Definite integrals. We shall study line integrals of f (z). In order to do this we shall need some preliminary definitions.

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5. OMPLEX INTEGRATION (A) Definite integrals Integrals are extremely important in the study of functions of a complex variable. The theory is elegant, and the proofs generally simple. The theory is put to much good use in applied mathematics. We shall study line integrals of f (z). In order to do this we shall need some preliminary definitions. Let F(t) = U(t) + iv(t) (a t b) where U,V are real-valued, piecewisecontinuous functions of t on [a, b], i.e. continuous except for at most a finite number of jumps. The definite integral of F on the interval a t b is now defined by: Definition a b F(t) dt = a b U(t) dt + i a b V(t) dt.

Properties of the definite integral 1. Re ( b F(t) dt) = a b U(t) dt = a b Re (F(t)) dt. a [Real part property] 2. b kf = k a b F ; (k, const). a [Scalar multiple property] 3. b (F + G) = a b F + a b G. a [Addition property] 4. b a F = a b F. [Interchange endpoints property] 5. b a F b a F (a b) [Modulus property] Property (1) follows immediately from the definition. The proofs of (2), (3), (4) are trivial, and follow from the properties of real integrals. We see from (2) and (3) that the integral behaves in a linear way.

Proof of Property (5) 5. a b F a b F (a b) [Modulus property] Proof By definition, a b F dt is a complex number. So we can set r 0 cis θ 0 = a b F dt. By Property (2), r 0 = a b F cis ( θ 0 ) dt. Each side is real, and when a complex number is real, it is the same as its real part. So by Property (1), r 0 = a b Re ( F cis ( θ 0 )) dt. But Re ( F cis ( θ 0 )) F cis ( θ 0 ) = F. cis ( θ 0 ) = F. So r 0 a b F dt, providing a b. Hence a b F dt a b F dt.

Arcs Definition A continuous arc is a set of points (x, y): x = φ(t), y = ψ(t ) (a t b), where φ, ψ are real continuous functions of the real parameter t. Notes 1. The definition gives a continuous mapping of [a, b ] to the arc with a corresponding ordering of points. 2. If no two distinct values of t map to the same point (x, y), the arc is a simple arc or a Jordan arc. 3. If Note (2) holds except that φ (a) = φ (b) and ψ (a) = ψ (b), the arc is a simple closed curve or Jordan curve. Examples In the adjacent figure we have: (a) Jordan arc (b) Non-simple curve (c) Jordan curve (d) Non-simple closed curve. (a) (b) (c) (d)

ontours If functions φ, ψ have continuous derivatives φ '(t),ψ'(t) not simultaneously zero, we say the arc (x, y) : x = φ(t), y = ψ(t) (a t b) is smooth (has a continuously turning tangent). Definition to end. A contour is a continuous chain of a finite number of smooth arcs joined end Examples S O ontour Simple closed contour

Length of an arc Definition For a smooth arc, the length exists and is given by L = a b [ φ ( t )] 2 + [ ψ ( t )] 2 dt, providing a b. Now, where does this strange formula come from? From Pythagoras Theorem, the length s of a small portion of the arc is given by s = [ x] 2 + [ y] 2. Dividing through by t gives s = x 2 + y t t t 2. Integrating this expression with respect to t gives the required result. s x y Note It can be shown that this formula is independent of the choice of parameter used.

QUIZ 5.1A 1. The function φ (F) = a b F is a linear function. (a) True ; (b) False. 2. If a b, then a b F a b F. (a) True ; (b) False. 3. A smooth continuous arc is a contour. (a) True ; (b) False. 1. True: follows from the Properties. 2. False: the second inequality should be reversed. 3. True: this is a special type of contour. 4. False: a contour need not be smooth. x 4. If is a contour, then must be a smooth continuous arc. (a) True ; (b) False.

QUIZ 5.1B We show a b F a b F (a b). By definition, a b F dt is a complex number. So we can set { 1. } = a b F dt. By Property (2), r 0 = { 2. }. Each side is real, and when a complex number is real, it is the same as its real part. So by Property (1), r 0 = { 3. }. But Re ( F cis ( θ 0 )) { 4. } = F. cis ( θ 0 ) = F. So r 0 a b F dt, providing a b. Hence a b F dt a b F dt. Match the above boxes 1, 2, 3, 4 with the selections (a) b F cis ( θ a 0 ) dt, (b) F cis ( θ 0 ), (c) r 0 cis θ 0, (d) b Re ( F cis ( θ a 0 )) dt. 1. (c) 2. (a) 3. (d) 4. (b) x My solutions: 1. 2. 3. 4.

Line Integrals Let be a contour extending from z = α to z = β, and set z = x + iy. Thus for z on, x = φ(t), y = ψ(t) (a t b) say, where φ, ψ are continuous and φ,ψ are sectionally continuous. Also t = a when z = α, and t = b when z = β. Let f (t) = u(t) + iv(t) be a (sectionally) continuous function on (that is, the real functions u = u(t) and v = v(t) are sectionally continuous over a t b.) Definition We define f(z) dz = b a f [φ (t) + i ψ (t)].[φ (t) + i ψ (t)] dt. Here, f(z) dz is a line integral, or contour integral. Note that the line integral exists because the integrand on right is sectionally continuous.

Expanding the Line Integral Suppose f(z) = u + iv = u(φ (t), ψ (t)) + iv(φ (t),ψ (t)). Then substituting f(z) = u + iv in the defining expression gives or simply f(z) dz = a b f [φ (t) + i ψ (t)].[φ (t) + i ψ (t)]dt, f(z) dz = a b (uφ vψ )dt + i a b (uψ + vφ )dt, f(z) dz = (u dx v dy) + i (u dy + v dx). (*) Note In summary, f(z) dz = (u + iv)(dx + i dy). Thus by (*) we have expressed the complex line integral in terms of two real line integrals.

Properties of the Line Integral α β 1. f ( z ) dz = f ( z ) dz (taken over the same contour). β α β β 2. kf( z ) dz = k f ( z ) dz (k, constant). α α β β β 3. [f(z) + g(z)] dz = α f ( z ) dz + α g ( z ) dz. α 4. If 1 is a contour (with parameter t from) α to β, 2 a contour from β to γ, and = 1 2 a contour from α to γ, then f ( z ) = 1 f ( z ) + 2 f ( z ). 5. If has length L and f (z) M on, then f ( z ) dz ML. Properties (2) and (3) express the linearity of the integral. Properties (1) to (4) follow easily from known properties of the real integral.

Proof of Property 5 Proof We use Property 5 of the Definite Integral: Now, a b F a b F (a b) (*) f (z) dz = a b f [φ (t) + i ψ (t)].[φ (t) + i ψ (t)]dt (a b) a b f [φ (t) + i ψ (t)].[φ (t) + i ψ (t)] dt (by inequality (*)) M a b φ (t) + i ψ (t) dt ( since f (z) M ) = M (φ (t)) 2 + (ψ (t)) 2 dt ab V = ML.

Line Integral Example I Find I 1 = 1 z 2 dz, where 1 is the illustrated path OB. Line OB has equation x = 2y. Taking y as parameter we obtain the set of points (2y, y) (0 y 1). Now, z 2 is continuous and on 1, z 2 = (x 2 y 2 ) + 2ixy = 3y 2 + 4y 2 i, dz = dx + i dy = (2 + i) dy [strictly (φ (y) + i ψ (y))dy]. Hence y O B(2, 1) 1 x I 1 = 0 1 (3y 2 + 4y 2 i)(2 + i)dy = (3 + 4i)(2 + i) 0 1 y 2 dy = 1 3. (2 + 11i).

Line Integral Example II Find I 2 = 2 z 2 dz, where 2 is the illustrated path OAB. Now I 2 = OA z 2 dz + AB z 2 dz = 0 2 x 2 dx + 0 1 [(4 y 2 ) + 4iy] i dy y B(2, 1) = 8 3 + [4 1 3 + 2i] O 2 A x = 1 3 (2 + 11i). Points on AB are (2, 2 + iy), with 0 y 1.

Some interesting questions Question 1 We see that in the previous examples, the integral from O to B is the same for both contours. Is this a coincidence? Or does it always happen? If it doesn't always happen, when does it? We can express this in a different way. We see that OABO = OAB + BO = I 2 I 1 = 0. So we ask: Is the integral around a closed contour always zero? Question 2 We observe that if we forget the contour altogether, and simply integrate, then we obtain: z 3 3 0 2+i = 1 3 (2 + i) 3 = 1 3 (2 + 11i ) again! Does this always happen? This would say that f is independent of the contour.

Line Integral Example III Find I 3 = 3 z dz, where 3 is the illustrated red path. Now 3 is the contour of points { (x, y ) x = cos θ, y = sin θ, π θ 0 } y and dz = ( sin θ + i cos θ ) dθ. 3 Hence we have I 3 = 3 z dz = π 0 (cos θ i sinθ )( sin θ + i cos θ ) dθ = π 0 idθ = π i. O x

Line Integral Example IV Find I 4 = 4 z dz, where 4 is the illustrated red path. In this case we obtain I 4 = z dz 4 = 2π idθ π = + π i. We observe that this is different from I 3! y O 4 x And if we set = ( 3 ) 4, then z dz = 2 π i. (not 0) where the contour is traversed in an anti-clockwise direction. Note On the contour, z 2 = zz = 1. That is, z = 1 / z. This suggests that there might be some special significance about the singular point z = 0 being inside the contour.

Line Integral Example V Without evaluating the integral, find an upper bound for dz / z 4 on the given contour. We make use of Property 5: In this case, the length L = 2. f ( z ) dz ML. y i Also, the contour has equation y = 1 x (0 x 1). Therefore for z on z 4 = (x 2 + y 2 ) 2 = [x 2 + (1 x) 2 ] 2 = [2x 2 2x + 1] 2. O 1 x That is, z 4 = [2(x 1 2 ) 2 + 1 2 ] 2 1 4. (In retrospect, this is obvious from the figure! Why?) Hence 1 / z 4 4 and I 4 2.

QUIZ 5.2 1. If is the line segment from O to 1 + i, then 2z dz =. 2. If is the line segment from O to 1, followed by the line segment from 1 to 1 + i, then 2z dz =. 3. If is the upper half, from π to 0, of the circle z = 2, then z dz =. 4. If is the circle centre O, radius k and fully traversed, then 1 / z dz 2π. (a) True (b) False. 1. 2i. Set z = x + iy and parameterize segment etc. 2. 2i. As for Q1 but see auchy s Theorem, next section. 3. The answer is 2 πi. 4. True, since 1 / z dz 1/k. 2π k. x

Green s Theorem Let R be a closed region in the real plane made up of a closed contour and all interior points. If P(x, y), Q(x, y) are real continuous functions over R and have continuous first order partial derivatives, then Green s Theorem says: (P dx + Q dy) = R (Q x P y ) dxdy where is described in the anti-clockwise direction. Outline Proof u ( x ) R P y dxdy = ab [ P l ( x ) y dy] dx = ab [ P(x, u(x)) P(x, l(x)) ] dx = Pdx etc. y O y = u(x) R y = l(x) a b x

auchy s Theorem Now consider a function f (z) = u (x, y) + iv(x, y) which is analytic at all points within and on the closed contour, and is such that f ( z ) is continuous there. We show that f (z) dz = 0. The given conditions tell us that u, v continuous. Now and their first order partial derivatives are f ( z ) dz = (u dx v dy) + i (u dy + v dx) = R (v x + u y ) dx dy + i R (u x v y ) dxdy = 0, using Green s Theorem and the auchy-riemann equations. This result was discovered by auchy.

Examples and the auchy- Goursat Theorem As a consequence of auchy s Theorem we have the following: Examples dz = 0, z dz = 0, z 2 dz = 0, for all closed contours, since these functions are analytic everywhere and their derivatives are everywhere continuous. Goursat showed that auchy s condition f (z) is continuous can be omitted. This discovery is important, because from it we can deduce that all derivatives of analytic functions are also analytic. But, proving this stronger result takes much more effort! Theorem 5.1 (auchy-goursat Theorem) If a function f is analytic at all points interior to and on a closed contour, then f (z) dz = 0.

auchy - Goursat Theorem, Example I Find z 2 dz where the contour is the unit circle z = 1. z 3 Now the integrand z2 / (z 3) is analytic everywhere except at the point z = 3. This point lies outside the circular disk z 1. Hence by the auchy-goursat Theorem z 2 dz = 0. z 3 Most of the useful applications of the auchy-goursat Theorem are as yet beyond us, but the next example gives us a glimpse of what can be done.

auchy-goursat Theorem, Example II Assuming Laplace s Integral: show that e t 2 dt = π 0 e x 2 cos 2bx dx = π 2 e b2. [We note that Laplace's integral can be evaluated by writing e x2 dx e y2 dy = e x2 y 2 dx dy and expressing this second integral in polar coordinates.] We integrate f ( z ) = exp( z 2 ) around the rectangle defined by x R, 0 y b. Later we let R. Since exp ( z 2 ) is entire, the auchy-goursat Theorem applies, that is, e z2 dz = 0. [ontinued]

Hence Example II, continued R R e x 2 dx + 0 b e R 2 +y 2 2 iryi dy R R e x 2 +b 2 2 xbi dx 0 b e R 2 +y 2 + 2 iryi dy = 0. Taking out the factor e R2 from the second and fourth integrals and letting R, we get a zero contribution (using the dy ML formula). Hence letting R, e x 2 +b 2 2 xbi dx = e t 2 dt = π (given). Equating the real parts, or e b 2 e x 2 cos 2bx dx = π y b 0 e x 2 cos 2bx dx = π 2 e b2 since the integrand is even. R O R x

Indefinite Integrals Let f be analytic in D and z 0, z D. Then for contours 1, 2 lying in D, joining points z 0, z, and being traversed from z 0 to z, 1 f 2 f = 0, by the auchy-goursat Theorem. Theorem 5.2 ( Primitive Theorem) For all such paths in the domain D has the same value, and F (z) = f (z). F ( z ) = z 0 z f ( z ) dz Note This will allow us to evaluate some line integrals by straight integration. We shall see that the name of the theorem comes from the fact that the function F satisfying F (z) = f (z) is called a primitive of f.

Proof Let z + z be a point in D. Then Proof of the Primitive Theorem F (z + z) F ( z ) = z 0 z+ z f(z )dz z 0 z f(z )dz = z z+ z f(z )dz, where since z is very small, we may take the path from z to z + z to be a line segment. Now clearly on the segment, z z+ z dz = z. So Then f ( z ) = f ( z ) z z z+ z dz = 1 z z z+ z f ( z ) dz. F (z + z) z F ( z ) f ( z ) = 1 z z z+ z [ f(z ) f( z )] dz. [ontinued]

Proof of the Primitive Theorem (ontinued) Now f is continuous at z. Hence for all ε > 0, there exists δ > 0 : z < δ f (z ) f (z) < ε. Hence, when z < δ, F (z + z) z F ( z ) f ( z ) 1 z z z+ z [ f(z ) f( z )] dz 1 z. ε. z = ε, (using Property 5). That is, lim F (z + z) F ( z ) z z 0 z = f ( z ) and F ( z ) exists at each point of D, and F ( z ) = f ( z ).

Notes on the Primitive Theorem We say that F is an indefinite integral or primitive (anti-derivative) of f and write F ( z ) = f ( z ) dz. That is, F is an analytic function whose derivative is f ( z ). Since α β f ( z ) dz = z 0 β f ( z ) dz z 0 α f ( z ) dz = F( β ) F( α ), we can use this as a means of evaluating line integrals. (All paths here are assumed to be in the domain D.)

QUIZ 5.3 1. If f(z) = z / (z 2 4), and is the circle z i =1 traversed positively, then f ( z ) dz = 2. If in Q1 f ( z ) = Log(z +1), then f ( z ) dz = 3. If in Q1 f ( z ) = 1 / (z i), then f ( z ) dz = 4. If and f are as in Q1, then the integrals from O to 2i along either semicircle of are equal. (a) True ; (b) False. 1. 0, since z = ± 2 lie outside. 2. 0, since the cut lies outside. 3. 2πi. Substitute the arc coordinates and evaluate. 4. True, since f is analytic inside. x