6 Simple Steps To Determine The Laurent Series Of A Function

Laurent series

Understanding the Laurent collection of a perform is essential for unlocking a robust software in mathematical evaluation. It supplies a approach to signify a perform as an infinite sum of advanced exponentials, revealing its conduct close to particular factors within the advanced airplane. Not like 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 perform, we should first outline an remoted singularity. An remoted singularity happens at some extent within the advanced airplane the place the perform fails to be analytic, however its conduct close to that time could be described by a Laurent collection. By analyzing the perform’s conduct across the singularity, we will establish its order and principal half, that are important elements for developing the Laurent collection.

Moreover, the coefficients of the Laurent collection are decided by a means of contour integration. By integrating the perform round a rigorously chosen contour that encircles the singularity, we will extract the coefficients of the person phrases within the collection. This method supplies a scientific approach to signify the perform in a kind that captures its conduct 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 perform, we have to find its remoted singularities. These are factors the place the perform isn’t outlined or has a detachable discontinuity. To establish remoted singularities, we will look at the denominator of the perform.

  • 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 $z=a$ isn’t 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

Think about the perform $f(z)=frac{1}{z^2-1}$. The denominator could be factored as $(z-1)(z+1)$. Each $z=1$ and $z=-1$ are remoted singularities as a result of the denominator has components of $(z-1)^1$ and $(z+1)^1$.

Poles of Constructive and Detrimental Order

In advanced evaluation, a pole of a perform is some extent within the advanced airplane the place the perform isn’t outlined attributable to an infinite discontinuity. Poles could be of two sorts: optimistic order and adverse order.

Poles of Constructive Order

A pole of optimistic order happens when the denominator of a rational perform has an element of the shape $(z – a)^n$, the place $n$ is a optimistic integer. The order of the pole is $n$. At a pole of order $n$, the perform 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

Think about the perform $f(z) = frac{1}{(z – 2)^3}$. This perform 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 Detrimental Order

A pole of adverse order happens when the denominator of a rational perform has an element of the shape $(z – a)^{-n}$, the place $n$ is a optimistic integer. The order of the pole is $-n$. At a pole of order $-n$, the perform 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

Think about the perform $f(z) = frac{z}{(z – 1)^2}$. This perform 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 Collection Growth for Poles

A pole is some extent within the advanced airplane the place the perform has a detachable singularity. Which means the perform could 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 perform on the pole, that are essential in lots of purposes resembling discovering the zeros of a perform.

To seek 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 most important 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 formulation to search out the Laurent collection growth for the perform:

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

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 exhibits the Laurent collection growth for some frequent kinds of poles:

Pole Sort Laurent Collection 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 Collection

The principal a part of a Laurent collection, often known as the singular half, is the portion that accommodates the adverse powers of (z-a). Generally, the principal a part of a Laurent collection for a perform (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 adverse 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 might 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 accommodates 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 a vital singularity at (z=a), then the principal a part of its Laurent collection accommodates an infinite variety of adverse phrases:

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

the place no less than 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 just (0), indicating that there are not any adverse energy phrases within the collection:

“`
0
“`

Growth of Meromorphic Features

A meromorphic perform is a perform that’s holomorphic aside from a set of remoted singularities.
Laurent collection can be utilized to increase meromorphic capabilities round their singularities.
The Laurent collection of a meromorphic perform (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 adverse 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 perform (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 perform round a singularity:

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

Dedication of Laurent Collection at Infinity

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

1. Simplify the Perform right into a Rational Type

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

2. Issue the Denominator

Subsequent, we issue the denominator of the rational perform into linear components.

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 seek out the constants A, we use the strategy of residues. This includes evaluating the integral of the perform ( 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 Elements to Type Laurent Collection

Lastly, we mix the principal components to kind the Laurent collection of the perform:

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

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

Laurent Collection for Rational Features

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

The Laurent collection for a rational perform could be decided through the use of the next steps:

1. Issue the denominator into linear components.

If the denominator of the rational perform could be factored into linear components, then the Laurent collection could be written as a sum of partial fractions.

2. Discover the residues of the rational perform.

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

3. Write the Laurent collection for the rational perform.

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

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

The denominator of this perform could be factored into the linear components
$$z^2-1 = (z-1)(z+1).$$

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

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

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

Cauchy’s Integral System and Laurent Collection

Cauchy’s Integral System

One magical formulation that assists in figuring out the Laurent collection for a perform is Cauchy’s Integral System:

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

On this formulation, (f(w)) is the perform we search to decipher, (w) is a fancy variable touring alongside a contour (gamma), and (z) is a particular level inside or exterior the contour.

Laurent Collection for a Perform Inside a Circle

When the advanced perform (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 Collection for a Perform Outdoors a Circle

Within the case the place the perform (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 formulation as earlier than:

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

Laurent Collection for a Perform with an Important Singularity

When the perform (f(z)) has a vital singularity on the origin, its Laurent collection consists of infinitely many nonzero phrases in each the optimistic and adverse 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 formulation:

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

Laurent Collection Illustration

The Laurent collection of a perform

f(z)

in a site

Omega

specifies the perform as a sum of its Taylor collection and a principal half, which accommodates the adverse powers of

z-z_0

. The Laurent collection for a perform 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.

Utility to Advanced Integration

The Laurent collection illustration permits us to judge advanced integrals utilizing the residue theorem. The residue of a perform 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 perform round a closed contour

C

enclosing a singularity

z_0

is the same as

2pi i

instances the residue of the perform at

z_0

.

Calculating Residues

To calculate the residue of a perform at a pole

z_0

, we will use the next formulation:

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

Cauchy’s Integral System

Cauchy’s integral formulation is a robust software 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

instances the worth of

f(z)

at

z_0

.

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

Instance

Think about the integral:

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

the place

C

is the unit circle centered on the origin. The perform

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 formulation, 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 perform 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 could be estimated utilizing the next formulation:

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

Decide the Laurent Collection of a Perform

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

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

1. Discover the remoted singular factors of the perform.
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) could 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.

Folks Additionally Ask About Decide the Laurent Collection of a Perform

What’s the Laurent collection?

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

How do I discover the Laurent collection of a perform?

To seek out the Laurent collection of a perform, you need to use the next steps:

  1. Discover the remoted singular factors of the perform.
  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.