《化工应用数学》PPT课件.ppt
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1、化工應用數學授課教師:郭修伯Lecture 6Functions and definite integralsVectorsChapter 5Functions and definite integralsThere are many functions arising in engineering which cannot be integrated analytically in terms of elementary functions.The valuesof many integrals have been tabulated,much numerical work can beav
2、oided if the integral to be evaluated can be altered to a form that is tabulated.Ref.pp.153We are going to study some of these special functions.Special functionsFunctionsDetermine a functional relationship between two or more variablesWe have studied many elementary functions such as polynomials,po
3、wers,logarithms,exponentials,trigonometric and hyperbolic functions.Four kinds of Bessel functions are useful for expressing the solutions of a particular class of differential equations.Legendre polynomials are solutions of a group of differential equations.Learn some more now.The error functionIt
4、occurs in the theory of probability,distribution of residence times,conduction of heat,and diffusion matter:0 xzerf xz:dummy variableProof in next slidex and y are two independent Cartesian coordinatesin polar coordinatesError between the volume determined by x-y and r-The volume of has a base area
5、which isless than 1/2R2 and a maximum height of e-R2 More about error functionDifferentiation of the error function:Integration of the error function:The above equation is tabulated under the symbol“ierf x”with(Therefore,ierf 0=0)Another related function is the complementary error function“erfc x”Th
6、e gamma functionfor positive values of n.t is a dummy variable since the value of the definite integral is independent of t.(N.B.,if n is zero or a negative integer,the gamma function becomes infinite.)repeatThe gamma function is thus a generalized factorial,for positive integervalues of n,the gamma
7、 function can be replaced by a factorial.(Fig.5.3 pp.147)More about the gamma functionEvaluateChapter 7Vector analysisIt has been shown that a complex number consisted of a real part andan imaginary part.One symbol was used to represent a combinationof two other symbols.It is much quicker to manipul
8、ate a single symbolthan the corresponding elementary operations on the separate variables.This is the original idea of vector.Any number of variables can be grouped into a single symbol in two ways:(1)Matrices(2)TensorsThe principal difference between tensors and matrices is the labelling andorderin
9、g of the many distinct parts.TensorsGeneralized as zmA tensor of first rank since one suffix m is needed to specify it.The notation of a tensor can be further generalized by using more thanone subscript,thus zmn is a tensor of second rank(i.e.m,n).The symbolism for the general tensor consists of a m
10、ain symbol suchas z with any number of associated indices.Each index is allowed totake any integer value up to the chosen dimensions of the system.Thenumber of indices associated with the tensor is the“rank”of the tensor.Tensors of zero rank(a tensor has no index)It consists of one quantity independ
11、ent of the number of dimensions of the system.The value of this quantity is independent of the complexity of the system and it possesses magnitude and is called a“scalar”.Examples:energy,time,density,mass,specific heat,thermal conductivity,etc.scalar point:temperature,concentration and pressure whic
12、h are all signed by a number which may vary with position but not depend upon direction.Tensors of first rank(a tensor has a single index)The tensor of first rank is alternatively names a“vector”.It consists of as many elements as the number of dimensions of the system.For practical purposes,this nu
13、mber is three and the tensor has three elements are normally called components.Vectors have both magnitude and direction.Examples:force,velocity,momentum,angular velocity,etc.Tensors of second rank(a tensor has two indices)It has a magnitude and two directions associated with it.The one tensor of se
14、cond rank which occurs frequently in engineering is the stress tensor.In three dimensions,the stress tensor consists of nine quantities which can be arranged in a matrix form:The physical interpretation of the stress tensorxzypxxxyxzThe first subscript denotes the plane and the second subscript deno
15、tes the direction of the force.xy is read as“the shear force on the x facing plane acting in the y direction”.Geometrical applicationsIf A and B are two position vectors,find the equation of the straightline passing through the end points of A and B.ABCApplication of vector method for stagewise proc
16、essesIn any stagewise process,there is more than one property to be conserved and for the purpose of this example,it will be assumed that the three properties,enthalpy(H),total mass flow(M)and mass flow of one component(C)are conserved.In stead of considering three separate scalar balances,one vecto
17、r balance can be takenby using a set of cartesian coordinates in the following manner:Using x to measure M,y to measure H and z to measure CAny process stream can be represented by a vector:MHCA second stream can be represented by:Using vector addition,Thus,OR with represents of the sum of the two s
18、treams must be a constantvector for the three properties to be conserved within the system.To perform a calculation,when either of the streams OM or ON is determined,the other is obtained by subtraction from the constant OR.Example:when x=1,Ponchon-Savarit method(enthalpy-concentration diagram)xyzMR
19、NBAPThe constant line OR cross the plane x=1 at point POpoint A is:point B is:point P is:Multiplication of vectorsTwo different interactions(whats the difference?)Scalar or dot product:the calculation giving the work done by a force during a displacementwork and hence energy are scalar quantities wh
20、ich arise from the multiplication of two vectorsif AB=0The vector A is zeroThe vector B is zero=90ABVector or cross product:n is the unit vector along the normal to the plane containing A and B and its positive direction is determined as the right-hand screw rulethe magnitude of the vector product o
21、f A and B is equal to the area of the parallelogram formed by A and Bif there is a force F acting at a point P with position vector r relative to an origin O,the moment of a force F about O is defined by:if A B=0The vector A is zeroThe vector B is zero=0ABCommutative law:Distribution law:Associative
22、 law:Unit vector relationshipsIt is frequently useful to resolve vectors into components along the axial directions in terms of the unit vectors i,j,and k.Scalar triple productThe magnitude of is the volume of the parallelepiped with edges parallel to A,B,and C.ABCABVector triple productThe vector i
23、s perpendicular to the plane of A and B.When the further vectorproduct with C is taken,the resulting vector must be perpendicular to and hence in the plane of A and B:ABCABwhere m and n are scalar constants to be determined.Since this equation is validfor any vectors A,B,and CLet A=i,B=C=j:Different
24、iation of vectorsIf a vector r is a function of a scalar variable t,then when t varies by anincrement t,r will vary by an increment r.r is a variable associated with r but it needs not have either thesame magnitude of direction as r:As t varies,the end point of the position vector r will trace out a
25、 curve in space.Taking s as a variable measuring length along this curve,the differentiation processcan be performed with respect to s thus:is a unit vector in the direction of the tangent to the curveis perpendicular to the tangent .The direction of is the normal to the curve,and the two vectors de
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