTIATION |
163 |
Remark 14 In the following exercises, use the substitution to reduce the integral to a familiar form and then use the integral tables if necessary.
Exercises 4.2 In each of the following, evaluate the indefinite integral by using the given substitution. Use the formula:
ZZ
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xe−x2 dx, u = −x2 |
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sin(7x + 1)dx; u = 7x + 1 |
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sec2(3x + 1)dx, u = 3x + 1 |
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4.3Linear First Order Di erential Equations
Definition 4.3.1 If p(x) and q(x) are defined on some open interval, then an equation of the form
dxdy + p(x)y = q(x)
is called a linear first order di erential equation in the variable y.
Example 4.3.1 (Exponential Growth). A model for exponential growth is the first order di erential equation
dy
dx = ky, k > 0, y(0) = y0.
To solve this equation we divide by y, integrate both sides with respect to x,
dy
replacing dx by dy as follows: dx
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k dx |
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|y| = ekx+c = ecekx
y = ±ecekx.
4.3. LINEAR FIRST ORDER DIFFERENTIAL EQUATIONS |
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Next, we impose the condition y(0) = y0 to get
y(0) = ±ec = y0
y = y0ekx .
The number y0 is the value of y at x = 0. If the variable x is replaced by the time variable t, we get
y(t) = y(0)ekt.
If k > 0, this is an exponential growth model. If k < 0, this is an example of an exponential decay model.
Theorem 4.3.1 (Linear First Order Di erential Equations) If p(x) and q(x) are continuous, then the di erential equation
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has the one-parameter family of solutions
R Z R
y(x) = e− p(x)dx q(x)e p(x)dxdx + c .
R
Proof. We multiply the given di erential equation (1) by e called the integrating factor.
eR p(x)dx dxdy + p(x)eR p(x)dxy = q(x)eR p(x)dx.
p(x)dx, which is
(2)
Since the integrating factor is never zero, the equation (2) has exactly the same solutions as equation (1). Next, we observe that the left side of the equation is the derivative of the product the integrating factor and y:
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eR p(x)dxy = q(x)eR p(x)dx. |
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eR p(x)dxy = |
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q(x)eR p(x)dxdx + c. |
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Next, we multiply both sides of equation (4) by e− R p(x)dx |
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q(x)eR p(x)dxdx + c |
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Equation (5) gives a one-parameter family of solutions to the equation. To pick a particular member of the family, we specify either a point on the curve, or the slope at a point of the curve. That is,
y(0) = y0 or |
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Example 4.3.2 Solve the di erential equation |
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y0 + 4y = 10 , |
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Step 1. We multiply both sides by the integrating factor |
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Step 2. We observe that the left side is the derivative of the integrating factor and y.
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Step 3. Using the definition of the indefinite integral, we antidi erentiate:
Z
e4xy = (10e4x)dx + c.
Step 4. We multiply both sides by e−4x.
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Exercises 4.3 Find y(t) in each of the following: |
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The population P (t) of a certain country is given by the equation: |
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(i)Find the time when the population will double.
(ii)Find the time when the population will be 3 million.
8.Money grows at the rate of r% compounded continuously if
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where A(t) is the amount of money at time t.
(i)Determine the time when the money will double.
(ii)If A = $5000, determine the time for which A(t) = $15,000.
168 CHAPTER 4. APPLICATIONS OF DIFFERENTIATION
9. A radioactive substance satisfies the equation
A0(t) = −0.002A(t), A(0) = A0,
where t is measured in years.
(i)Determine the time when A(t) = 21 A0. This time is called the half-life of the substance.
(ii)If A0 = 20 grams, find the time t for which A(t) equals 5 grams.
10.The number of bacteria in a test culture increases according to the equation
N0(t) = rN(t), n(0) = N0,
where t is measured in hours. Determine the doubling period. If N0 = 100, r = 0.01, find t such that N(t) = 300.
11.Newton’s law of cooling states that the time rate of change of the temperature T (t) of a body is proportional to the di erence between T and the temperature A of the surrounding medium. Suppose that K stands for the constant of proportionality. Then this law may be expressed as
T 0(t) = K(A − T (t)).
Solve for T (t) in terms of time t and T0 = T (0).
12.In a draining cylindrical tank, the level y of the water in the tank drops according to Torricelli’s law
y0(t) = −Ky1/2
for some constant K. Solve for y in terms of t and K.
13. The rate of change P 0(t) of a population P (t) is proportional to the square root of P (t). Solve for P (t).
14.The rate of change v0(t) of the velocity v(t) of a coasting car is proportional to the square of v. Solve for v(t).
In exercises 15–30, solve for y.