6 Simple Steps To Determine The Laurent Series Of A Function

Laurent series

Understanding the Laurent collection of a operate is essential for unlocking a robust instrument in mathematical evaluation. It offers a method to signify a operate as an infinite sum of advanced exponentials, revealing its habits close to particular factors within the advanced aircraft. In contrast to different collection expansions, the Laurent collection is especially adept at dealing with singularities, permitting for a deeper exploration of capabilities with advanced singularities.

To embark on the journey of figuring out the Laurent collection of a operate, we should first outline an remoted singularity. An remoted singularity happens at some extent within the advanced aircraft the place the operate fails to be analytic, however its habits close to that time will be described by a Laurent collection. By analyzing the operate’s habits across the singularity, we will determine its order and principal half, that are important parts for setting up the Laurent collection.

Moreover, the coefficients of the Laurent collection are decided by a technique of contour integration. By integrating the operate round a rigorously chosen contour that encircles the singularity, we will extract the coefficients of the person phrases within the collection. This method offers a scientific method to signify the operate in a kind that captures its habits close to each common and singular factors, providing a complete understanding of its analytical properties.

Figuring out Remoted Singularities

Earlier than we will decide the Laurent collection of a operate, we have to find its remoted singularities. These are factors the place the operate shouldn’t be outlined or has a detachable discontinuity. To determine remoted singularities, we will study the denominator of the operate.

  • If the denominator has an element of $(z-a)^n$ with $n>0$, then $z=a$ is an remoted singularity.
  • If the denominator has an element of $(z-a)^n$ with $n<0$, then $z=a$ shouldn’t be an remoted singularity.
  • If the denominator has an element of $e^{az}-1$ or $e^{az}+1$ with $aneq 0$, then $z=0$ is an remoted singularity.

Instance

Take into account the operate $f(z)=frac{1}{z^2-1}$. The denominator will be factored as $(z-1)(z+1)$. Each $z=1$ and $z=-1$ are remoted singularities as a result of the denominator has elements of $(z-1)^1$ and $(z+1)^1$.

Poles of Optimistic and Damaging Order

In advanced evaluation, a pole of a operate is some extent within the advanced aircraft the place the operate shouldn’t be outlined on account of an infinite discontinuity. Poles will be of two varieties: constructive order and unfavourable order.

Poles of Optimistic Order

A pole of constructive order happens when the denominator of a rational operate has an element of the shape $(z – a)^n$, the place $n$ is a constructive integer. The order of the pole is $n$. At a pole of order $n$, the operate has the next Laurent collection growth:

“`
f(z) = frac{a_{-n}}{(z – a)^n} + frac{a_{-n+1}}{(z – a)^{n-1}} + cdots + frac{a_{-1}}{z – a} + a_0 + a_1(z – a) + a_2(z – a)^2 + cdots
“`

the place $a_k$ are advanced coefficients.

Instance

Take into account the operate $f(z) = frac{1}{(z – 2)^3}$. This operate has a pole of order 3 at $z = 2$. The Laurent collection growth of $f(z)$ round $z = 2$ is:

“`
f(z) = frac{1}{(z – 2)^3} + frac{1}{(z – 2)^2} + frac{1}{z – 2} + 1 + (z – 2) + (z – 2)^2 + cdots
“`

Poles of Damaging Order

A pole of unfavourable order happens when the denominator of a rational operate has an element of the shape $(z – a)^{-n}$, the place $n$ is a constructive integer. The order of the pole is $-n$. At a pole of order $-n$, the operate has the next Laurent collection growth:

“`
f(z) = a_{-n} + a_{-n+1}(z – a) + a_{-n+2}(z – a)^2 + cdots + a_{-1}(z – a)^{n-1} + frac{a_0}{(z – a)^n} + frac{a_1}{(z – a)^{n+1}} + cdots
“`

the place $a_k$ are advanced coefficients.

Instance

Take into account the operate $f(z) = frac{z}{(z – 1)^2}$. This operate has a pole of order $-2$ at $z = 1$. The Laurent collection growth of $f(z)$ round $z = 1$ is:

“`
f(z) = 1 + (z – 1) + (z – 1)^2 + frac{1}{z – 1} + frac{1}{(z – 1)^2} + frac{1}{(z – 1)^3} + cdots
“`

Laurent Sequence Growth for Poles

A pole is some extent within the advanced aircraft the place the operate has a detachable singularity. Which means the operate will be made steady on the pole by eradicating the singularity. Laurent collection growth for poles can be utilized to search out the residues of the operate on the pole, that are essential in lots of purposes equivalent to discovering the zeros of a operate.

To search out the Laurent collection growth for a pole, we first want to search out the order of the pole. The order of the pole is the biggest integer n such that (z – a)^n f(z) is analytic at z = a. As soon as we all know the order of the pole, we will use the next method to search out the Laurent collection growth for the operate:

$$sum_{n=-infty}^{infty} c_n (z – a)^n$$

The place

$$c_n = frac{1}{2pi i} int_{C} frac{f(z)}{(z – a)^{n+1}} dz$$

and C is a circle centered at z = a with radius r such that C doesn’t enclose every other singularities of f(z).

The next desk reveals the Laurent collection growth for some widespread varieties of poles:

Pole Kind Laurent Sequence Growth
Easy pole $$frac{a_{-1}}{z – a} + sum_{n=0}^{infty} c_n (z – a)^n$$
Double pole $$frac{a_{-2}}{(z – a)^2} + frac{a_{-1}}{z – a} + sum_{n=0}^{infty} c_n (z – a)^n$$
Triple pole $$frac{a_{-3}}{(z – a)^3} + frac{a_{-2}}{(z – a)^2} + frac{a_{-1}}{z – a} + sum_{n=0}^{infty} c_n (z – a)^n$$

Principal A part of the Laurent Sequence

The principal a part of a Laurent collection, often known as the singular half, is the portion that incorporates the unfavourable powers of (z-a). Usually, the principal a part of a Laurent collection for a operate (f(z)) centered at (z=a) takes the shape:

“`
sum_{n=1}^{infty} frac{a_{-n}}{(z-a)^n}
“`

The place (a_{-n}) are the coefficients of the unfavourable powers of (z-a). The principal a part of the Laurent collection represents the contributions from the remoted singularity at (z=a). Relying on the character of the singularity, the principal half could have a finite variety of phrases or an infinite variety of phrases.

Pole of Order (m):

If (f(z)) has a pole of order (m) at (z=a), then the principal a part of its Laurent collection incorporates precisely (m) phrases:

“`
frac{a_{-1}}{z-a} + frac{a_{-2}}{(z-a)^2} + cdots + frac{a_{-m}}{(z-a)^m}
“`

the place (a_{-1}, a_{-2}, cdots, a_{-m}) are non-zero constants.

Important Singularity:

If (f(z)) has an important singularity at (z=a), then the principal a part of its Laurent collection incorporates an infinite variety of unfavourable phrases:

“`
sum_{n=1}^{infty} frac{a_{-n}}{(z-a)^n}
“`

the place at the least one of many coefficients (a_{-n}) is non-zero for all (n).

Detachable Singularity:

If (f(z)) has a detachable singularity at (z=a), then the principal a part of its Laurent collection is solely (0), indicating that there aren’t any unfavourable energy phrases within the collection:

“`
0
“`

Growth of Meromorphic Capabilities

A meromorphic operate is a operate that’s holomorphic aside from a set of remoted singularities.
Laurent collection can be utilized to develop meromorphic capabilities round their singularities.
The Laurent collection of a meromorphic operate (f(z)) round a singularity (z_0) has the next kind:

$$sum_{n=-infty}^infty a_n(z-z_0)^n$$

the place (a_n) are constants.
The principal a part of the Laurent collection is the sum of the phrases with unfavourable powers of ((z-z_0)).
The order of the singularity is the diploma of the pole of the principal half.

For instance, the Laurent collection of the operate (f(z) = frac{1}{z-1}) across the singularity (z=1) is

$$sum_{n=-infty}^infty (-1)^n(z-1)^n = frac{1}{z-1} – 1 + (z-1) – (z-1)^2 + …$$

The principal a part of this collection is (frac{1}{z-1}), and the order of the singularity is 1.

The next desk summarizes the steps for increasing a meromorphic operate round a singularity:

Step Description
1 Discover the residues of the operate on the singularity.
2 Write the principal a part of the Laurent collection as a sum of phrases with unfavourable powers of ((z-z_0)).
3 Discover the Laurent collection of the operate by including the principal half to an everyday operate.

Willpower of Laurent Sequence at Infinity

To find out the Laurent collection of a operate at infinity, we observe these steps:

1. Simplify the Operate right into a Rational Kind

First, we simplify the operate right into a rational kind the place the denominator is linear within the variable. This entails dividing the numerator by the denominator utilizing polynomial lengthy division.

2. Issue the Denominator

Subsequent, we issue the denominator of the rational operate into linear elements.

3. Create a Principal Half for Poles

For every linear issue (z – a) within the denominator, we create a principal a part of the shape ( frac{A}{z – a} ), the place A is a continuing.

4. Discover the Coefficients A

To search out the constants A, we use the strategy of residues. This entails evaluating the integral of the operate ( f(z) over z – a ) across the circle centred at ( z = 0 ) with radius ( R ), after which taking the restrict as ( R to infty ).

5. Discover the Principal Half for Infinity

We create a principal a part of the shape ( sum_{n=0}^infty a_n z^n ), the place the ( a_n ) are constants.

6. Mix Principal Components to Kind Laurent Sequence

Lastly, we mix the principal elements to kind the Laurent collection of the operate:

$$ f(z) = left(sum_{n=1}^infty frac{A_n}{z – a_n}proper) + left(sum_{n=0}^infty a_n z^nright) $$

The place the primary time period represents the principal half for poles, and the second time period represents the principal half for infinity.

Laurent Sequence for Rational Capabilities

A rational operate is a operate that may be expressed because the quotient of two polynomials. In different phrases, it’s a operate of the shape
$$f(z) = frac{p(z)}{q(z)},$$
the place and are polynomials.

The Laurent collection for a rational operate will be decided by utilizing the next steps:

1. Issue the denominator into linear elements.

If the denominator of the rational operate will be factored into linear elements, then the Laurent collection will be written as a sum of partial fractions.

2. Discover the residues of the rational operate.

The residue of a rational operate at a singularity is the coefficient of the ^-1 time period within the Laurent collection growth of the operate.

3. Write the Laurent collection for the rational operate.

The Laurent collection for a rational operate is a sum of the partial fractions and the residues of the operate.

For instance, contemplate the rational operate
$$f(z) = frac{1}{z^2-1}.$$

The denominator of this operate will be factored into the linear elements
$$z^2-1 = (z-1)(z+1).$$

The residues of the operate on the singularities and are 1/2 and -1/2, respectively.

Due to this fact, the Laurent collection for the operate is
$$f(z) = frac{1}{2(z-1)} – frac{1}{2(z+1)}.$$

This collection converges for all aside from and . The operate has a easy pole at and a easy pole at .

Cauchy’s Integral Method and Laurent Sequence

Cauchy’s Integral Method

One magical method that assists in figuring out the Laurent collection for a operate is Cauchy’s Integral Method:

(f(z) = frac{1}{2pi i} intlimits_gamma frac{f(w)}{w-z} dw)

On this method, (f(w)) is the operate we search to decipher, (w) is a posh variable touring alongside a contour (gamma), and (z) is a selected level inside or exterior the contour.

Laurent Sequence for a Operate Inside a Circle

When the advanced operate (f(z)) is analytic inside and on a positively oriented circle centered on the origin with radius (R>0), then it has an related Laurent collection legitimate for (0<|z|

(f(z) = sumlimits_{n=-infty}^infty a_n z^n) = (…+frac{a_{-2}}{z^2} + frac{a_{-1}}{z} + a_0 + a_1 z + a_2 z^2 + …)

Right here, the coefficients (a_n) are given by:

(a_n = frac{1}{2pi i} intlimits_=R frac{f(z)}{z^{n+1}} dz)

Laurent Sequence for a Operate Outdoors a Circle

Within the case the place the operate (f(z)) is analytic exterior and on a positively oriented circle centered on the origin with radius (R>0), its Laurent collection converges for ( |z| > R ):

(f(z) = sumlimits_{n=-infty}^infty a_n z^n) = (…+ a_{-2} z^2 + a_{-1} z + a_0 + frac{a_1}{z} + frac{a_2}{z^2} + …)

The coefficients (a_n) are nonetheless calculated utilizing the identical method as earlier than:

(a_n = frac{1}{2pi i} intlimits_=R frac{f(z)}{z^{n+1}} dz)

Laurent Sequence for a Operate with an Important Singularity

When the operate (f(z)) has an important singularity on the origin, its Laurent collection consists of infinitely many nonzero phrases in each the constructive and unfavourable powers of (z):

(f(z) = sumlimits_{n=-infty}^infty a_n z^n) = (… + a_{-2} z^2 + a_{-1} z + a_0 + a_1 z + a_2 z^2 + …)

The coefficients (a_n) are nonetheless obtained utilizing the identical method:

(a_n = frac{1}{2pi i} intlimits_=R frac{f(z)}{z^{n+1}} dz)

Laurent Sequence Illustration

The Laurent collection of a operate

f(z)

in a site

Omega

specifies the operate as a sum of its Taylor collection and a principal half, which incorporates the unfavourable powers of

z-z_0

. The Laurent collection for a operate that’s analytic in an annular area is given by:

$$f(z)=sum_{n=-infty}^{infty}c_n(z-z_0)^n$$

the place

c_n

are the Laurent coefficients.

Software to Advanced Integration

The Laurent collection illustration permits us to guage advanced integrals utilizing the residue theorem. The residue of a operate at a singularity

z_0

is the coefficient of the

(z-z_0)^{-1}

time period in its Laurent collection. The residue theorem states that the integral of a operate round a closed contour

C

enclosing a singularity

z_0

is the same as

2pi i

occasions the residue of the operate at

z_0

.

Calculating Residues

To calculate the residue of a operate at a pole

z_0

, we will use the next method:

$$operatorname{Res}[f(z), z_0] = lim_{z to z_0} (z – z_0) f(z)$$

Cauchy’s Integral Method

Cauchy’s integral method is a robust instrument for evaluating advanced integrals. It states that if

f(z)

is analytic in a site containing a closed contour

C

and

z_0

is inside

C

, then the integral of

f(z)

round

C

is the same as

2pi i

occasions the worth of

f(z)

at

z_0

.

$$ oint_C f(z) dz = 2pi i f(z_0) $$

Instance

Take into account the integral:

$$ I = oint_C frac{1}{z^2 + 1} dz $$

the place

C

is the unit circle centered on the origin. The operate

f(z) = frac{1}{z^2 + 1}

has two poles at

z = pm i

. The residue of

f(z)

at

z = i

is:

$$ operatorname{Res}[f(z), i] = lim_{z to i} (z – i) frac{1}{z^2 + 1} = frac{1}{2i} $$

Utilizing Cauchy’s integral method, we will consider the integral as:

$$ I = 2pi i operatorname{Res}[f(z), i] = 2pi i cdot frac{1}{2i} = pi $$

Convergence and Error Estimation

The Laurent collection of a operate f(z) converges uniformly in an annulus r1 < |z| < r2 if and provided that f(z) is steady on the boundary of the annulus. If f(z) is steady on the closed annulus [r1, r2], then the Laurent collection converges uniformly to f(z) on the open annulus r1 < |z| < r2.

The error in approximating f(z) by its Laurent collection with n phrases is given by the rest time period:

The rest Time period

Rn(z) = f(z) – Sn(z)

the place Sn(z) is the nth partial sum of the Laurent collection.

The rest time period will be estimated utilizing the next method:

Error Estimation

|Rn(z)| ≤ M/(r- |z|)n+1

the place M = max |f(z)| on the boundary of the annulus.

Situation Convergence
f(z) is steady on the boundary of the annulus r1 < |z| < r2 Laurent collection converges uniformly within the annulus
f(z) is steady on the closed annulus [r1, r2] Laurent collection converges uniformly to f(z) within the open annulus r1 < |z| < r2
|f(z)| ≤ M on the boundary of the annulus r1 < |z| < r2 Error in approximating f(z) by its Laurent collection with n phrases is bounded by M/(r- |z|)n+1

Easy methods to Decide the Laurent Sequence of a Operate

The Laurent collection of a operate $f(z)$ is a illustration of the operate as a sum of powers of (z-a), the place (a) is a singular level of the operate. The collection is legitimate in an annular area across the singular level, and it may be used to guage the operate at factors in that area.

To find out the Laurent collection of a operate, you need to use the next steps:

1. Discover the remoted singular factors of the operate.
2. For every singular level, discover the order of the pole or zero.
3. Write the Laurent collection within the kind
$$f(z) = sum_{n=-infty}^{infty} c_n (z-a)^n$$
the place (c_n) are the coefficients of the collection.

The coefficients (c_n) will be discovered utilizing the next formulation:

$$c_n = frac{1}{2pi i} int_{C} frac{f(z)}{(z-a)^{n+1}} dz$$
the place (C) is a circle across the singular level.

Individuals Additionally Ask About Easy methods to Decide the Laurent Sequence of a Operate

What’s the Laurent collection?

The Laurent collection is a illustration of a operate as a sum of powers of (z-a), the place (a) is a singular level of the operate. The collection is legitimate in an annular area across the singular level, and it may be used to guage the operate at factors in that area.

How do I discover the Laurent collection of a operate?

To search out the Laurent collection of a operate, you need to use the next steps:

  1. Discover the remoted singular factors of the operate.
  2. For every singular level, discover the order of the pole or zero.
  3. Write the Laurent collection within the kind
    $$f(z) = sum_{n=-infty}^{infty} c_n (z-a)^n$$
    the place (c_n) are the coefficients of the collection.

What are the coefficients of the Laurent collection?

The coefficients of the Laurent collection are given by the next formulation:

$$c_n = frac{1}{2pi i} int_{C} frac{f(z)}{(z-a)^{n+1}} dz$$
the place (C) is a circle across the singular level.