of the features:
require(dprep)
data(diabetes)
outbox(diabetes,nclass=1)
box plots online
require(dprep)
data(diabetes)
outbox(diabetes,nclass=1)
The man looks at me and doesn't really understand what the crap I'm talking about. So I get up and head to the board and explain myself while doing the freaking problem. Most of these punks are still lost and so it takes another 20 mins before everyone understands what the hell I'm talking about.
Response: Wow...u learnt that from Africa? or did u read it on the internet. My response...Mary and her grandmother didn't do very well in teaching you math.
that's my piece.
Helpful resources, examples and links
BBC Bitesize is always good GCSE Maths tutor - technical but some worksheets and videos | |
Some people fing watching a YouTube video can help, but be aware that they use real Maths teachers | |
MyMaths Surds1 goes through the topics in a gentle way. | |
Surds2 - a little harder |
i\hbar\frac{\partial\psi}{\partial t} = -\frac{\hbar^2}{2m}\nabla^2\psi + V(\mathbf{r})\psi
E^2 = p^2c^2 + m_0^2c^4
\begin{align*}
\hat{E}=-i\hbar\frac{\partial}{\partial t} \\
\hat{p}=-i\hbar\nabla
\end{align*}
\psi(\mathbf{x},t)=A\exp(i\mathbf{k}\cdot\mathbf{x}-i\omega t)
, these operators give the expected relationships for energy and momentum as their eigenvalues:
\begin{align*}
\hat{E}\psi = -i\hbar i\omega\psi = \hbar\omega\psi \\
\hat{p}\psi = -i\hbar i\mathbf{k} = \hbar\mathbf{k}
\end{align*}
(\hbar=c=1)
and writing the rest mass m_0=m
.
\begin{align*}
\hat{E}^2\psi = \hat{p}^2\psi+m^2\psi\\
\Rightarrow -\frac{\partial^2}{\partial t^2}\psi = -\nabla^2\psi + m^2\psi \\
\Rightarrow \left(-\frac{\partial^2}{\partial t^2} + \nabla^2 -m^2\right)\ps! i = 0 \\
\Rightarrow \left(\partial_\mu\partial^\mu + m^2! \right)\ psi = 0 \\
\Rightarrow \left( \Box +m^2\right)\psi(\mathbf{x},t) = 0
\end{align*}
\Box = \partial_\mu\partial^\mu = \frac{\partial^2}{\partial t^2}-\nabla^2
.
\begin{align*}
\psi(\mathbf{x},t)=N\exp(-iEt+i\mathbf{p}\cdot\mathbf{x}) \\
= N\exp(-ip\cdot x) \\
\mathrm{where~}p\cdot x = p_\mu x^\mu = Et - \mathbf{p}\cdot\mathbf{x}
\end{align*}
E^2=p^2+m^2
, the energy solutions are:
E = \pm\sqrt{\mathbf{p}^2+m^2}
\rho = |\psi|^2 = \psi\psi^\dagger
. If we take the Klein-Gordon equation as:
\frac{\partial^2\psi}{\partial t^2}-\nabla^2\psi + m^2\psi = 0
\psi^\star
and subtract \psi
the complex conjugate of the Klein-Gordon equation. This results in:
\frac{\partial\rho}{\partial t}+\nabla\cdot\mathbf{j}=0
\begin{align*}
\rho=i\left[\psi^\star \frac{\partial\psi}{\partial t}-\left(\frac{\partial\psi^\star}{\partial t}\right)\psi\right] \\
\mathbf{j} = \frac{1}{i}\left[\psi^\star\nabla\psi - (\nabla\psi^\star)\psi\right]
\end{align*}
\partial_\mu j^\mu = 0
j^\mu = (\rho, \mathbf{j}) = i\left[\psi^\star\partial^\mu\psi - (\partial^\mu\psi^\star)\psi\right]
\psi
is Lorentz invariant, and \partial^\mu
is a contravariant four-vector, j^\mu
is also contravariant.\rho
is not, therefore, constrained to be positive definite. For plane wave solutions:
\begin{align*}
\psi=N\exp(-iEt-i\mathbf{p}\cdot\mathbf{x}) \\
\rho! = 2|N|^2E \\
E = \pm\sqrt{\mathbf{p}^2+m^2} \\
\Rightarrow \rho = \pm 2|N|^2\sqrt{\mathbf{p}^2+m^2}
\end{align*}
\frac{1}{\sqrt{2}}(u\bar{u}-d\bar{d})
can be considered at low energies. In order to deal with fermions (spin-1/2 particles) we need to look at the Dirac equation, which I might write about another time. Mathematically Correct Seventh Grade Mathematics Review
Dale Seymour Publications
Connected Mathematics Program
Lappan, Fey, Fitzgerald, Friel and Phillips
Menlo Park
--------------------------------------------------------------------------------
Introduction
This is part of a series of second, fifth! , and seventh grade Mathematics Program Reviews. This review i! ncludes a summary of the structure of the program, evaluations of a selected set of content areas, and evaluations of program quality. Ratings in these areas were made on a scale from 1 (poor) to 5 (outstanding). The overall evaluation was made using the traditional system of letter grades. For details of the methods used in this evaluation see Methods for Seventh Grade Program Reviews.
Student Text Structure
This course is composed of 8 "books" of about 70-90 pages each.
Each book is arranged around a mathematical topic
1. Variables and patterns
2. Stretching and shrinking
3. Comparing and scaling
4. Accentuate the negative
5. Moving straight ahead
6. Filling and wrapping
7. What do you expect?
8. Data around us
Content Area Evaluations
Properties, Order of Operations [1.0]
If this topic is covered, it is extremely difficult to find. In any case, the coverage is insuffici! ent.
Exponents, squares, roots [1.0]
This topic is very weak. Positive integers are raised to whole number powers only in the context of prime factorization. The small coverage of scientific notation includes only positive integer exponents and heavily emphasizes the use of calculators. All other topics are completely absent.
Fractions [1.0]
This topic is missing or cryptic.
Decimals [1.0]
None of these topics are presented in this book. Expressing decimals as percents is assumed. Perhaps students were taught to make this conversion on their calculators in an earlier grade.
Percents [1.2]
There is no evidence of development of this topic in this book. At the start of book 3 "percent" is described as one of the "terms developed in previous units." Perhaps so, but if so, the level of development was low. There is certainly no teaching of percent. Some percent problems are intermixed with r! atio problems in the various exercises, but there is no instru! ction on interconverting fractions, decimals and percents. There are almost no word problems on discount, markups, commissions, increase or decrease. Some "scale factors" for similarity are expressed as percents.
Proportions [3.5]
This is an adequate treatment of this topic. Most of the grade 7 topics are covered at some level. It is interesting that although proportions are used relatively often, by the standards of this book, they are not referred to as such as the authors have decided to put "proportion" in the list of nonessential terms at the front of the book.
Expressions and Equations - Simplifying and Solving [1.1]
This book is devoid of algebraic manipulation. The only solving of equations is graphical, and that is limited to problems involving direct variation. It is difficult to see how a student can become prepared for any mathematics-based profession with this little instruction in the key skills leading to algebra.
Expressions and Equations - Writing [2.1]
This book has a heavy emphasis on using proportions to find the lengths of similar parts of similar figures. On the other hand, there is very little practice or instruction in writing equations from a verbal description. The problems related to this topic are stretched over an excessive period of time as students answer endless questions about the situation. Essentially all of these problems are dealt with via tables and then in a graphical context.
Graphing [4.0]
The one advantage of the heavy emphasis that this book places on graphical over analytic solutions is that graphing is covered moderately well. Nearly all topics that should be covered are covered.
Shapes, Objects, Angles, Similarity, Congruence [2.5]
Formulas and derivations, or even "discoveries" of area of two dimensional figures are not given. They may be assumed to have been mastered at an earlier year. Surface a! rea and volume are "discovered" in a long series of constructi! on proje cts, many of which look doomed to failure. At the end of this formulas that have been discovered are not explicitly stated in the text. The teacher's manual suggests that the appropriate formulae will "come out" in discussion. If the student discovered the wrong formula, or forgot to write it down, good luck, since there is no way to look back and remember a formula.
The exercises on finding volumes of irregular objects using displacement are interesting extensions. On the other hand, much of the teaching is absurd and again abjures analysis for experiment. For example, students spend who-knows-how-much-time filling cylinders and cones with beans to discover, approximately, the relationship between the volume of cylinders and the volume of cones. This is a waste of time and inaccurate. Unfortunately, this could describe many of the activities in this book.
Area, Volume, Perimeter, Distance [1.0]
Essentially none of the grade 7 level topics ar! e covered. They may be assumed from previous years, but one cannot assume that from the presentation.
Program Quality Evaluations
Mathematical Depth [1.7]
There is very little mathematical content in this book. Students leaving this course will have no background in or facility with analytic or pre-algebra skills.
Quality of Presentation [1.4]
This book is completely dedicated to a constructivist philosophy of learning, with heavy emphasis on discovery exercises and rejection of whole class teacher directed instruction. The introduction to Part 1 says "Connected Mathematics was developed with the belief that calculators should be available and that students should decide when to use them." In one of the great understatements, the Guide to the Connected Mathematics Curriculum states, "Students may not do as well on standardized tests assessing computational skills as students in classes that spend" time practicing these ! skills.
Quality of Student Work [1.5]
St! udents a re busy, but they are not productively busy. Most of their time is directed away from true understanding and useful skills.
Overall Program Evaluation
F
Overall Evaluation [1.7]
This rating is perhaps deceivingly high, as 7 of the 11 topics rate no higher than 1.2. The rating is as high as it is based largely on two high subscores, proportions and graphing. It is impossible to recommend a book with as little content as this and an inefficient, if philosophically attractive, instructional method.
Polynomials are one of the most important concepts in algebra and througho! ut mathematics and science. They are used to form polynomial equations, which encode a wide range of problems, from elementary word problems to complicated problems in the sciences; they are used to define polynomial functions, which appear in settings ranging from basic chemistry and physics to economics, and are used in calculus and numerical analysis to approximate other functions. Polynomials are used to construct polynomial rings, one of the most powerful concep! ts in algebra and algebraic geometry.
Overview
|
A polynomial is either zero, or can be written as the sum of one or more non-zero terms. The number of terms is finite. These terms consist of a constant (called the coefficient of the term) multiplied by zero or more variables (which are usually represented by letters). Each variable may have an exponent that is a non-negative integer. The exponent on a variable in a term is equal to the degree of that variable in that term. Since x = x1, the degree of a variable without a written exponent is one. A term with no variables is called a constant term, or just a constant. The degree of a constant term is 0. The coefficient of a term may be any number, including fractions, irrational numbers, negative numbers, and ! complex numbers.
For e! xample,< /p>
is a term. The coefficient is –5, the variables are x and y, the degree of x is two, and the degree of y is one.
The degree of the entire term is the sum of the degrees of each variable in it. In the example above, the degree is 2 + 1 = 3.
A polynomial is a sum of terms. For example, the following is a polynomial:
It consists of three terms: the first is degree two, the second is degree one, and the third is degree zero. Here "− 5x" stands for "+ (−5)x", so the coefficient of the middle term is −5.
When a polynomial in one variable is arranged in the traditional order, the terms of higher degree come before the terms of lower degree. In the first term above, the coefficient is 3, the variable is x, and the exponent is 2. In the second term, the coefficient is –5. T! he third term is a constant. The degree of a non-zero p! olynomia l is the largest degree of any one term. In this example, the polynomial has degree two.
An expression that can be converted to polynomial form through a sequence of applications of the commutative, associative, and distributive laws is usually considered to be a polynomial. For instance,
is a polynomial because it can be worked out to x3 + 3x2 + 3x + 1. Similarly,
is considered a valid term in a polynomial, even though it involves a division, because it is equivalent to and is just a constant. The coefficient of this term is therefore . For similar reasons, if complex coefficients are! allowed, one may have a single term like (2 + 3 i)x3; even though it looks like it should be worked out to two terms, the complex number 2+3i is in fact just a single coefficient in this case that happens to require a "+" to be written down.
Division by an expression containing a variable is not generally allowed in polynomials.[1] For example,
is not a polynomial because it includes division by a variable. Similarly,
is not a polynomial, because it has a variable exponent.
Since subtraction can be treated as addition of the additive opposite, and since exponentiation to a constant positive whole number power can be treated as repeated multiplication, polynomials can be constructed from constants and variables with just the two operations addition and multiplication.
A polynomial function is a function defined by evaluating a polynomial. A function Æ' of one argument is called a polynomial function if it satisfies
for all arguments x, where n is a nonnegative integer and a0, a1,a2, ..., an are constant coefficients.
For example, the function Æ', taking real numbers to real numbers, defined by
is a polynomial function of one argument. Polynomial functions of multiple arguments can also be defined, using polynomials in multiple variables, as in
Polynomial functions are an important class of smooth functions.
A polynomial equation is an equation in which a polynomial is set equal to another polynomial.
is a polynomial equation. In case of a polynomial equation the variable is considered an unknown, and one seeks to find the possi! ble valu es for which both members of the equation evaluate to the same value (in general more than one solution may exist). A polynomial equation is to be contrasted with a polynomial identity like (x + y)(x – y) = x2–y2, where both members represent the same polynomial in different forms, and as a consequence any evaluation of both members will give a valid equality.
Polynomials serve to approximate other functions, such as sine, cosine, and exponential.
All polynomials have an expanded form, in which the distributive law has been used to remove all brackets. All polynomials with real or complex coefficients also have a factored form in which the polynomial is written as a product of linear polynomials. For example, the polynomial
is the expanded form of the polynomial
which is written in factored form. Note that the constants in the linear polynomial! s (like -3 and +1 in the above example) may be complex numbers in certain cases, even if all coefficients of the expanded form are real numbers. This is because the field of real numbers is not algebraically closed; however, the fundamental theorem of algebra states that the field of complex numbers is algebraically closed.
In school algebra, students learn to move easily from one form to the other (see: factoring).
Every polynomia! l in one variable is equivalent to a polynomial with the form
This form is sometimes taken as the definition of a polynomial in one variable.
Evaluation of a polynomial consists of assigning a number to each variable and carrying out the indicated multiplications and additions. Evaluation is sometimes performed more efficiently using the Horner scheme
In elementary alge! bra, methods are given for solving all first degree and second degree polynomial equations in one variable. In the case of polynomial equations, the variable is often called an unknown. The number of solutions may not exceed the degree, and will equal the degree when multiplicity of solutions and complex number solutions are counted. This fact is called the fundamental theorem of algebra.
A system of polynomial equations is a set of equations in which a given variable must take on the same value everywhere it appears in any of the equations. Systems of equations are usually grouped with a single open brace on the left. In elementary algebra, methods are given for solving a system of linear equations in several unknowns. To get a unique solution, the number of equations should equal the number of unknowns. If there are more unknowns than equations, the system is called underdetermined. If there are more equations than unknowns, the system is called overdetermined. This important subject is studied extensively in the area of mathematics known as linear algebra. Overdetermined systems are common in practical applications. For example, one U.S. mapping survey used computers to solve 2.5 million equations in 40! 0,000 unknowns.[2]
| This article may require cleanup to meet Wikipedia's quality standards. Please improve this article if you can. (Septemb! er 2008) |
The earliest known use of the equal sign is in Robert Recorde's The Whetstone of Witte, 1557. The signs + for addition, − for subtraction, and the use of a letter for an unknown appear in Michael Stifel's Arithemetica integra, 1544. René Descartes, in La géometrie, 1637, int! roduced the concept of the graph of a polynomial equation. He ! populari zed the use of letters from the beginning of the alphabet to denote constants and letters from the end of the alphabet to denote variables, as can be seen above, in the general formula for a polynomial in one variable, where the a 's denote constants and x denotes a variable. Descartes introduced the use of superscripts to denote exponents as well.[3]
Every polynomial corresponds to a polynomial function, where f(x) is set equal to the polynomial, and to a polynomial equation, where the polynomial is set equal to zero. The so! lutions to the equation are called the roots of the polynomial and they are the zeroes of the function and the x-intercepts of its graph. If x = a is a root of a polynomial, then (x − a) is a factor of that polynomial.
Some polynomials, such as f(x) = x2 + 1, do not have any roots among the real numbers. If, however, the set of allowed candidates is expanded to the complex numbers, every (non-constant) polynomial has at least one distinct root; this follows from the fundamental theorem of algebra.
There is a difference between approximating roots and fin! ding exact roots. Formulas for the roots of polynomials up to ! a degree of 2 have been known since ancient times (see quadratic equation) and up to a degree of 4 since the 16th century (see Gerolamo Cardano, Niccolo Fontana Tartaglia). But formulas for degree 5 eluded researchers. In 1824, Niels Henrik Abel proved the striking result that there can be no general formula (involving only the arithmetical operations and radicals) for the roots of a polynomial of degree 5 or greater in terms of its coefficients (see Abel-Ruffini theorem). This result marked the start of Galois theory which engages in a detailed study of relationships among roots of polynomials.
Numerically solving a polynomial equation in one unknown is easily done on a computer by the Durand-Kerner method or by some other root-finding algorithm. The reduction of equations in several unknowns to equations each in one unknown is discussed in the article on the Buchberger's algorithm. The special case where all the polynomials are of degree one is cal! led a system of linear equations, for which a range of different solution methods exist, including the classical gaussian elimination.
It has been shown by Richard Birkeland and Karl Meyr that the roots of any polynomial may be expressed in terms of multivariate hyperg! eometric functions. Ferdinand von Lindemann and Hiroshi Umemura showed that the roots may also be expressed in terms of Siegel modular functions, generalizations of the theta functions that appear in the theory of elliptic functions. These characterizations of the roots of arbitrary polynomials are generalizations of the methods previously discovered to solve the quin tic equation.
A polynomial function in one real variable can be represented by a graph.
Polynomial graphs are analyzed in calculus using intercepts, slopes, concavity, and end behavior.
The illustrations below show graphs of polynomials.
One important aspect of calculus is the project of analyzing complicated functions by means of approximating them with polynomials. The culmination of these efforts is Taylor's theorem, which roughly states that every differentiable function locally looks like a polynomial, and the Stone-Weierstrass theorem, which states that every continuous function defined on a compact interval of the real axis can be approximated on the whole interval as closely as desired by a polynomial. Polynomials are also frequently used to interpolate functions.
Quotients of polynomials are called rational expressions, and functions that evaluate rational expressions are called rational functions. Rational functions are the only functions that can be evaluated on a computer by a fixed sequence of instructions involving operations of addition, multiplication, division, which operations on floating point numbers are usually implemented in hardware. All the other functions that computers need to evaluate, such as trigonometric functions, logarithms and exponential functions, must then be computed in software that may use approximations to those functions on certain intervals by rational functions, and possibly iteration.Calculating derivatives and integrals of polynomials is particularly simple. For the polynomial
the derivative with respect to x is
and the indefin! ite inte gral is
In abstract algebra, one must take care to distinguish between polynomials and polynomial functions. A polynomial f in one variable X over a ring R is defined to be a formal expression of the form
where n is a natural number, the coefficients are elements of R, Here X is a formal symbol, whose powers Xi are at this point just placeholders for the corresponding coefficients ai, so that the given formal expression is just a way to encode the sequence (a0,a1,...), where there is an N such that! ai=0 for all i>N. Two ! polynomi als sharing the same value of n are considered to be equal if and only if the sequences of their coefficients are equal; furthermore any polynomial is equal to any polynomial with greater value of n obtained from it by adding terms in front whose coefficient is zero. These polynomials can be added by simply adding corresponding coefficients (the rule for extending by terms with zero coefficients can be used to make sure such coefficients exist). Thus each polynomial is actually equal to the sum of the terms used in its formal expression, if such a term aiXi is interpreted as a polynomial that has zero coefficients at all powers of X other than Xi. Then to define multiplication, it suffices by the distributive law to desc! ribe the product of any two such terms, which is given by the rule
Thus the set of all polynomials with coefficients in the ring R forms itself a ring, the ring of polynomials over R, which is denoted by R[X]. The map from R to R[X] sending r to rX0 is an injective homomorphism of rings, by which R is viewed as a subring of R[X]. If R is commu tative, then R[X] is an algebra over R.
One can think of the ring R[X] as arising from R by adding one new element X to R, and extending in a minimal way to a ring in which X satisfies no other relations than the obligatory ones, plus commutation with all elements of R (that is Xr = rX). To do this, one must add all powers of X and their linear combinations as well.
Formation of the polynomial ring, together with forming factor rings by factoring out ideals, are important tools for constructing new rings out of known ones. For instance, the ring (in fact field) of complex numbers! , which can be constructed from the polynomial ring R[X] over the real numbers by factoring out the ideal of multiples of the polynomial X2 + 1. Another example is the construction of finite fields, which proceeds similarly, starting out with the field of integers modulo some prime number as the coefficient ring R (see modular arithmetic).
If R is commutative, then one can associate to every polynomial P in R[X], a polynomial function f wi! th domain and range equal to R (mo re generally one can take domain and range to be the same unital associative algebra over R). One obtains the value f(r) by everywhere replacing the symbol X in P by r. One reason that algebraists distinguish between polynomials and polynomial functions is that over some rings different polynomials may give rise to the same polynomial function (see Fermat's little theorem for an example where R is the integers modulo p). This is not the case when R is the real or complex numbers and therefore many analysts often don't separate the two concepts. An even more important reason to distinguish between polynom! ials and polynomial functions is that many operations on polynomials (like Euclidean division) require looking at what a polynomial is composed of as an expression rather than evaluating it at some constant value for X. And it should be noted that if R is not commutative, there is no (well behaved) notion of polynomial function at all.
In commutative algebra, one major focus of study is divisibility among polynomials. If R is an integral domain and f and g are polynomials in R[X], it is said that f divides g if there exists a polynomial q in R[X] such that f q = g. One can then show that "every zero gives rise to a linear factor", or more formally: if f is a polynomial in R[X] and r is an element of R such that f(r) = 0, then the polynomial (X − r) divides f. The converse is also true. The quotient can be computed using the Horner scheme.
If F is a field and f and g are polynomials in F[X] with g ≠ 0, then there exist unique polynomials q and r in F[X] with
and such that the degree of r is smaller than the degree of g. The polynomials q and r are uniquely determined by f and g. This is called "division with remainder" or "polynomial long division" and shows that the ring F[X] is a Euclidean domain.
Analogously, polynomial "primes" (more correctly, irreducible polynomials) can be defined which cannot be factorized into the product of two polynomials of lesser degree. It is not easy to determine if a given polynomial is irreducible. One can start by simply checking if the polynomial has linear factors. Then, one can check divisibility by some other irreducible polynomials. Eisenstein's criterion can also be used in some cases to determine irreducibility.
See also: Greatest common divisor of two polynomials.
The most important classification of polynomials is based on the number of distinct variables. A polynomial in! one variable is called a univariate polynomial, a polynomial in more than one variable is called a multivariate polynomial. These notions refer more to the kind of polynomials one is generally working with than to individual polynomials; for instance when working with univariate polynomials one does not exclude constant polynomials (which may result for instance from the subtraction of non-constant polynomials), although strictly speaking constant polynomials do not contain any variables at all. It is possible to further classify multivariate polynomials as bivariate, trivariate etc., according to the number of variables, but this is rarely done; it is more common for instance to say simply "polynomials in x, y, and z". A (usually multivariate) polynomial is called homogeneous of degree n if all! its terms have degree ! n .
Univariate polynomials have many properties not shared by multivariate polynomials. For instance, the terms of a univariate polynomial are completely ordered by their degree, and it is conventional to always write them in order of decreasing degree. A univariate polynomial in x of degree n then takes the general form
where cn, cn-1, ..., c2, c1 and c0 are constants, the coefficients of this polynomial. Here the term cnxn is called the leading term and its coefficient cn the leading coefficient; i! f the leading coefficient is 1, the univariate polynomial is called monic. Note that apart from the leading coefficient cn (which must be non-zero or else the polynomial would not be of degree n) this general form allows for coefficients to be zero; when this happens the corresponding term is zero and may be removed from the sum without changing the polynomial. It is nevertheless common to refer to ci as the coefficient of xi, even when ci happens to be 0, so that xi does not really occur in any term; for instance one can speak of the constant term of the polynomial, meaning c0 even if it should be zero.
Polynomials can similarly be class! ified by the kind of constant values allowed as coefficients. ! One can work with polynomials with integral, rational, real or complex coefficients, and in abstract algebra polynomials with many other types of coefficients can be defined. Like for the previous classification, this is about the coefficients one is generally working with; for instance when working with polynomials with complex coefficients one includes polynomials whose coefficients happen to all be real, even though such polynomials can also be considered to be a polynomials with real coefficients.
Polynomials can further be classified by their degree and/or the number of non-zero terms they contain.
Degree | Name | Example |
---|---|---|
−∞ | zero | 0 |
0 | (non-zero) const! ant | 1 |
1 | linear | x + 1 |
2 | quadratic | x2 + 1 |
3 | cubic | x3 + 1 |
4 | quartic (or biquadratic) | x4 + 1 |
5 | quintic | x5 + 1 |
6 | sextic or hexic | x6 + 1 |
7 | septic or heptic | x7 + 1 |
8 | octic | x8 + 1 |
9 | nonic | x9 + 1 |
10 | decic | x10 + 1 |
Usually, a polynomial of degree 4 or higher is referred to as a polynomial of degree n, although the phrases quartic polynomial and quin! tic polynomial are also used. The names for degrees higher than 5 are even less common. The names for the degrees may be applied to the polynomial or to its terms. For example, a constant may refer to a zero degree polynomial or to a zero degree term.
The polynomial 0, which may be considered to have no terms at all, is called the zero polynomial. Unlike other constant polynomials, its degree is not zero. Rather the degree of the zero polynomial is either left explicitly undefined, or defined to be negative (either –1 or –∞).[4] The latter convention is important when defining Euclidean division of polynomials.
Number of non-zero terms | Name | Example |
---|---|---|
0 | zero polynomial | 0 |
1 | monomial | x2 |
2 | binomial | x2 + 1 |
3 | trinomial | x2 + x + 1 |
The word monomial can be ambiguous, as it is also often used to denote just a power of the variable, or in the multivariate case product of such powers, without any coefficient. Two or more terms which involve the same monomial in the latter sense, in other words which differ only in the value of th! eir coefficients, are called similar terms; they can be combined into a single term by adding their coefficients; if the resulting term has coefficient zero, it may be removed altogether. The above classification according to the number of terms assumes that similar terms have been combined first.
Polynomials are frequently used to encode information about some other object. The characteristic polynomial of a matrix or linear operator contains information about the operator's eigenvalues. The minimal polynomial of an algebraic element records the simplest algebraic relation satisfied by that element. The chromatic polynomial of a graph counts the number of proper colourings of that graph.
Polynomials can involve more than one variable, in which they are called multivariate. Rings of polynomials in a finite nu! mber of variables are of fundamental importance in algebraic geometry which studies the simultaneous zero sets of several such multivariate polynomials. These rings can alternatively be constructed by repeating the construction of univariate polynomials with as ceofficient ring another ring of polynomials: thus the ring R[X,Y] of polynomials in X and Y can be viewed as the ring (R[X])[Y] of polynomials in Y with as coeffcients polynomials in X, or as the ring (R[Y])[X] of polynomials in X with as coeffcients polynomials in Y. These identifications are compatible with arithmetic operations (they are isomorphisms of rings), but some notions such as degree or whether a polynomial is considered monic can change be! tween these points of view. One can construct rings of polynom! ials in infinitely many variables, but since polynomials are (finite) expressions, any individual polynomial can only contain finitely many variables.
Laurent polynomials are like polynomials, but allow negative powers of the variable(s) to occur.
Rational functions are formal quotients of polynomials (they are formed from polynomials just as rational numbers are formed from integers, writing a fraction of two of them; fractions related by the cancelling of common factors are identified with each other). The rational functions contain the Laurent polynomials, but do not limit denominators to ! be powers of a variable.
Formal power series are like polynomials, but allow infinitely many nonzero terms to occur, so that they do not have finite degree. Unlike polynomials they cannot in general be explicitly and fully written down (just like real numbers cannot), but the rules for manipulating their terms are the same as for polynomials.