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Handbook of mathematics for engineers and scienteists part 46 ppsx

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The integral on the right-hand side is easy to take, since the integrand is the sum of power functions.. By removing the brackets, one obtains a sum of integrals like x n e ax dx, which

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are evaluated using the formulas

sin α cos β = 12[sin(α + β) + sin(α – β)], cos α cos β = 12[cos(α + β) + cos(α – β)], sin α sin β = 12[cos(α – β) – cos(α + β)].

4 Integrals of the form



sinm xcosn x dx , where m and n are integers, are evaluated

as follows:

(a) if m is odd, one uses the change of variable cos x = z, with sin x dx = –dz;

(b) if n is odd, one uses the change of variable sin x = z, with cos x dx = dz;

(c) if m and n are both even nonnegative integers, one should use the degree reduction

formulas

sin2x= 12(1– cos2x), cos2x= 12(1+ cos2x), sin x cos x = 12 sin2x

Example 3 Evaluate the integral

 sin5x dx.

This integral corresponds to odd m: m =5 With simple rearrangement and the change of variable

cos x = z, we have



sin5x dx=

 (sin2x)2sin x dx = –

 ( 1 – cos2x)2d cos x = –

 ( 1– z2)2dz

= 23z3–15z5– z + C = 23cos3x–15cos5x – cos x + C.

Remark In general, the integrals

 sinp xcosq x dxare reduced to the integral of a differential binomial

by the substitution y = sin x.

7.1.6 Integration of Polynomials Multiplied by Elementary Functions

 Throughout this section, P n (x) designates a polynomial of degree n.

7.1.6-1 Integration of the product of a polynomial by exponential functions

General formulas:



P n (x)e ax dx = e ax



P n (x)

aP n  (x)

a2 +· · · + (–1 )n P

(n)

n (x)

a n+1



+ C,



P n (x) cosh(ax) dx = sinh(ax)



P n (x)

a + P  (x)

a3 +· · ·



– cosh(ax)



P 

n (x)

a2 + P n  (x)

a4 +· · ·



+ C,



P n (x) sinh(ax) dx = cosh(ax)



P n (x)

a + P  (x)

a3 +· · ·



– sinh(ax)



P 

n (x)

a2 +P n  (x)

a4 +· · ·



+ C.

These formulas are obtained by repeated integration by parts; see formula 4 from

Para-graph 7.1.2-2 with f (x) = P n (x) for g(n+1)(x) = e ax , g(n+1)(x) = cosh(ax), and g(n+1)(x) = sinh(ax), respectively.

In the special case P n (x) = x n, the first formula gives



x n e ax dx = e axn

k=0

(–1)n–k

a n+1 –k

n!

k!x

k + C.

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284 INTEGRALS

7.1.6-2 Integration of the product of a polynomial by a trigonometric function

1 General formulas:



P n (x) cos(ax) dx = sin(ax)



P n (x)

aP  (x)

a3 +· · ·



+ cos(ax)



P 

n (x)

a2 – P n  (x)

a4 +· · ·



+ C,



P n (x) sin(ax) dx = sin(ax)



P 

n (x)

a2 – P n  (x)

a4 +· · ·



– cos(ax)



P n (x)

aP  (x)

a3 +· · ·



+ C.

These formulas are obtained by repeated integration by parts; see formula 4 from

Para-graph 7.1.2-2 with f (x) = P n (x) for g(n+1)(x) = cos(ax) and g(n+1)(x) = sin(ax), respectively.

2 To evaluate integrals of the form



P n (x) cos m (ax) dx,



P n (x) sin m (ax) dx, with m =2,3, , one should first use the trigonometric formulas

cos2k (ax) = 1

22k–1

k–1



i=0

C i

2kcos[2(k – i)ax] + 1

22k C2k k (m =2k),

cos2k+1(ax) = 1

22k

k



i=0

C i

2k+1cos[(2k–2i+1)ax] (m =2k+1),

sin2k (ax) = 1

22k–1

k–1



i=0

(–1)k–i C i

2kcos[2(k – i)ax] + 212k C k

2k (m =2k),

sin2k+1(ax) = 1

22k

k



i=0

(–1)k–i C i

2k+1sin[(2k–2i+1)ax] (m =2k+1),

thus reducing the above integrals to those considered in Item1.

3 Integrals of the form



P n (x) e ax sin(bx) dx,



P n (x) e ax cos(bx) dx

can be evaluated by repeated integration by parts

In particular,



x n e ax sin(bx) = e axn+1

k=1

(–1)k+1n!

(n – k +1)! (a2+ b2)k/2x n–k+1sin(bx + kθ) + C,



x n e ax cos(bx) = e axn+1

k=1

(–1)k+1n!

(n – k +1)! (a2+ b2)k/2x n–k+1cos(bx + kθ) + C, where

sin θ = – √ b

a2+ b2, cos θ =

a

a2+ b2.

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7.1.6-3 Integrals involving power and logarithmic functions.

1◦ The formula of integration by parts with g  (x) = P n (x) is effective in the evaluation of

integrals of the form



P n (x) ln(ax) dx = Q n+1(x) ln(ax) – a



Q n+1(x)

x dx,

where Q n+1(x) =



P n (x) dx is a polynomial of degree n+1 The integral on the right-hand

side is easy to take, since the integrand is the sum of power functions

Example Evaluate the integral



ln x dx.

Setting f (x) = ln x and g  (x) =1, we find f  (x) = 1

x and g(x) = x Substituting these expressions into

the formula of integration by parts, we obtain



ln x dx = x ln x –



dx = x ln x – x + C.

2 The easiest way to evaluate integrals of the more general form

I =

 n i=0

lni (ax)

m

j=0

b ij x β ij



dx,

where the β ij are arbitrary numbers, is to use the substitution z = ln(ax), so that

I =

 n i=0

z im

j=0

b ij

a β ij+ 1e(β ij+1)z



dz

By removing the brackets, one obtains a sum of integrals like



x n e ax dx, which are easy

to evaluate by the last formula in Paragraph 7.1.6-1

7.1.6-4 Integrals involving inverse trigonometric functions

1◦ The formula of integration by parts with g  (x) = P n (x) also allows the evaluation of the

following integrals involving inverse trigonometric functions:



P n (x) arcsin(ax) dx = Q n+1(x) arcsin(ax) – a



Q n+1(x)

1– a2x2 dx,



P n (x) arccos(ax) dx = Q n+1(x) arccos(ax) + a



Q n+1(x)

1– a2x2 dx,



P n (x) arctan(ax) dx = Q n+1(x) arctan(ax) – a



Q n+1(x)

a2x2+1 dx,



P n (x) arccot(ax) dx = Q n+1(x) arccot(ax) + a



Q n+1(x)

a2x2+1 dx,

where Q n+1(x) =



P n (x) dx is a polynomial of degree n+1 The integrals with radicals on

the right-hand side in the first two formulas can be evaluated using the techniques described

in Paragraph 7.1.4-2 The integrals of rational functions on the right-hand side in the last two formulas can be evaluated using the techniques described in Subsection 7.1.3

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286 INTEGRALS

Remark. The above formulas can be generalized to contain any rational functions R  (x) and R(x) instead

of the polynomials P n (x) and Q n+1(x), respectively.

2 The following integrals are taken using a change of variable:



P n (x) arcsin m (ax) dx = 1

a



cos z P n



sin z a



z m dz, substitution z = arcsin(ax);



P n (x) arccos m (ax) dx = –1

a



sin z P n



cos z a



z m dz , substitution z = arccos(ax),

where m = 2,3, The expressions cos z sink z and sin z cos k z (k = 1, , n) in the integrals on the right-hand sides should be expressed as sums of sines and cosines with appropriate arguments Then it remains to evaluate integrals considered in Paragraph 7.1.6-2

7.2 Definite Integral

7.2.1 Basic Definitions Classes of Integrable Functions.

Geometrical Meaning of the Definite Integral

7.2.1-1 Basic definitions

Let y = f (x) be a bounded function defined on a finite closed interval [a, b] Let us partition this interval into n elementary subintervals defined by a set of points{x0, x1, , x n}such

that a = x0 < x1 <· · · < x n = b Each subinterval [x k–1, x k] will be characterized by its

lengthΔx k = x k – x k–1and an arbitrarily chosen point ξ k[x k–1, x k] Let us make up an

integral sum (a Cauchy–Riemann sum, also known as a Riemann sum)

s n=

n



k=1

f (ξ k)Δx k (x k–1 ≤ξ kx k).

If, as n → ∞ and, accordingly, Δx k → 0 for all k, there exists a finite limit of the integral sums s n and it depends on neither the way the interval [a, b] was split up, nor the selection of the points ξ k, then this limit is denoted b

a f (x) dx and is called the definite

integral (also the Riemann integral) of the function y = f (x) over the interval [a, b]:

 b

a f (x) dx = lim n→∞ s n



max 1≤k n Δx k →0 as n → ∞

In this case, the function f (x) is called integrable on the interval [a, b].

7.2.1-2 Classes of integrable functions

1 If a function f (x) is continuous on an interval [a, b], then it is integrable on this

interval

2 If a bounded function f (x) has finitely many jump discontinuities on [a, b], then it is integrable on [a, b].

3 A monotonic bounded function f (x) is always integrable.

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7.2.1-3 Geometric meaning of the definite integral.

If f (x) ≥ 0 on [a, b], then the integral  b

a f (x) dx is equal to the area of the domain

D={axb, 0 ≤yf (x)}(the area of the curvilinear trapezoid shown in Fig 7.1)

D

y=f x( )

y

x

O

Figure 7.1 The integral of a nonnegative function f (x) on an interval [a, b] is equal to the area of the shaded

region.

7.2.2 Properties of Definite Integrals and Useful Formulas

7.2.2-1 Qualitative properties of integrals

1 If a function f (x) is integrable on [a, b], then the functions cf (x), with c = const, and

|f (x)| are also integrable on [a, b].

2 If two functions f (x) and g(x) are integrable on [a, b], then their sum, difference, and product are also integrable on [a, b].

3 If a function f (x) is integrable on [a, b] and its values lie within an interval [c, d], where a function g(y) is defined and continuous, then the composite function g(f (x)) is also integrable on [a, b].

4 If a function f (x) is integrable on [a, b], then it is also integrable and on any subin-terval [α, β] ⊂ [a, b] Conversely, if an interval [a, b] is partitioned into a number of subintervals and f (x) is integrable on each of the subintervals, then it is integrable on the whole interval [a, b].

5 If the values of a function are changed at finitely many points, this will not affect the integrability of the function and will not change the value of the integral

7.2.2-2 Properties of integrals in terms of identities

1 The integral over a zero-length interval is zero:

 a

a f (x) dx =0

2 Antisymmetry under the swap of the integration limits:

 b

a f (x) dx = –

 a

b f (x) dx.

This property can be taken as the definition of a definite integral with a > b.

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288 INTEGRALS

3 Linearity If functions f (x) and g(x) are integrable on an interval [a, b], then

 b

a



Af (x) Bg (x)

dx = A

 b

a f (x) dx B

 b

a g (x) dx for any numbers A and B.

4 Additivity If c[a, b] and f (x) is integrable on [a, b], then

 b

a f (x) dx =

 c

a f (x) dx +

 b

c f (x) dx.

5 Differentiation with respect the variable upper limit If f (x) is continuous on [a, b],

then the function Φ(x) =  x

a f (t) dt is differentiable on [a, b], andΦ (x) = f (x) This can

be written in one relation:

d dx

 x

a f (t) dt



= f (x).

6 Newton–Leibniz formula:

 b

a f (x) dx = F (x)



b

a = F (b) – F (a), where F (x) is an antiderivative of f (x) on [a, b].

7 Integration by parts If functions f (x) and g(x) have continuous derivatives on [a, b],

a f (x)g

 (x) dx =

f (x)g(x)b

a

 b

a f

 (x)g(x) dx.

8 Repeated integration by parts:

 b

a f (x)g

(n+1 )(x) dx =

*

f (x)g(n) (x) – f  (x)g(n–1)(x) + · · · + (–1)n f(n) (x)g(x)+b

a

+ (–1)n+1 b

a f

(n+1 )(x)g(x) dx, n=0,1,

9 Change of variable (substitution) in a definite integral Let f (x) be a continuous function on [a, b] and let x(t) be a continuously differentiable function on [α, β] Suppose also that the range of values of x(t) coincides with [a, b], with x(α) = a and x(β) = b Then

 b

a f (x) dx =

 β

α f x (t)

x  (t) dt.

Example Evaluate the integral

 3 0

dx

(x –8 )

x+ 1.

Perform the substitution x +1= t2, with dx =2t dt We have t =1at x =0and t =2at x =3 Therefore

 3

0

dx

(x –8 )

x+ 1 =

 2 1

2t dt

(t2 – 9)t =2

 2 1

dt

t2– 9 =

1

3lnt– 3

t+ 3 

2 1

= 1

3ln

2

5.

10 Differentiation with respect to a parameter Let f (x, λ) be a continuous function in

a domain axb , λ1≤λλ2and let it has a continuous partial derivative ∂λ ∂ f (x, λ) in the

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same domain Also let u(λ) and v(λ) be differentiable functions on the interval λ1≤λλ2

such that au (λ)b and av (λ)b Then

d

 u(λ)

v(λ) f (x, λ) dx = f u (λ), λ

du(λ)

dλ – f v (λ), λ dv(λ)

+

 u(λ)

v(λ)

∂λ f (x, λ) dx.

11 Cauchy’s formula for multiple integration:

 x

a dx1

 x1

a dx2 .

 x n–1

a f (x n ) dx n=

1

(n –1)!

 x

a (x – t)

n–1f (t) dt.

7.2.3 General Reduction Formulas for the Evaluation of Integrals

Below are some general formulas, involving arbitrary functions and parameters, that could facilitate the evaluation of integrals

7.2.3-1 Integrals involving functions of a linear or rational argument

 b

a f (a + b – x) dx =

 b

a f (x) dx;

 a

0 [f (x) + f (a – x)] dx =2

 a

0 f (x) dx;

 a

0 [f (x) – f (a – x)] dx =0;

 aa f (x) dx =0 if f (x) is odd;

 aa f (x) dx =2

 a

0 f (x) dx if f (x) is even;

 b

a f (x, a + b – x) dx =0 if f (x, y) = –f (y, x);

 1

0 f 2x √

1– x2

dx=

 1

0 f 1– x2) dx.

7.2.3-2 Integrals involving functions with trigonometric argument

 π

0 f (sin x) dx =2

 π/2

0 f (sin x) dx;

 π/2

0 f (sin x) dx =

 π/2

0 f (cos x) dx;

 π/2

0 f (sin x, cos x) dx =0 if f (x, y) = –f (y, x);

 π/2

0 f(sin2x ) cos x dx =

 π/2

0 f(cos

2x ) cos x dx;

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