Math 1120 Class 2 Dan Barbasch Aug. 28, 2012 Dan Barbasch () Math - - PowerPoint PPT Presentation

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Math 1120 Class 2 Dan Barbasch Aug. 28, 2012 Dan Barbasch () Math - - PowerPoint PPT Presentation

Math 1120 Class 2 Dan Barbasch Aug. 28, 2012 Dan Barbasch () Math 1120 Class 2 Aug. 28, 2012 1 / 19 Fundamental Theorem of Calculus The Fundamental Theorem of Calculus (FTC) says the following: Theorem: Let y = f ( x ) be continuous on the


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Math 1120 Class 2

Dan Barbasch

  • Aug. 28, 2012

Dan Barbasch () Math 1120 Class 2

  • Aug. 28, 2012

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Fundamental Theorem of Calculus

The Fundamental Theorem of Calculus (FTC) says the following: Theorem: Let y = f (x) be continuous on the interval [a, b]. Then f (x) has an antiderivative F(x), and b

a

f (x) dx = F(b) − F(a). What does this mean?! The LHS(left hand side) is the definite integral. The RHS(right hand side) involves evaluating the antiderivative F of f .

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Fundamental Theorem of Calculus

The definition of the definite integral (LHS) b

a f (x) dx is very deep. You

approximate y = f (x) by step functions over the interval, and take a limit. The definition is in section 5.3. You may need 5.2 for the notation and

  • ther technicalities.

The definite integral is what arises in applications. You can see them in section 5.1; area, distance travelled, displacement, average of a function. When you compute a definite integral by finding an antiderivative and evaluating, you are invoking FTC (mostly without explicit mention). Question: How many antiderivatives can a function y = f (x) have? The mean value theorem implies that if F ′(x) = G ′(x) over some interval, then there is a constant C such that F(x) = G(x) + C. Question: How does this fit with FTC?

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Fundamental Theorem of Calculus

Example: Compute the area under the graph of y = 1 − x2 and above the x−axis. The notion of the area of a region is by definition a definite integral; the limit of Riemann sums. A = b

a

|f (x)| dx is the area bounded by x = a, x = b y = f (x) and the x−axis.

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Fundamental Theorem of Calculus

Solution to Exercise: The graph of y = 1 − x2 in the region −1 ≤ x ≤ 1 is FTC reduces the problem of computing the area to finding the antiderivative of f (x) = 1 − x2. We know that F(x) = x − x3/3 satisfies F ′(x) = 1 − x2. So by FTC, A = 1

−1

  • 1 − x2

dx =

  • x − x3/3
  • |1

−1=

= (1 − 1/3) − (−1 + 1/3) = 4/3.

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FTC

The Fundamental Theorem of Calculus (FTC) also says the following: Theorem: Assume that y = f (x) is continuous in the interval [a, b]. Then x

a f (t) dt (as a limit of Riemann sums) exists for any a ≤ x ≤ b. The

function F(x) := x

a f (t) dt therefore exists for any a ≤ x ≤ b.

Furthermore F(x) is differentiable in the interval, and F ′(x) = f (x). I say appropriate because the way one proves the theorem is by applying properties of the definite integral proved from the definition in terms of Riemann sums and their limit.

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Differentiating Integrals

Exercises: Compute the following.

  • 1. d

dx x

  • 1 + t2 dt
  • 2. d

dx x2

  • 1 + y2 dy
  • 3. G(x) := d

dx tan x

sin x

csc2 t dt

  • Dan Barbasch ()

Math 1120 Class 2

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Differentiating Integrals

The Key: b

a f (t) dt = F(b) − F(a) where F ′(x) = csc2(x). So

tan x

sin x

csc2 t dt = F(tan x) − F(sin x) The chain rule implies G(x) = F ′(tan x) (tan x)′ − F ′(sin x) (sin x)′ . Exercise: Finish the calculation.

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Answer

(tan x)′ = 1 cos2 x , (sin x)′ = cos x, So G(x) = csc2 (tan x) · 1 cos2 x − csc2 (sin x) · cos x

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A Few Other Notions in 5.4

Area between the graph of a function y = f (x) and the x-axis Signed Area. Exercise: Find the area of the region between the graph of y = (x − 2)2, the x-axis and the lines x = 1 and x = 3. Exercise: Find the area of the region between the graph of ln x

x , the x-axis,

and the lines x = 1/e and x = e.

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Area, Marginal Cost, Distance, Displacement

If f (x) ≥ 0 for a ≤ x ≤ b, then the area of the region is A = b

a f (x) dx.

If f (x) ≥ 0 throughout the interval, then the integral b

a f (x) dx

represents the signed area of the region. The area is A = b

a |f (x)| dx.

Marginal cost is the derivative of total cost C(x) with respect to quantity

  • x. Similar for Marginal Revenue.

Velocity is the derivative of position with respect to time v(t) = s′(t). So position (displacement) is the integral of velocity s(b) − s(a) = b

a v(t) dt.

Total distance traveled is D = b

a |v(t)| dt.

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(Hints to) Answers

The function y = (x − 2)2 is positive in the interval [1, 3], so A = 3

1 (x − 2)2 dx = (x−2)3 3

|3

1= (3−2)3 3

− (1−2)2

3

The function ln x

x

is nonpositive in the interval 1/e ≤ x ≤ 1 and nonnegative in the interval 1 ≤ x ≤ e. Thus A = e

1/e

| ln x x | dx = − 1

1/e

ln x x dx + e

1

ln x x dx. The antiderivative of ln x

x

IS (ln x)2

2

because of the chain rule!

ln x x

= (ln x) (1/x) = (ln x) (ln x)′.

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Examples

  • 1. 5.4, problem 74. Suppose a company’s marginal revenue r(x) from

selling x eggbeaters is r(x) = 2 − 2 (x + 1)2 r(x) in thousands of $, x in thousands of units. How much money does the company earn from 3000 eggbeaters?

  • 2. 5.4, problem 77. Suppose

x

1 f (t) dt = x2 − 2x + 1. Find f (4) and

f (x).

  • 3. 5.4 problem 75b. The temperature T(t) (in
  • F) of a room at time t

minutes is given by T(t) = 85 − 3√25 − t for 0 ≤ t ≤ 25. Find the room’s average temperature for 0 ≤ t ≤ 25.

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Hints to the answers

  • 1. R(x) =

x

0 r(u) du.

  • 2. The function f (x) is the derivative of x2 − 2x + 1.
  • 3. The average of a function y = f (x) over an interval a ≤ x ≤ b is

Avg(f ) :=

1 b−a

b

a f (x) dx.

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Some Integrals

(1) 3 (x − 2)2 dx (2) 3

1

(x − 2)2 dx (3)

  • 1

3

√x dx (4) 2

1

x + √x x2 dx (5) e

1

ln x x dx (6)

  • cos2 x sin x dx

(7)

  • csc x cot x dx

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(Hints to) Answers

In the first three problems we use

  • xn dx = xn+1

n+1 + C for n = −1. In

problem (4) we need to use the algrbraic identity x+√x

x2

= x−1 + x−3/2. For (6), the antiderivative is − cos3 x

3

+ C. Check the answer by differentiating; the chain rule is crucial. For (7), the expression is (sin x)−2 cos x = (sin x)−2(sin x)′.

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Substitution

In (5)-(7) we had to rely on the chain rule to obtain the correct answer. The method of substitution makes this procedure systematic. Substitute u = h(x) in

  • f (x) dx.

The substitution u = h(x) must be 1-1; compute/solve x = h−1(u). Compute dx =

  • h−1′ (u) du.

Substitute

  • f (x) dx =
  • f
  • h−1(u)

h−1′ (u) du. If already x = r(u),

  • f (x) dx =
  • f (r(u))) r′(u) du.

For definite integrals, b

a

f (x) dx = h−1(b)

h−1(a)

f

  • h−1(u)

h−1′ (u) du, b

a

f (x) dx = r(b)

r(a)

f (r(u))) r′(u) du.

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Computing a Definite Integral

b

a

f (x) dx Check that the function is continuous in the interval [a, b], or at least piecewise continuous. NO ASYMPTOTES! Find an antiderivative F(x) of f (x) F ′(x) = f (x). Evaluate F(b) − F(a).

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Examples of Substitutions

Exercise: Compute the area of the circle of radius r > 0.

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We use r = 2, the general case is not that different. A = 2 2

−2

  • 4 − x2 dx.

Make the substitution x = 2 sin θ with −π/2 ≤ θ ≤ π/2. Then dx = 2 cos xdx. If x ranges between −2 ≤ x ≤ 2, then −π/2 ≤ θ ≤ π/2. So we change the endpoints of the integral: A = 2 π/2

−π/2

  • 4 − 4 sin2 θ · 2 cos θ dθ.

Because 4 − 4 sin2 θ = 4(1 − sin2 θ) = 4 cos2 θ, √ 4 − 4x2 = 2| cos θ|; the square root must be nonnegative, but cos θ may be negative. !Again, note that −π/2 ≤ θ ≤ π/2, cos θ ≥ 0!

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The area is A = 8 π/2

−π/2

cos2 θ dθ.

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The area is A = 8 π/2

−π/2

cos2 θ dθ.

Important Formulas for Integration

sin(a ± b) = sin a cos b ± sin b cos a cos(a ± b) = cos a cos b ∓ sin a sin b sin 2x = 2 sin x cos x cos 2x = cos2 x − sin2 x cos 2x = 2 cos2 x − 1 cos 2x = 1 − 2 sin2 x.

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Important Formulas for Integration

sin(a ± b) = sin a cos b ± sin b cos a cos(a ± b) = cos a cos b ∓ sin a sin b sin 2x = 2 sin x cos x cos 2x = cos2 x − sin2 x cos 2x = 2 cos2 x − 1 cos 2x = 1 − 2 sin2 x. This gives sin2 x = 1 − cos 2x 2 cos2 x = 1 + cos 2x 2 These will be available on the formula sheets. No need to memorize, but make sure you practice with them!

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So A = 8 π/2

−π/2

1 + cos 2θ 2 dθ = 4 π/2

−π/2

1 dθ + 4 π/2

−π/2

cos 2θ dθ = 4π. In other words, the second integral is 0. Here’s a simple way to see this, using symmetry. Make the substitution u = 2θ; so du = 2dθ, and the limits of integration change from θ = −π/2, π/2 to u = 2θ = −π, π : π/2

−π/2

cos 2θ dθ = π

−π

cos u du/2 = 1 2 π

−π

cos u du By symmetry, this integral is 0.

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