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Linear equations, simultaneous, matrix solution

The matrix solution for the parameters of the simultaneous linear equations is stated here without proof ... [Pg.74]

The matrix approach to the solution of a set of simultaneous linear equations is entirely general. Requirements for a solution are that there be a number of equations exactly equal to the number of parameters to be calculated and that the determinant... [Pg.74]

The matrix approach to the solution of a set of simultaneous linear equations is entirely general. Requirements for a solution are that there be a number of equations exactly equal to the number of parameters to be calculated and that the determinant D of the X matrix be nonzero. This latter requirement can be seen from Equations 5.14 and 5.15. Elements a and c of the X matrix associated with the present model are both equal to unity (see Equations 5.10 and 5.7) thus, with this model, the condition for a nonzero determinant (see Equation 5.12) is that element b (xu) not equal element d (x12). When the experimental design consists of two experiments carried out at different levels of the factor xt (xn = x12 see Figure 5.1), the condition is satisfied. [Pg.68]

To make the most efficient use of computer storage, and to give a quick response time, the efficient sparse matrix solution algorithm developed by D. J. Gunn (1977) (1982) is used in program MM3, but any suitable procedure for the solution of linear simultaneous equations can be used. [Pg.186]

A set of simultaneous linear equations can also be solved by using matrices, as shown in Chapter 9. The solution matrix is obtained by multiplying the matrix of constants by the inverse of the matrix of coefficients. Applying this simple solution to the spectrophotometric data used above, the inverted matrix is obtained by selecting a 3R x 3C array of cells, entering the array formula... [Pg.343]

One of the uses of matrix inversion is in the solution of systems of simultaneous linear equations... [Pg.513]

The procedure outlined above for a 2 x 2 matrix may be extended to m X m matrices. This involves the solution of m simultaneous linear equations in m unknowns,... [Pg.520]

Numerical methods include those based on finite difference calculus. They are ideally suited for tabulated experimental data such as one finds in thermodynamic tables. They also include methods of solving simultaneous linear equations, curve fitting, numerical solution of ordinary and partial differential equations and matrix operations. In this appendix, numerical interpolation, integration, and differentiation are considered. Information about the other topics is available in monographs by Hornbeck [2] and Lanczos [3]. [Pg.608]

In the previous chapter we saw how determinants are used to tackle problems involving the solution of systems of linear equations. In general, the branch of mathematics which deals with linear systems is known as linear algebra, in which matrices and vectors play a dominant role. In this chapter we shall explore how matrices and matrix algebra are used to address problems involving coordinate transformations, as well as revisiting the solution of sets of simultaneous linear equations. Vectors are explored in Chapter 5. [Pg.55]

Simultaneous linear equations occur in various engineering problems. The reader knows that a given system of linear equations can be solved by Cramer s rule or by the matrix method. However, these methods become tedious for large systems. However, there exist other numerical methods of solution which are well suited for computing machines. The following is an example. [Pg.612]

As the based point is varied across the spatial domain, a set of simultaneous linear equations is generated which may be represented in diagonal band matrix form. However, at the base points (z, 1) and i,N), it is difficult to write the analogs since they require points outside the solution domain, that is, at (z,0), (i-l-1,0), i,N+ ), and (i-l-1, N+ ). This problem is handled by writing the analogs using the fictitious points, and then the points outside the spatial domain are eliminated via use of the boundary conditions. In this way, the boundary conditions are incorporated in the solution. [Pg.387]

Therefore, a set of 2N simultaneous linear equations is obtained in 2N unknowns, and solution consists of inverting the coefficient matrix. [Pg.389]

The degree of the least polynomial of a square matr ix A, and henee its rank, is the number of linearly independent rows in A. A linearly independent row of A is a row that eannot be obtained from any other row in A by multiplieation by a number. If matrix A has, as its elements, the eoeffieients of a set of simultaneous nonhomo-geneous equations, the rank k is the number of independent equations. If A = , there are the same number of independent equations as unknowns A has an inverse and a unique solution set exists. If k < n, the number of independent equations is less than the number of unknowns A does not have an inverse and no unique solution set exists. The matrix A is square, henee k > n is not possible. [Pg.38]

Systems of reversible first-order reactions lead to sets of simultaneous linear differential equations with constant coefficients. A solution may be obtained by means of a matrix formulation that is widely used in quantum mechanics and vibrational... [Pg.90]

The corrected parameters are used to calculate a new A matrix and F vector, new corrections are calculated and the process is repeated until the calculated corrections are essentially zero. As will be shown later, a total of four parameters must be specified in order to determine a unique solution for the E and C numbers, because we are not dealing with linear simultaneous equations. The following parameters were held fixed and not allowed to vary iodine Ea = 1.00 iodine Ca = 1.00 DMA Eb = T32 diethyl sulfide Cb=7.40. These latter two parameters where selected to yield a solution close to the earlier one 39). [Pg.92]

The energies of the (/-orbitals for the system , , i = 1-5, are then obtained by diagonalization of the real symmetrical matrix Zfy, i = dzi...dy2. The real (/-orbital linear combinations which correspond to these energies are then obtained by substituting the solutions, into the sets of simultaneous equations derived from the secular determinant. [Pg.275]


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