This document discusses partial derivatives, which are used to describe the rate of change of functions with multiple variables. It defines:
1) Partial derivatives as the rate of change of the dependent variable with respect to one independent variable, while holding other variables constant.
2) Functions of two variables have level curves where the function value is constant. Their graphs are surfaces in 3D space.
3) Higher order partial derivatives describe the rate of change of the first partial derivatives.
4) The chain rule extends differentiation to composite functions, allowing functions of variables that are themselves functions of other variables.
The document discusses Fourier series, which represent periodic functions as an infinite series of sines and cosines. Fourier series can be used to represent functions that are discontinuous or non-differentiable. The key formulas for the Fourier series coefficients are presented. Fourier series expansions take different forms depending on whether the function is even, odd, or defined on different intervals. Half-range Fourier series are also discussed as representations of functions defined on half periods.
Analytic Function, C-R equation, Harmonic function, laplace equation, Construction of analytic function, Critical point, Invariant point , Bilinear Transformation
The document discusses partial differentiation and its applications. It covers functions of two variables, first and second partial derivatives, and applications including the Cobb-Douglas production function and finding marginal productivity from a production function. Examples are provided to demonstrate calculating partial derivatives of various functions and applying partial derivatives in contexts like production analysis.
1. The document defines ordinary and partial differential equations and discusses the order and degree of differential equations.
2. Examples of common second order linear differential equations with constant coefficients are given, including equations for free fall, spring displacement, and RLC circuits.
3. The document also discusses homogeneous linear equations and Newton's law of cooling as examples of differential equations.
Partial derivatives are used to calculate the rate of change of a function of two or more variables with respect to one variable, while holding the other variables constant. The partial derivative of z with respect to x, denoted ∂z/∂x, is defined as the limit of the difference quotient as Δx approaches 0, while holding y constant. Similarly, the partial derivative of z with respect to y, denoted ∂z/∂y, is defined as the limit of the difference quotient as Δy approaches 0, while holding x constant. Notations for higher order partial derivatives are also introduced. An example problem finds the first and second order partial derivatives of the function z=x^2y^3+6
The document is an introduction to ordinary differential equations prepared by Ahmed Haider Ahmed. It defines key terms like differential equation, ordinary differential equation, partial differential equation, order, degree, and particular and general solutions. It then provides methods for solving various types of first order differential equations, including separable, homogeneous, exact, linear, and Bernoulli equations. Specific examples are given to illustrate each method.
1) The document presents information on ordinary differential equations including definitions, types, order, degree, and solution methods.
2) Differential equations can be written in derivative, differential, and differential operator forms. Common solution methods covered are variable separable, homogeneous, linear, and exact differential equations.
3) Applications of differential equations include physics, astronomy, meteorology, chemistry, biology, ecology, and economics for modeling various real-world systems.
A partial differential equation contains one dependent variable and more than one independent variable. The partial derivatives of a function f(x,y) with respect to x and y at a point (x,y) are represented as ∂f/∂x and ∂f/∂y. Higher order partial derivatives can be found by taking partial derivatives multiple times with respect to the independent variables. The chain rule can be used to find partial derivatives when the dependent variable is a function of other variables that are themselves functions of the independent variables.
The document discusses Fourier series, which represent periodic functions as an infinite series of sines and cosines. Fourier series can be used to represent functions that are discontinuous or non-differentiable. The key formulas for the Fourier series coefficients are presented. Fourier series expansions take different forms depending on whether the function is even, odd, or defined on different intervals. Half-range Fourier series are also discussed as representations of functions defined on half periods.
Analytic Function, C-R equation, Harmonic function, laplace equation, Construction of analytic function, Critical point, Invariant point , Bilinear Transformation
The document discusses partial differentiation and its applications. It covers functions of two variables, first and second partial derivatives, and applications including the Cobb-Douglas production function and finding marginal productivity from a production function. Examples are provided to demonstrate calculating partial derivatives of various functions and applying partial derivatives in contexts like production analysis.
1. The document defines ordinary and partial differential equations and discusses the order and degree of differential equations.
2. Examples of common second order linear differential equations with constant coefficients are given, including equations for free fall, spring displacement, and RLC circuits.
3. The document also discusses homogeneous linear equations and Newton's law of cooling as examples of differential equations.
Partial derivatives are used to calculate the rate of change of a function of two or more variables with respect to one variable, while holding the other variables constant. The partial derivative of z with respect to x, denoted ∂z/∂x, is defined as the limit of the difference quotient as Δx approaches 0, while holding y constant. Similarly, the partial derivative of z with respect to y, denoted ∂z/∂y, is defined as the limit of the difference quotient as Δy approaches 0, while holding x constant. Notations for higher order partial derivatives are also introduced. An example problem finds the first and second order partial derivatives of the function z=x^2y^3+6
The document is an introduction to ordinary differential equations prepared by Ahmed Haider Ahmed. It defines key terms like differential equation, ordinary differential equation, partial differential equation, order, degree, and particular and general solutions. It then provides methods for solving various types of first order differential equations, including separable, homogeneous, exact, linear, and Bernoulli equations. Specific examples are given to illustrate each method.
1) The document presents information on ordinary differential equations including definitions, types, order, degree, and solution methods.
2) Differential equations can be written in derivative, differential, and differential operator forms. Common solution methods covered are variable separable, homogeneous, linear, and exact differential equations.
3) Applications of differential equations include physics, astronomy, meteorology, chemistry, biology, ecology, and economics for modeling various real-world systems.
A partial differential equation contains one dependent variable and more than one independent variable. The partial derivatives of a function f(x,y) with respect to x and y at a point (x,y) are represented as ∂f/∂x and ∂f/∂y. Higher order partial derivatives can be found by taking partial derivatives multiple times with respect to the independent variables. The chain rule can be used to find partial derivatives when the dependent variable is a function of other variables that are themselves functions of the independent variables.
The document presents information on partial differentiation including:
- Partial differentiation involves a function with more than one independent variable and partial derivatives.
- Notation for partial derivatives is presented.
- Methods for computing first and higher order partial derivatives are explained with examples.
- The concepts of homogeneous functions and the chain rule for partial differentiation are defined.
- Green's Theorem relates a line integral around a closed curve C to a double integral over the region D bounded by C. It expresses the line integral as the double integral of the curl or divergence of the vector field over D.
- The curl and divergence operators can be used to write Green's Theorem in vector forms involving the tangential and normal components of the vector field along C.
- Parametric surfaces in 3D space can be described by a vector-valued function r(u,v) of two parameters u and v. The set of points traced out by this function as u and v vary is the parametric surface.
1. The document provides information on multiple integrals including double integrals, triple integrals, and integrals in spherical and cylindrical coordinates. It defines each type of integral and gives their general formulas.
2. Examples are provided for calculating double and triple integrals over different regions in rectangular, cylindrical, and spherical coordinate systems. The order of integration can be changed by considering strips or slices of the region.
3. Properties of the integrals include applying Fubini's theorem to change the order of integration, and relating the triple integral over a region to the double integral over the bounds and integrating over the third variable.
1) First order ordinary linear differential equations can be expressed in the form dy/dx = p(x)y + q(x), where p and q are functions of x.
2) There are several types of first order linear differential equations, including separable, homogeneous, exact, and linear equations.
3) Separable equations can be solved by separating the variables and integrating both sides. Homogeneous equations involve functions that are homogeneous of the same degree in x and y.
This document provides an overview of different types of differential equations. It defines ordinary and partial differential equations, and explains that ordinary differential equations contain only ordinary derivatives while partial differential equations contain partial derivatives. It also defines key concepts like the order of a differential equation as the order of the highest derivative, and the degree as the power of the highest order derivative. The document then describes various types of first order differential equations including separable variables, homogeneous, linear, and exact equations. Examples are provided for each type.
La transformada de Fourier es una operación matemática que transforma una señal del dominio del tiempo al dominio de la frecuencia y viceversa. Permite descomponer una señal en componentes de diferentes frecuencias, mostrando cómo se distribuye la energía de la señal a través del espectro de frecuencias. Tiene muchas aplicaciones importantes en áreas como el procesamiento de señales, diseño de filtros, resolución de ecuaciones diferenciales y tratamiento digital de imágenes.
The document discusses key concepts in calculus including continuity, differentiation, integration, and their applications. It defines continuity as being able to draw a function's graph without lifting the pen, and differentiation as computing the rate of change of a dependent variable with respect to changes in the independent variable. The document also covers differentiation rules and techniques for implicit, inverse, exponential, logarithmic, and parametric functions.
Using integration by parts, one can evaluate integrals of more complex functions. The formula for integration by parts is:
(u dv - v du) where u and v are the integral and derivative of two functions. Several examples show how to choose u and v and apply the formula repeatedly to simplify integrals. Integration by parts can also be used to evaluate definite integrals using the Fundamental Theorem of Calculus.
Any analytic function is locally represented by a convergent power series and is infinitely differentiable. Real analytic functions are defined on an open set of the real line, while complex analytic functions are defined on an open set of the complex plane. Both are infinitely differentiable, but complex analytic functions have additional properties like Liouville's theorem stating bounded complex analytic functions defined on the whole complex plane are constant. Real analytic functions do not have this property and their power series need only converge locally rather than on the entire domain.
This document provides two examples of using double and triple integrals to calculate the moment of inertia and volume of solids. The first example calculates the moment of inertia of a solid inside a cylinder using cylindrical coordinates. The second example finds the volume of a solid inside a sphere and outside a cone using spherical coordinates. It converts the equations to spherical coordinates and sets up the integral to evaluate the volume.
This document summarizes Chapter 10 from a mathematics textbook. The chapter covers limits and continuity. It introduces limits, such as one-sided limits and limits at infinity. It defines continuity as a function being continuous at a point if the limit exists and is equal to the function value. Discontinuities can occur if a limit does not exist or is infinite. The chapter applies limits and continuity to solve inequalities involving polynomials and rational functions. Examples show how to use the definition of a limit to evaluate various types of limits and test continuity.
The document discusses various topics related to complex functions and complex analysis. It defines concepts such as distance between complex numbers, circles, circular disks, neighborhoods, annuli, open and closed sets, connected sets, domains, regions, bounded regions, single-valued and multi-valued functions, and limits and continuity of complex functions. Specific examples are provided to illustrate definitions of circles, neighborhoods, single-valued and multi-valued functions. The limit of a complex function as z approaches a point z0 is defined using the epsilon-delta definition of a limit.
First order linear differential equationNofal Umair
1. A differential equation relates an unknown function and its derivatives, and can be ordinary (involving one variable) or partial (involving partial derivatives).
2. Linear differential equations have dependent variables and derivatives that are of degree one, and coefficients that do not depend on the dependent variable.
3. Common methods for solving first-order linear differential equations include separation of variables, homogeneous equations, and exact equations.
This document outlines the 7 steps for sketching the curve of a function: 1) Determine the domain, 2) Find critical points, 3) Determine graph direction and max/min, 4) Use the second derivative to find concavity and points of inflection, 5) Find asymptotes, 6) Find intercepts and important points, 7) Combine evidence to graph the function. Key tests are outlined for max/min, concavity, and points of inflection using the first and second derivatives.
The document discusses inverse functions. An inverse function reverses the input and output of a function. For a function f(x) to have an inverse function f-1(y), it must be one-to-one, meaning that different inputs produce different outputs. The inverse of a function f(x) is found by solving the original function equation for x in terms of y. Examples show finding the inverse of specific functions like f(x) = x - 5 by solving for x. A function is one-to-one if for any two different inputs u and v, their outputs f(u) and f(v) are also different.
The document discusses surface integrals. It defines a surface integral as integrating a density function w over a surface σ. The surface σ is defined by a function z=f(x,y) over a domain D. The surface is partitioned into small patches, and each patch's area is approximated. The total mass of the surface is calculated as the limit of Riemann sums as the partitions approach zero. An example calculates the mass of a density function over a spherical surface portion.
- A differential equation involves an independent variable, dependent variable, and derivatives of the dependent variable with respect to the independent variable.
- The order of a differential equation is the order of the highest derivative, and the degree is the exponent of the highest order derivative.
- Linear differential equations involve the dependent variable and its derivatives only to the first power. Non-linear equations do not meet this criterion.
- The general solution of a differential equation contains as many arbitrary constants as the order of the equation. A particular solution results from assigning values to the arbitrary constants.
- Differential equations can be solved through methods like variable separation, inspection of reducible forms, and finding homogeneous or linear representations.
Este documento describe los conceptos fundamentales de la integración o antiderivación. Explica que una función F es una primitiva de f si su derivada es f, y que cualquier función de la forma F(x)+C también es una primitiva de f. Además, introduce las nociones de integral indefinida, integral definida, y el Teorema Fundamental del Cálculo.
The document provides an overview of the Mean Value Theorem and Rolle's Theorem. It discusses that the Mean Value Theorem states that for any function continuous on a closed interval, there exists a point where the slope of the tangent line equals the slope of the secant line through the endpoints. Rolle's Theorem is a special case where if a function is continuous on a closed interval and differentiable on the open interval, if the function is equal at the endpoints, the derivative at some interior point is zero. Graphical interpretations are also provided to illustrate these theorems.
Functions and its Applications in MathematicsAmit Amola
A function is a relation between a set of inputs and set of outputs where each input is related to exactly one output. An example is given of a function that relates shapes to colors, where each shape maps to one unique color. A function can be written as a set of ordered pairs, where the input comes first and the output second. The domain is the set of inputs, the codomain is the set of possible outputs, and the range is the set of outputs the function actually produces. A function is one-to-one if no two distinct inputs map to the same output, and onto if every element in the codomain is mapped to by at least one input.
This document is a calculus supplement to accompany a microeconomics textbook. It introduces the concept of partial derivatives and shows how they can be used to analyze economic concepts from the textbook like demand and supply functions, substitutes and complements, and elasticities. Partial derivatives allow the slope of demand and supply functions to be determined with respect to different variables. They also allow elasticities to be defined and calculated using calculus, providing an equivalent but alternative method to the algebraic approach in the textbook. The supplement aims to illustrate the connections between calculus and microeconomic concepts.
This document provides an outline for a calculus lecture on basic differentiation rules. It includes objectives to understand the derivative of constants, the constant multiple rule, the sum rule, the difference rule, and derivatives of sine and cosine. Examples are provided to find the derivatives of squaring, cubing, square root, and cube root functions using the definition of the derivative. Graphs and properties of these functions and their derivatives are also discussed.
The document presents information on partial differentiation including:
- Partial differentiation involves a function with more than one independent variable and partial derivatives.
- Notation for partial derivatives is presented.
- Methods for computing first and higher order partial derivatives are explained with examples.
- The concepts of homogeneous functions and the chain rule for partial differentiation are defined.
- Green's Theorem relates a line integral around a closed curve C to a double integral over the region D bounded by C. It expresses the line integral as the double integral of the curl or divergence of the vector field over D.
- The curl and divergence operators can be used to write Green's Theorem in vector forms involving the tangential and normal components of the vector field along C.
- Parametric surfaces in 3D space can be described by a vector-valued function r(u,v) of two parameters u and v. The set of points traced out by this function as u and v vary is the parametric surface.
1. The document provides information on multiple integrals including double integrals, triple integrals, and integrals in spherical and cylindrical coordinates. It defines each type of integral and gives their general formulas.
2. Examples are provided for calculating double and triple integrals over different regions in rectangular, cylindrical, and spherical coordinate systems. The order of integration can be changed by considering strips or slices of the region.
3. Properties of the integrals include applying Fubini's theorem to change the order of integration, and relating the triple integral over a region to the double integral over the bounds and integrating over the third variable.
1) First order ordinary linear differential equations can be expressed in the form dy/dx = p(x)y + q(x), where p and q are functions of x.
2) There are several types of first order linear differential equations, including separable, homogeneous, exact, and linear equations.
3) Separable equations can be solved by separating the variables and integrating both sides. Homogeneous equations involve functions that are homogeneous of the same degree in x and y.
This document provides an overview of different types of differential equations. It defines ordinary and partial differential equations, and explains that ordinary differential equations contain only ordinary derivatives while partial differential equations contain partial derivatives. It also defines key concepts like the order of a differential equation as the order of the highest derivative, and the degree as the power of the highest order derivative. The document then describes various types of first order differential equations including separable variables, homogeneous, linear, and exact equations. Examples are provided for each type.
La transformada de Fourier es una operación matemática que transforma una señal del dominio del tiempo al dominio de la frecuencia y viceversa. Permite descomponer una señal en componentes de diferentes frecuencias, mostrando cómo se distribuye la energía de la señal a través del espectro de frecuencias. Tiene muchas aplicaciones importantes en áreas como el procesamiento de señales, diseño de filtros, resolución de ecuaciones diferenciales y tratamiento digital de imágenes.
The document discusses key concepts in calculus including continuity, differentiation, integration, and their applications. It defines continuity as being able to draw a function's graph without lifting the pen, and differentiation as computing the rate of change of a dependent variable with respect to changes in the independent variable. The document also covers differentiation rules and techniques for implicit, inverse, exponential, logarithmic, and parametric functions.
Using integration by parts, one can evaluate integrals of more complex functions. The formula for integration by parts is:
(u dv - v du) where u and v are the integral and derivative of two functions. Several examples show how to choose u and v and apply the formula repeatedly to simplify integrals. Integration by parts can also be used to evaluate definite integrals using the Fundamental Theorem of Calculus.
Any analytic function is locally represented by a convergent power series and is infinitely differentiable. Real analytic functions are defined on an open set of the real line, while complex analytic functions are defined on an open set of the complex plane. Both are infinitely differentiable, but complex analytic functions have additional properties like Liouville's theorem stating bounded complex analytic functions defined on the whole complex plane are constant. Real analytic functions do not have this property and their power series need only converge locally rather than on the entire domain.
This document provides two examples of using double and triple integrals to calculate the moment of inertia and volume of solids. The first example calculates the moment of inertia of a solid inside a cylinder using cylindrical coordinates. The second example finds the volume of a solid inside a sphere and outside a cone using spherical coordinates. It converts the equations to spherical coordinates and sets up the integral to evaluate the volume.
This document summarizes Chapter 10 from a mathematics textbook. The chapter covers limits and continuity. It introduces limits, such as one-sided limits and limits at infinity. It defines continuity as a function being continuous at a point if the limit exists and is equal to the function value. Discontinuities can occur if a limit does not exist or is infinite. The chapter applies limits and continuity to solve inequalities involving polynomials and rational functions. Examples show how to use the definition of a limit to evaluate various types of limits and test continuity.
The document discusses various topics related to complex functions and complex analysis. It defines concepts such as distance between complex numbers, circles, circular disks, neighborhoods, annuli, open and closed sets, connected sets, domains, regions, bounded regions, single-valued and multi-valued functions, and limits and continuity of complex functions. Specific examples are provided to illustrate definitions of circles, neighborhoods, single-valued and multi-valued functions. The limit of a complex function as z approaches a point z0 is defined using the epsilon-delta definition of a limit.
First order linear differential equationNofal Umair
1. A differential equation relates an unknown function and its derivatives, and can be ordinary (involving one variable) or partial (involving partial derivatives).
2. Linear differential equations have dependent variables and derivatives that are of degree one, and coefficients that do not depend on the dependent variable.
3. Common methods for solving first-order linear differential equations include separation of variables, homogeneous equations, and exact equations.
This document outlines the 7 steps for sketching the curve of a function: 1) Determine the domain, 2) Find critical points, 3) Determine graph direction and max/min, 4) Use the second derivative to find concavity and points of inflection, 5) Find asymptotes, 6) Find intercepts and important points, 7) Combine evidence to graph the function. Key tests are outlined for max/min, concavity, and points of inflection using the first and second derivatives.
The document discusses inverse functions. An inverse function reverses the input and output of a function. For a function f(x) to have an inverse function f-1(y), it must be one-to-one, meaning that different inputs produce different outputs. The inverse of a function f(x) is found by solving the original function equation for x in terms of y. Examples show finding the inverse of specific functions like f(x) = x - 5 by solving for x. A function is one-to-one if for any two different inputs u and v, their outputs f(u) and f(v) are also different.
The document discusses surface integrals. It defines a surface integral as integrating a density function w over a surface σ. The surface σ is defined by a function z=f(x,y) over a domain D. The surface is partitioned into small patches, and each patch's area is approximated. The total mass of the surface is calculated as the limit of Riemann sums as the partitions approach zero. An example calculates the mass of a density function over a spherical surface portion.
- A differential equation involves an independent variable, dependent variable, and derivatives of the dependent variable with respect to the independent variable.
- The order of a differential equation is the order of the highest derivative, and the degree is the exponent of the highest order derivative.
- Linear differential equations involve the dependent variable and its derivatives only to the first power. Non-linear equations do not meet this criterion.
- The general solution of a differential equation contains as many arbitrary constants as the order of the equation. A particular solution results from assigning values to the arbitrary constants.
- Differential equations can be solved through methods like variable separation, inspection of reducible forms, and finding homogeneous or linear representations.
Este documento describe los conceptos fundamentales de la integración o antiderivación. Explica que una función F es una primitiva de f si su derivada es f, y que cualquier función de la forma F(x)+C también es una primitiva de f. Además, introduce las nociones de integral indefinida, integral definida, y el Teorema Fundamental del Cálculo.
The document provides an overview of the Mean Value Theorem and Rolle's Theorem. It discusses that the Mean Value Theorem states that for any function continuous on a closed interval, there exists a point where the slope of the tangent line equals the slope of the secant line through the endpoints. Rolle's Theorem is a special case where if a function is continuous on a closed interval and differentiable on the open interval, if the function is equal at the endpoints, the derivative at some interior point is zero. Graphical interpretations are also provided to illustrate these theorems.
Functions and its Applications in MathematicsAmit Amola
A function is a relation between a set of inputs and set of outputs where each input is related to exactly one output. An example is given of a function that relates shapes to colors, where each shape maps to one unique color. A function can be written as a set of ordered pairs, where the input comes first and the output second. The domain is the set of inputs, the codomain is the set of possible outputs, and the range is the set of outputs the function actually produces. A function is one-to-one if no two distinct inputs map to the same output, and onto if every element in the codomain is mapped to by at least one input.
This document is a calculus supplement to accompany a microeconomics textbook. It introduces the concept of partial derivatives and shows how they can be used to analyze economic concepts from the textbook like demand and supply functions, substitutes and complements, and elasticities. Partial derivatives allow the slope of demand and supply functions to be determined with respect to different variables. They also allow elasticities to be defined and calculated using calculus, providing an equivalent but alternative method to the algebraic approach in the textbook. The supplement aims to illustrate the connections between calculus and microeconomic concepts.
This document provides an outline for a calculus lecture on basic differentiation rules. It includes objectives to understand the derivative of constants, the constant multiple rule, the sum rule, the difference rule, and derivatives of sine and cosine. Examples are provided to find the derivatives of squaring, cubing, square root, and cube root functions using the definition of the derivative. Graphs and properties of these functions and their derivatives are also discussed.
This document provides an outline for a calculus lecture on basic differentiation rules. It includes objectives to understand key rules like the constant multiple rule, sum rule, and derivatives of sine and cosine. Examples are worked through to find the derivatives of functions like squaring, cubing, square root, and cube root using the definition of the derivative. Graphs and properties of derived functions are also discussed.
The document summarizes the Fundamental Theorem of Calculus, which establishes a connection between computing integrals (areas under curves) and computing derivatives. It shows that if f is continuous on an interval [a,b] and F is defined by integrating f, then F' = f. Graphs and examples are provided to justify this theorem geometrically and demonstrate its applications to computing derivatives and integrals.
This document contains a chapter on topics in vector calculus, including exercises on vector fields, divergence, curl, and applications of vector calculus identities and theorems. The exercises involve calculating divergence and curl of various vector fields, applying vector calculus operations like divergence and curl to scalar and vector functions, and manipulating vector calculus identities.
This document discusses theta functions with spherical coefficients and their behavior under transformations of the modular group. It begins by defining spherical polynomials and proving that a polynomial is spherical of degree r if and only if it is a linear combination of terms of the form (ξ·x)r, where ξ has zero norm if r is greater than or equal to 2. It then defines theta functions associated with a lattice Γ, a point z, and a spherical polynomial P. The behavior of these theta functions under substitutions of the modular group is studied by applying the Poisson summation formula. A table of relevant Fourier transforms is also provided.
The document discusses partial derivatives of functions with multiple variables. It defines a partial derivative as the ordinary derivative of a function with respect to one variable, while holding all other variables constant. Partial derivatives measure the rate of change of a function along coordinate axes. The document provides examples of calculating partial derivatives and discusses their geometric interpretation in terms of tangent lines and planes.
The basic rules of differentiation, including the power rule, the sum rule, the constant multiple rule, and the rule for differentiating sine and cosine.
1. The document discusses Fisher information and α-divergence for statistical models.
2. It defines the Fisher information matrix using second derivatives of the log-likelihood function and the α-divergence using first and second derivatives.
3. Examples of common statistical distributions are provided and it is shown how the Fisher information and α-divergence can be calculated for these models.
1) A quadratic function is an equation of the form f(x) = ax^2 + bx + c, where a ≠ 0. Its graph is a parabola.
2) The vertex of a parabola is the point where it intersects its axis of symmetry. If a > 0, the parabola opens upward and the vertex is a minimum. If a < 0, it opens downward and the vertex is a maximum.
3) The standard form of a quadratic equation is f(x) = a(x - h)^2 + k, where the vertex is (h, k) and the axis of symmetry is x = h.
This document discusses quantum modes and the correspondence between classical and quantum mechanics. It provides three key principles of quantum mechanics: (1) quantum states are represented by ket vectors, (2) quantum observables are hermitian operators, and (3) the Schrodinger equation governs the causal evolution of quantum systems. It also outlines how classical quantities like position and momentum correspond to quantum operators and how they form Lie algebras through commutation relations. Representations of quantum mechanics are discussed through examples like the energy basis of the harmonic oscillator.
The document discusses complex differentiability and analytic functions. It shows that for a function f(z) to be complex differentiable, the Cauchy-Riemann equations relating the partial derivatives of the real and imaginary parts must be satisfied. It also discusses representing functions as power series and their radii of convergence. Multivalued functions like logarithms and roots are discussed, noting the need for branch cuts to define single-valued branches.
This document discusses differentiable and analytic functions of a complex variable z. It defines the derivative of a complex function f(z) and shows that for f(z) to be differentiable, the Cauchy-Riemann equations relating the partial derivatives of the real and imaginary parts must be satisfied. Examples are provided to illustrate calculating derivatives and determining differentiability. The document also covers power series representations of functions, elementary functions like exponential and logarithmic functions, and the concepts of branch points and cuts for multi-valued complex functions.
This document discusses differentiation and defines the derivative. It begins by formally defining the derivative as a limit and then provides formulas to find the derivatives of simple functions like constants, linear functions, and power functions. It also covers numerical derivatives, implicit differentiation, and higher-order derivatives. Examples are provided to illustrate each concept.
[Vvedensky d.] group_theory,_problems_and_solution(book_fi.org)Dabe Milli
1) The document discusses problems related to group theory.
2) Problem 1 shows that the wave equation for light propagation is invariant under Lorentz transformations.
3) Problem 2 shows that the Schrodinger equation is invariant under a global phase change of the wavefunction, and uses Noether's theorem to show the conservation of probability.
The document is a math worksheet containing calculus problems involving functions. It includes 21 problems involving operations on functions such as composition, inversion and transformations of function graphs. The problems involve determining expressions for composed functions, inverses, graphs of related functions obtained through transformations of an original function graph. The document also provides answers to the problems.
This document provides an overview of subdifferentials and proximal operators for convex analysis. It defines subgradients and subdifferentials, and explains their relation to gradients of convex functions. It covers properties like monotonicity, maximal monotonicity, and strong monotonicity. It also discusses calculus rules for subdifferentials of sums and compositions. Finally, it introduces proximal operators and explains that evaluating a proximal operator is equivalent to computing an element of the subdifferential.
After defining the limit and calculating a few, we introduced the limit laws. Today we do the same for the derivative. We calculate a few and introduce laws which allow us to computer more. The Power Rule shows us how to compute derivatives of polynomials, and we can also find directly the derivative of sine and cosine.
This document discusses limits of functions. It begins by defining the limit of a function f(x) as x approaches a number c as the value that f(x) approaches as x gets closer to c. It provides examples of limits, including one-sided limits and limits at infinity. Key theorems are presented for computing limits, including properties of limits and the sandwich theorem. The document focuses on conceptual understanding and applying techniques to evaluate a variety of limit examples.
After defining the limit and calculating a few, we introduced the limit laws. Today we do the same for the derivative. We calculate a few and introduce laws which allow us to computer more. The Power Rule shows us how to compute derivatives of polynomials, and we can also find directly the derivative of sine and cosine.
Similar to Chapter 5(partial differentiation) (20)
1. BMM 104: ENGINEERING MATHEMATICS I Page 1 of 8
CHAPTER 5: PARTIAL DERIVATIVES
Functions of n Independent Variables
Suppose D is a set of n-tuples of real numbers ( x1 , x 2 ,..., x n ) . A real valued function f
on D is a rule that assigns a unique (single) real number
w = f ( x1 , x 2 ,..., x n )
to each element in D. The set D is the function’s domain. The set of w-values taken on
by f is the function’s range. The symbol w is the dependent variable of f, and f is said to
be a function of the n independent variables x1 to x n . We also call the x j ' s the
function’s input variables and call w the function’s output variable.
Level Curve, Graph, surface of Functions of Two Variables
The set of points in the plane where a function f ( x , y ) has a constant value f ( x , y ) = c
is called a level curve of f. The set of all points ( x , y , f ( x , y ) ) in space, for ( x , y ) in
the domain of f, is called the graph of f. The graph of f is also called the surface
z = f ( x , y) .
Functions of Three Variables
The set of points ( x , y , z ) in space where a function of three independent variables has a
constant value f ( x , y , z ) = c is called a level surface of f.
Example: Attend lecture.
Partial Derivatives of a Function of Two Variables
Definition: Partial Derivative with Respect to x
The partial derivative of f ( x , y ) with respect to x at the point ( x0 , y 0 ) is
∂f f ( x0 + h , y 0 ) − f ( x0 , y 0 )
= lim ,
∂x ( x0 , y0 )
h→0 h
provided the limit exists.
Definition: Partial Derivative with Respect to y
2. BMM 104: ENGINEERING MATHEMATICS I Page 2 of 8
The partial derivative of f ( x , y ) with respect to y at the point ( x0 , y0 ) is
∂f d f ( x0 , y 0 + h ) − f ( x0 , y 0 )
= f ( x0 , y ) = lim ,
∂y ( x0 , y0 ) dy y = y0 h→0 h
provided the limit exists.
Example:
∂f ∂f
1. Find the values of and ∂ at the point ( 4 ,− ) if
5
∂x y
f ( x , y ) = x 2 + 3 xy + y − 1 .
∂ f
2. Find if f ( x , y ) = y sin xy .
∂ x
2y
3. Find f x and f y if f ( x , y ) = y + cos x .
Functions of More Than Two Variables
Example:
∂f ∂f ∂f
1. Let f ( x , y , z ) = xy 2 z 3 . Find , ∂ and at (1,− ,− ) .
2 1
∂x y ∂z
y
2. Let g ( x , y , z ) = x 2 e z . Find g x , g y and g z .
Second-Order Partial Derivatives
When we differentiate a function f ( x , y ) twice, we produce its second-order
derivatives.
These derivatives are usually denoted by
∂2 f f xx
“ d squared fdx squared “ or “f sub xx “
∂x 2
∂2 f
“ d squared fdy squared “ or f yy “f sub yy “
∂ 2
y
∂2 f f xx
“ d squared fdx squared “ or “f sub xx “
∂x 2
∂ f
2
“ d squared fdxdy squared “ or f yx “f sub yx “
∂∂
x y
3. BMM 104: ENGINEERING MATHEMATICS I Page 3 of 8
∂ f
2
“ d squared fdydx squared “ or f xy “f sub xy “
∂∂
y x
The defining equations are
∂2 f ∂ ∂f ∂2 f ∂ ∂
f
= , =
∂
∂x 2
∂x ∂x ∂∂
x y ∂ y
x
and so on. Notice the order in which the derivatives are taken:
∂ f
2
Differentiate first with respect to y, then with respect to x.
∂∂
x y
f yx = ( f y ) x Means the same thing.
Example:
∂2 f ∂ f
2
∂ f ∂ f
2 2
1. Let f ( x , y ) = x 3 y 2 − x 4 y 6 . Find , , and .
∂x 2 ∂ ∂ ∂
y x y2 ∂∂x y
∂2 f ∂ f
2
∂2 f ∂ f
2
2. If f ( x , y ) = x cos y + ye x , find , , and .
∂x 2 ∂ ∂ ∂
y x y2 ∂∂x y
The Chain Rule
Chain Rule for Functions of Two Independent Variables
If w = f ( x , y ) has continuous partial derivatives f x and f y and if x = x( t ) , y = y ( t )
are
differentiable functions of t, then the compose w = f ( x( t ) , y ( t ) ) is a differentiable
function of t and
df
= f x ( x ( t ) , y ( t ) ) • x ' ( t ) + f y ( x( t ) , y ( t ) ) • y ' ( t ) ,
dt
or
dw ∂f dx ∂f dy
= + .
dt ∂x dt ∂y dt
Example:
Use the chain rule to find the derivative of w = xy , with respect to t along the path
4. BMM 104: ENGINEERING MATHEMATICS I Page 4 of 8
π
x = cos t , y = sin t . What is the derivative’s value at t = ?
2
Chain Rule for Functions of Three Independent Variables
If w = f ( x , y , z ) is differentiable and x, y and z are differentiable functions of t, then w
is
a differentiable function of t and
dw ∂f dx ∂f dy ∂f dz
= + + .
dt ∂x dt ∂y dt ∂z dt
Example:
dw
Find if w = xy + z , x = cos t , y = sin t , z =t.
dt
Chain Rule for Two Independent Variables and Three Intermediate Variables
Suppose that w = f ( x , y , z ) , x = g ( r , s ) , y = h( r , s ) , and z = k ( r , s ) . If all four
functions
are differentiable, then w has partial derivatives with respect to r and s, given by the
formulas
∂w ∂ ∂
w x ∂ ∂w y ∂ ∂
w z
= + +
∂r ∂ ∂
x r ∂ ∂
y r ∂ ∂
z r
∂w ∂ ∂
w x ∂ ∂w y ∂ ∂
w z
= + +
∂s ∂ ∂
x s ∂ ∂
y s ∂ ∂
z s
Example:
∂w ∂w
Express and in terms of r and s is
∂r ∂s
r
w = x +2y + z2, x = , y = r 2 + ln s , z = 2 r .
s
If w = f ( x , y ) , x = g ( r , s ) , and y = h( r , s ) , then
∂w ∂ ∂
w x ∂ ∂
w y ∂w ∂ ∂
w x ∂ ∂
w y
= + and = +
∂r ∂ ∂
x r ∂ ∂
y r ∂s ∂ ∂
x s ∂ ∂
y s
Example:
∂w ∂w
Express and in terms of r and s if
∂r ∂s
5. BMM 104: ENGINEERING MATHEMATICS I Page 5 of 8
w = x2 + y2 , x= r− s, y =r+s.
If w = f ( x ) and x = g ( r , s ) , then
∂w dw ∂x ∂w dw ∂x
= and = .
∂r dx ∂r ∂s dx ∂s
PROBLEM SET: CHAPTER 5
1. Sketch and name the surfaces
(a) f ( x, y , z ) = x 2 + y 2 + z 2 (e) f ( x, y, z ) = x 2 + y 2
(b) f ( x , y , z ) = ln( x 2 + y 2 + z 2 ) (f) f ( x, y, z ) = y 2 + z 2
(c) f ( x, y , z ) = x + z (g) f ( x, y, z ) = z − x 2 − y 2
x2 y2 z2
(d) f ( x, y, z ) = z (h) f ( x, y , z ) = + +
25 16 9
∂f ∂f
2. Find and ∂ .
∂x y
(a) f ( x , y ) = 5 xy − 7 x 2 − y 2 + 3 x − 6 y + 2
y
(b) f ( x , y ) = tan −1
x
(c) f ( x, y) = e ( x + y +1)
(d) f ( x , y ) = e −x sin( x + y )
(e) f ( x , y ) = ln( x + y )
(f) f ( x , y ) = sin 2 ( x − 3 y )
3. Find f x , f y and f z .
(a) f ( x , y , z ) = sin −1 ( xyz )
f ( x , y , z ) = e −( x )
2
+ y 2 +z 2
(b)
(c) f ( x , y , z ) = e −xyz
(d) f ( x , y , z ) = tanh( x + 2 y + 3 z )
4. Find all the second-order partial derivatives of the following functions.
(a) f ( x , y ) = x + y + xy
(b) f ( x , y ) = sin xy
(c) f ( x , y ) = x 2 y + cos y + y sin x
6. BMM 104: ENGINEERING MATHEMATICS I Page 6 of 8
(d) f ( x , y ) = xe y + y + 1
5. Verify that w xy = w yx .
(a) w = ln( 2 x + 3 y ) (c) w = xy 2 + x 2 y 3 + x 3 y 4
(b) w = e x + x ln y + y ln x (d) w = x sin y + y sin x + xy
dw
6. In the following questions, (a) express as a function of t, both by using
dt
the Chain Rule and by expressing w in terms of t and differentiating directly with
dw
respect to t. The (b) evaluate at the given value of t.
dt
(i) w = x2 + y2 , x = cos t , y = sin t ; t=π .
x y 1
(ii) w= + , x = cos 2 t , y = sin 2 t , z= t =3.
z z t
∂z ∂z
7. In the following questions, (a) express and as a functions of u and v
∂u ∂v
both by using the Chain Rule and by expressing z directly in terms of u and v
∂z ∂z
before differentiating. Then (b) evaluate and at the given point (u , v ) .
∂u ∂v
(i) z = 4 e x ln y , x = ln( u cos v ) , y = u sin v ; ( u ,v ) = 2 , π
4
(ii)
x
z = tan −1 ,
y x = u cos v , y = u sin v ; ( u ,v ) = 1.3 , π
6
ANSWERS FOR PROBLEM SET: CHAPTER 5
∂f ∂f
2. (a) = 5 y − 14 x + 3 , = 5 x − 2 y −6
∂x ∂y
∂f y ∂f x
(b) =− 2 , = 2
∂x x + y 2 ∂y x + y2
∂f ∂f
(c) = e ( x +y +1) , = e ( x +y +1 )
∂x ∂y
∂f ∂f
(d) = −e −x sin( x + y ) + e −x cos ( x + y ) , = e −x cos ( x + y )
∂x ∂y
∂f 1 ∂f 1
(e) = , =
∂x x + y ∂y x+y
∂f ∂f
(f) = 2 sin( x − 3 y ) cos( x − 3 y ) , = −6 sin( x − 3 y ) cos( x − 3 y )
∂x ∂x
7. BMM 104: ENGINEERING MATHEMATICS I Page 7 of 8
yz xz xy
3. (a) fx = , fy = , fz =
1−x y z2 2 2
1−x y z
2 2 2
1 − x2 y2 z2
f x = −2 xe −( x ) , f = −2 ye −( x f z = −2 ze − ( x + y + z )
(b)
2
+ y 2 +z 2 2
+ y 2 +z 2 ) , 2 2 2
y
(c) f x = −yze −xyz , f y = −xze −xyz , f z = −xye − xyz
(d) f x = sec h 2 ( x + 2 y + 3 z ) , f y = 2 sec h 2 ( x + 2 y + 3 z ) ,
f z = 3 sec h 2 ( x + 2 y + 3 z )
∂f ∂f ∂2 f
=1 + x , ∂ f = 0,
2
∂2 f ∂2 f
4. (a) = 1 + y, = 0, = =1
∂x ∂y ∂x 2 ∂y 2 ∂∂
y x ∂∂
x y
∂f ∂f ∂2 f
= x cos xy , ∂ f = − y 2 sin xy ,
2
(b) = y cos xy , = −x 2 sin xy ,
∂x ∂y ∂x 2 ∂y 2
∂2 f ∂2 f
= = cos xy − xy sin xy
∂y∂x ∂x∂y
∂f ∂f
= x 2 − sin y + sin x , ∂ f = 2 y − y sin x ,
2
(c) = 2 xy + y cos x ,
∂x ∂y ∂x 2
∂ f
2
∂2 f ∂2 f
= −cos y , = = 2 x + cos x
∂y 2
∂y∂x ∂x∂y
∂f ∂f ∂2 f
= xe y + 1 , ∂ f = 0 ,
2
∂2 f ∂2 f
(d) =ey = xe y , = =e y
∂x ∂y ∂x 2 ∂y 2
∂∂
y x ∂∂
x y
∂w 2 ∂w 3 ∂2 w −6
5. (a) = , = , = , and
∂x 2 x + 3 y ∂y 2 x + 3 y ∂y∂x (2x + 3 y) 2
∂2 w −6
=
∂x∂y ( 2 x + 3 y ) 2
∂w y ∂w x ∂2 w 1 1
(b) = e x + ln y + , = + ln x , = + , and
∂x x ∂y y ∂∂
y x y x
∂2w 1 1
= +
∂x∂y y x
∂w ∂w
(c) = y 2 + 2 xy 3 + 3 x 2 y 4 , = 2 xy + 3 x 2 y 2 + 4 x 3 y 3 ,
∂x ∂y
∂2 w ∂2 w
= 2 y + 6 xy 2 + 12 x 2 y 3 , and = 2 y + 6 xy 2 + 12 x 2 y 3
∂y∂x ∂x∂y
8. BMM 104: ENGINEERING MATHEMATICS I Page 8 of 8
∂w ∂w
(d) = sin y + y cos x + y , = x cos y + sin x + x ,
∂x ∂y
∂2 w ∂2 w
= cos y + cos x + 1, and = cos y + cos x + 1
∂y∂x ∂x∂y
dw
6. (i) (a) =0 (b) 0
dt
dw
(ii) (a) =1 (b) 1
dt
∂z
7. (i) (a) = ( 4 cos v ) ln( u sin v ) + 4 cos v
∂u
∂z 4u cos 2 v
= ( − 4u sin v ) ln( u sin v ) +
∂v sin v
∂z
(b) = 2 ( ln 2 + 2 )
∂u
∂z
= −2 2 ln 2 + 4 2
∂v
∂z
(ii) (a) =0
∂u
∂z
= −1
∂v
∂z
(b) =0
∂u
∂z
= −1
∂v
9. BMM 104: ENGINEERING MATHEMATICS I Page 8 of 8
∂w ∂w
(d) = sin y + y cos x + y , = x cos y + sin x + x ,
∂x ∂y
∂2 w ∂2 w
= cos y + cos x + 1, and = cos y + cos x + 1
∂y∂x ∂x∂y
dw
6. (i) (a) =0 (b) 0
dt
dw
(ii) (a) =1 (b) 1
dt
∂z
7. (i) (a) = ( 4 cos v ) ln( u sin v ) + 4 cos v
∂u
∂z 4u cos 2 v
= ( − 4u sin v ) ln( u sin v ) +
∂v sin v
∂z
(b) = 2 ( ln 2 + 2 )
∂u
∂z
= −2 2 ln 2 + 4 2
∂v
∂z
(ii) (a) =0
∂u
∂z
= −1
∂v
∂z
(b) =0
∂u
∂z
= −1
∂v
10. BMM 104: ENGINEERING MATHEMATICS I Page 8 of 8
∂w ∂w
(d) = sin y + y cos x + y , = x cos y + sin x + x ,
∂x ∂y
∂2 w ∂2 w
= cos y + cos x + 1, and = cos y + cos x + 1
∂y∂x ∂x∂y
dw
6. (i) (a) =0 (b) 0
dt
dw
(ii) (a) =1 (b) 1
dt
∂z
7. (i) (a) = ( 4 cos v ) ln( u sin v ) + 4 cos v
∂u
∂z 4u cos 2 v
= ( − 4u sin v ) ln( u sin v ) +
∂v sin v
∂z
(b) = 2 ( ln 2 + 2 )
∂u
∂z
= −2 2 ln 2 + 4 2
∂v
∂z
(ii) (a) =0
∂u
∂z
= −1
∂v
∂z
(b) =0
∂u
∂z
= −1
∂v
11. BMM 104: ENGINEERING MATHEMATICS I Page 8 of 8
∂w ∂w
(d) = sin y + y cos x + y , = x cos y + sin x + x ,
∂x ∂y
∂2 w ∂2 w
= cos y + cos x + 1, and = cos y + cos x + 1
∂y∂x ∂x∂y
dw
6. (i) (a) =0 (b) 0
dt
dw
(ii) (a) =1 (b) 1
dt
∂z
7. (i) (a) = ( 4 cos v ) ln( u sin v ) + 4 cos v
∂u
∂z 4u cos 2 v
= ( − 4u sin v ) ln( u sin v ) +
∂v sin v
∂z
(b) = 2 ( ln 2 + 2 )
∂u
∂z
= −2 2 ln 2 + 4 2
∂v
∂z
(ii) (a) =0
∂u
∂z
= −1
∂v
∂z
(b) =0
∂u
∂z
= −1
∂v