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3 DERIVATIVES.

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Presentation on theme: "3 DERIVATIVES."— Presentation transcript:

1 3 DERIVATIVES

2 Trigonometric Functions
DERIVATIVES 3.4 Derivatives of Trigonometric Functions In this section, we will learn about: Derivatives of trigonometric functions and their applications.

3 DERIVATIVES OF TRIGONOMETRIC FUNCTIONS
Let’s sketch the graph of the function f(x) = sin x, it looks as if the graph of f’ may be the same as the cosine curve. Figure 3.4.1, p. 149

4 From the definition of a derivative, we have:
DERIVS. OF TRIG. FUNCTIONS Equation 1 From the definition of a derivative, we have:

5 Two of these four limits are easy to evaluate.
DERIVS. OF TRIG. FUNCTIONS Two of these four limits are easy to evaluate.

6 DERIVS. OF TRIG. FUNCTIONS
Since we regard x as a constant when computing a limit as h → 0, we have:

7 The limit of (sin h)/h is not so obvious.
DERIVS. OF TRIG. FUNCTIONS Equation 2 The limit of (sin h)/h is not so obvious. In Example 3 in Section 2.2, we made the guess—on the basis of numerical and graphical evidence—that:

8 DERIVS. OF TRIG. FUNCTIONS
Proof of Eq.2 Assume that θ lies between 0 and π/2, the figure shows a sector of a circle with center O, central angle θ, and radius 1. BC is drawn perpendicular to OA. By the definition of radian measure, we have arc AB = θ. Also, |BC| = |OB| sin θ = sin θ. Figure 3.4.2a, p. 150

9 We see that |BC| < |AB| < arc AB
DERIVS. OF TRIG. FUNCTIONS Proof of Eq.2 We see that |BC| < |AB| < arc AB Thus, Figure 3.4.2a, p. 150

10 Let the tangent lines at A and B intersect at E. Thus,
DERIVS. OF TRIG. FUNCTIONS Proof of Eq.2 Let the tangent lines at A and B intersect at E. Thus, θ = arc AB < |AE| + |EB| < |AE| + |ED| = |AD| = |OA| tan θ = tan θ Figure 3.4.2a, p. 150

11 Therefore, we have: So, We know that
DERIVS. OF TRIG. FUNCTIONS Proof of Eq.2 Therefore, we have: So, We know that So, by the Squeeze Theorem, we have:

12 However, the function (sin θ)/θ is an even function.
DERIVS. OF TRIG. FUNCTIONS Proof of Eq.2 However, the function (sin θ)/θ is an even function. So, its right and left limits must be equal. Hence, we have:

13 DERIVS. OF TRIG. FUNCTIONS
We can deduce the value of the remaining limit in Equation 1 as follows.

14 DERIVS. OF TRIG. FUNCTIONS
Equation 3

15 If we put the limits (2) and (3) in (1), we get:
DERIVS. OF TRIG. FUNCTIONS Formula 4 If we put the limits (2) and (3) in (1), we get: So, we have proved the formula for sine,

16 Differentiate y = x2 sin x.
DERIVS. OF TRIG. FUNCTIONS Example 1 Differentiate y = x2 sin x. Using the Product Rule and Formula 4, we have: Figure 3.4.3, p. 151

17 Using the same methods as in the proof of Formula 4, we can prove:
DERIV. OF COSINE FUNCTION Formula 5 Using the same methods as in the proof of Formula 4, we can prove:

18 DERIV. OF TANGENT FUNCTION
Formula 6

19 DERIVS. OF TRIG. FUNCTIONS
We have collected all the differentiation formulas for trigonometric functions here. Remember, they are valid only when x is measured in radians.

20 For what values of x does the graph of f have a horizontal tangent?
DERIVS. OF TRIG. FUNCTIONS Example 2 Differentiate For what values of x does the graph of f have a horizontal tangent?

21 The Quotient Rule gives:
Solution: Example 2 The Quotient Rule gives: tan2 x + 1 = sec2 x

22 Since sec x is never 0, we see that f’(x)=0 when tan x = 1.
DERIVS. OF TRIG. FUNCTIONS Example 2 Since sec x is never 0, we see that f’(x)=0 when tan x = 1. This occurs when x = nπ + π/4, where n is an integer. Figure 3.4.4, p. 152

23 APPLICATIONS Example 3 An object at the end of a vertical spring is stretched 4 cm beyond its rest position and released at time t = 0. In the figure, note that the downward direction is positive. Its position at time t is s = f(t) = 4 cos t Find the velocity and acceleration at time t and use them to analyze the motion of the object. Figure 3.4.5, p. 152

24 The velocity and acceleration are:
Solution: Example 3 The velocity and acceleration are:

25 The period of the oscillation is 2π, the period of cos t.
Solution: Example 3 The object oscillates from the lowest point (s = 4 cm) to the highest point (s = -4 cm). The period of the oscillation is 2π, the period of cos t. Figure 3.4.5, p. 152

26 Solution: Example 3 The speed is |v| = 4|sin t|, which is greatest when |sin t| = 1, that is, when cos t = 0. So, the object moves fastest as it passes through its equilibrium position (s = 0). Its speed is 0 when sin t = 0, that is, at the high and low points. Figure 3.4.6, p. 153

27 The acceleration a = -4 cos t = 0 when s = 0.
Solution: Example 3 The acceleration a = -4 cos t = 0 when s = 0. It has greatest magnitude at the high and low points. Figure 3.4.6, p. 153

28 Find the 27th derivative of cos x.
DERIVS. OF TRIG. FUNCTIONS Example 4 Find the 27th derivative of cos x. The first few derivatives of f(x) = cos x are as follows:

29 Therefore, f (24)(x) = cos x
Solution: Example 4 We see that the successive derivatives occur in a cycle of length 4 and, in particular, f (n)(x) = cos x whenever n is a multiple of 4. Therefore, f (24)(x) = cos x Differentiating three more times, we have: f (27)(x) = sin x

30 DERIVS. OF TRIG. FUNCTIONS
Example 5 Find In order to apply Equation 2, we first rewrite the function by multiplying and dividing by 7:

31 If we let θ = 7x, then θ → 0 as x → 0. So, by Equation 2, we have:
Solution: Example 5 If we let θ = 7x, then θ → 0 as x → 0. So, by Equation 2, we have:

32 Calculate . Example 6 DERIVS. OF TRIG. FUNCTIONS
We divide the numerator and denominator by x: by the continuity of cosine and Eqn. 2


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