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ContentTheory of Equation
Theory of EquationElimination582Solution of π Linear Equations in π VariablesThe equations and the values of the variables are arranged below: π1π₯1+π2π₯2+β―+πππ₯π=π1 π1π₯1+π2π₯2+β―+πππ₯π=π2 β― π1π₯1+π2π₯2+β―+πππ₯π=ππ and π₯1β=π΄1π1+π΅1π2+β―+πΏ1ππ π₯2β=π΄2π1+π΅2π2+β―+πΏ2ππ β― π₯πβ=π΄ππ1+π΅ππ2+β―+πΏπππ where β is the determinant annexed, and π΄1, π΅1, β―, are its first minors.π1β―ππβ―π1β―ππTo find the value of one of the unknowns π₯π. RuleMultiply the equations respectively by the minors of the πth column, and add the results. π₯π will be equal to the fraction whose numerator is the determinant β, with its πth column replaced by π1, π2, β―, ππ, and whose denominator is β itself. 582 If π1, π2, β―, ππ, and β all vanish, then π₯1, π₯2, β―, π₯π are in the ratios of the minors of any row of the determinant β. For example, in the ratios πΆ1:πΆ2:πΆ3: β―:πΆπ.The eliminant of the given equations is now β=0. 584 Orthogonal TransformationIf the two sets of variables in the π equations (582) be connected by the relation π₯1+π₯22+β―+π₯ 2π=π1+π 22+β―+π 2π1 then the changing from one set of variables to the other, by substituting the values of the π's in terms of the π₯'s in any function of th former, or vice verssa, is called orthogonal transformation. When equation [1] is satisified, two results follow. I. The determinant β=Β±1. II. Each of the constituents of β is equal to the corresponding minor, or else to minus that minor according as β is positiive or negative ProofSubstitute the values of π1, π2, β―, ππ in terms of π₯1, π₯2, β―, π₯π in equation [1], and equate coefficients of the squares and products of the new variables. We get the π2 equationsπ } π2π1+π2π1+=0π } π3π1+π3π1+=0π3π2+π3π2+=0π }Also β= π1π1β―π1π2π2β―π2π3π3β―π3β―β―β―β―ππππβ―ππFrom the square of the determinant β by the rule (570), and these equations show that the product is a determinant in which the only constituents that do not vanish constitute a diagonal of 'ones'. Therefore β2=1 and β=Β±1 Again, solving the first set of equations for π1 (writing π { π1β=π΄1+π΄20+π΄30+=π΄1π2β=π΄10+π΄2+π΄30+=π΄2π3β=π΄10+π΄20+π΄3+=π΄3β―585 TheoremThe πβ2th power of a determinant of the πth order multiplied by any constituent is equal to the corresponding minor of the reciprocal determinant.ProofLet π be the reciprocal determinant of β, and π½π the minor of π΅π in π. Write the transformed equations (582) for the π₯'s in terms of the π's, and solve them for π2. Then equate the coefficient of π₯π in the result with its coefficient in the original value of π2.Thus ππ2=β(π½1π₯1+β―+π½ππ₯π+β―), and π2=π1π₯1+β―+πππ₯π+β―; β΄ βπ½π=πππ=βπβ1ππ by (575); β΄ π½π=βπβ2ππ 586 To eliminate π₯ from the two equations ππ₯π+ππ₯πβ1+ππ₯πβ2+β―=01 πβ²π₯π+πβ²π₯πβ1+πβ²π₯πβ2+β―=02 If it is desired that the equation should be homogeneous in π₯ and π¦; put π₯π¦instead of π₯, and clear of fractions. The following methods will still be applicable. I. Bezout's MethodSuppose π>πRule: Bring the equations to the same degree by multiplying [2] by π₯πβπ. Then multiply [1] by πβ², and [2] by π, and subtract. Again, multiply [1] by πβ²π₯+πβ², and [2] by (ππ₯+π), and subtract. Again, multiply [1] by πβ²π₯2+πβ²π₯+πβ², and [2] by (ππ₯2+ππ₯+π), and subtract, and so on until π equations have been obtained. Each will be of the degree πβ1. Write under these the πβπ equations obtained by multiplying [2] successively by π₯. The eliminant of the π equations is the result required. ExampleLet the equations be{ ππ₯5+ππ₯4+ππ₯3+ππ₯2+ππ₯+π=0πβ²π₯3+πβ²π₯2+πβ²π₯+πβ²=0The five equations obtained by the method, and their eliminant, by (583), are, writing capital letters for the functions of π, π, π, π, π, π, π΄1π₯4+π΅1π₯3+πΆ1π₯2+π·1π₯+πΈ1=0π΄2π₯4+π΅2π₯3+πΆ2π₯2+π·2π₯+πΈ2=0π΄3π₯4+π΅3π₯3+πΆ3π₯2+π·3π₯+πΈ3=0πβ²π₯4+πβ²π₯3+πβ²π₯2+πβ²π₯ =0 πβ²π₯3+πβ²π₯2+πβ²π₯+πβ²=0 }and π΄1π΅1πΆ1π·1πΈ1π΄2π΅2πΆ2π·2πΈ2π΄3π΅3πΆ3π·3πΈ3πβ²πβ²πβ²πβ²00πβ²πβ²πβ²πβ²=0 Should the equations be of the same degree, the eliminant will be a symmetrical determinant. 587 II. Sylvester's Dialytic MethodRule: Multiply equation [1] successively by π₯, πβ1 times; and equation [2] πβ1 times; and eliminate π₯ from the π+π resulting equations.ExampleTo eliminate π₯ fromππ₯3+ππ₯2+ππ₯+π=0ππ₯2+ππ₯+π=0 }The π+π equations and their eliminant are ππ₯2+ππ₯+π=0 ππ₯3+ππ₯2+ππ₯ =0ππ₯4+ππ₯3+ππ₯2 =0 ππ₯3+ππ₯2+ππ₯+π=0ππ₯4+ππ₯3+ππ₯2+ππ₯ =0 }and 00πππ0πππ0πππ000ππππππππ0=0 588 III. Method of elimination by Symmetrical FunctionsDivide the two equations in (586) respectively by the coefficients of their first terms, thus reducing them to the forms π(π₯)β‘π₯π+π1π₯πβ1+β―+ππ=0 π(π₯)β‘π₯π+π1π₯πβ1+β―+ππ=0RuleLet π, π, π, β―, represent the roots of π(π₯). Form the equation π(π)π(π)π(π)β―=0. This will contain symmetrical functions only of the roots π, π, π, β―.Express these functions in terms of π1, π2, β― by (538), β―, and the equation becomes the eliminant. Reason of the rule: The eliminant is the condition for a common root of the two equations. That root must make one of the factors π(π), π(π), β―, vanish, and therefore it makes their product vanish. 589 The eliminant expressed in terms of the roots π, π, π, β―, of π(π₯), and the roots πΌ, π½, πΎ, β―, of π(π₯), will be (πβπΌ)(πβπ½)(πβπΎ)β―(πβπΌ)(πβπ½)(πβπΎ)β― β― being the product of all possible differences between a root of one equation and a root of another. 590 The eliminant is a homogeneous function of the coefficients of either equation, beign of the πth degree in the coefficients of π(π₯), and of the πth degree in the coefficients of π(π₯). 591 The sum of the suffixes of π and π in each term of the eliminant = ππ. Also, if π, π contain π§; if π2, π2 contain π§2; if π3, π3 contain π§3; and so on, the eliminant will contain π§ππ. Proved by the fact that ππ is a homogeneous function of π dimensions of the roots π, π, π, β―, by (406). 592 If the two equations involve π₯ and π¦, the elimination may be conducted with respect to π₯; and π¦ will be contained in the coefficients π1, π2, β―, π1, π2, β―. 593 Elimination by the Method of Highest Common FactorLet two algebraical equations in π₯ and π¦ be represented by π΄=0 and π΅=0.It is required to eliminate π₯. Arrange π΄ and π΅ according to descending powers of π₯, and, having rejected any factor which is a function of π¦ only, proceed to find the Highest Common Factor of π΄ and π΅. The process may be exhibited as follows: π1π΄=π1π΅+π1π 1 π2π΅=π2π 1+π2π 2 π3π 1=π3π 2+π3π 3 π4π 2=π4π 3+π4 }π1, π2, π3, π4 are the mulipliers required at each stage in order to avoid fractional quotients; and these must be constants or functions of π¦ only. π1, π2, π3, π4 are the successive quotients. π1π 1, π2π 2, π3π 3, π4 are the successive remainders; π1, π2, π3, π4 being functions of π¦ only. The process terminates as soon as a remainder is obtained which is a function of π¦ only; π4 is here supposed to be such a remainder. Now, the simplest factors having been taken for π1, π2, π3, π4, we see that 1 is the H.C.F> of π1 and π1 π2 is the H.C.F> of π1 and π2 π3 is the H.C.F> of }The values of π₯ and π¦, which satisfy simultaneously the equations π΄=0 and π΅=0, are those obtained by the four pairs of simultaneous equations following: π1=0 and π΅=01 }The final equation in π¦, which gives all admissible values, is π1π2π3π4π2π3π4=0, If it should happen that the remainder π4 is zero, the simultaneous equations [1], [2], [3], and [4] reduce to π1=0, and π΅π 3=0; π2π2=0, and π 1π 3=0; π3π3=0, and π 2π 3=0; 594 To find infinite values of π₯ or π¦ which satisfy the given equations. Put π₯= 1π§. Clear of fractions, and make π§=0. If the two resulting equations in π¦ have any common roots, such roots, together with π₯=β, satisfy simultaneously the equations proposed. similarly we may put π¦= 1π§. Sources and Referenceshttps://archive.org/details/synopsis-of-elementary-results-in-pure-and-applied-mathematics-pdfdriveΒ©sideway ID: 210800025 Last Updated: 8/25/2021 Revision: 0 Ref: References
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