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ContentTheory of Equation
Theory of EquationIncommensurable Roots506 Sturm's Theorem: If π(π₯), freed from equal roots, be divided by π'(π₯), and the last divisor by the last remainder, changing the sign of each remainder before dividing by it, until a remainder independent of π₯ is obtained, or else a remainder which cannot change its sign; then π(π₯), π'(π₯), and the successive remainders constitute Sturm's functions, and are denoted by π(π₯), π1(π₯), π2(π₯), β―, ππ(π₯) The operation may be exhibited as follows:π(π₯)=π1π1(π₯)βπ2(π₯)
π1(π₯)=π2π2(π₯)βπ3(π₯)
π2(π₯)=π3π3(π₯)βπ4(π₯)
β―
ππβ2(π₯)=ππβ1ππβ1(π₯)βππ(π₯)
507
Note: Any constant factor of a remainder may be rejected, and the quotient may be set down for the corresponding function.
508
An inspection of the foregoing equations shews:
For, before π(π₯) takes the value zero, π(π₯) and π1(π₯) have contrary signs, and afterwards they have the same sign; as may be shewn by making β small, and changing its sign in the expansion of π(π₯+β), by (426). 510 If any other of Sturm's functions vanishes, there is neither loss nor gain in the number of changes of sign. This will appear on inspecting the equations. 511 Result. The number of roots of π(π₯) between π and π is equal to the difference in the number of changes of sign in Sturm;s functions, when π₯=π and when π₯=π. 512 Cor. The total number of roots of π(π₯) will be found by taking π=+β and π=ββ; the sign of each function will then be the same as that of its first term. 513 When the number of functions exceed the degree of π(π₯) by unity, the two following theorems hold: If the first terms in all the functions, after the first, are positive; all the roots of π(π₯) are real. 514 If the first terms are not all positive; then, for every change of sign, there will be a pair of imaginary roots. For the proof put π=+β and π=ββ, and examine the number of changes of sign in each case, applying Descartes' rule 416 515 If π(π₯) has no factor in common with π(π₯), and if π(π₯) and π'(π₯) take the same sigtn when π(π₯)=0; then the rest of Sturm's functions may be found from π(π₯) and π(π₯), instead of π'(π₯). For the reasoning in (509) and (510) will apply to the new functions. 516 If Sturm's functions be formed without first removing equal roots from π(π₯), the theorem will still give the number of distinct roots, without repetitions, between assigned limits. For if π(π₯) and π1(π₯) be divided by their highest common factor (see 444), and if the quotients be used instead of π(π₯) and π1(π₯) to form Sturm's functions; then, by (515), the theorem will apply to the new set of functions, which will differ only from those formed from π(π₯) and π1(π₯) by the absence of the same factor in every term of the series. 517 Example:- To find the position of the roots of the equation π₯4β4π₯3+π₯2+6π₯+2=0 Sturm's functions, formed according to the rule given above, are here calculated. π(π₯)=π₯4β4π₯3+π₯2+6π₯+2
π1(π₯)= 2π₯3β6π₯2+π₯+3
π2(π₯)= 5π₯2β10π₯β7
π3(π₯)= π₯β1
π3(π₯)= 12
The first terms of the functions are all positive; therefore there is no imaginary root.
π₯=β2β101234
π(π₯)=+++++++
π1(π₯)=ββ++β++
π2(π₯)=++βββ++
π3(π₯)=βββ++++
π4(π₯)=+++++++
No. of changes of signs4422200
The changes of sign in the functions, as π₯ passes through integral values, are exhibited in the adjoining table. There are two changes of sign lost while π₯ passes from β1 to 0, and two more lost while π₯ passes from 2 to 3. There are therefore two roots lying between 0 and β1; and two roots also between 2 and 3.These roots are all incommensurable, by (503). 518 Fourier's Theorem: Fourier's functions are the following quantities π(π₯), πβ²(π₯), πβ³(π₯), β―, πn(π₯) 519 Properties of Fourier's functions: As π₯ increases, Fourier's functions lose one change of sign for each roo of the equation π(π₯)=0, through which π₯ passes, and π changes of sign for π repeated roots. 520 If any of the other functions vanish, an even number of changes of sign is lost. 521 Results: The number of real roots of π(π₯) between πΌ and π½ cannot be more than the difference between the number of changes of sign in Fourier's functions when π₯=πΌ, and the number of changes when π₯=π½. 522 When that difference is odd, the number of intermediate roots is odd, and therfore one at least. 523 When the same difference is even, the number of intermediate roots is either even or zero. 524 Descartes's rule of signs follows from the above for the sign of Fourier's functions, when π₯=0 are the signs of the terms in π(π₯); and when π₯=β, Fourier's functions are all positive. 525 Lagrange's method of approximating to the incommensurable roots of an equation.Let πΌ be the greatest integer less than an incommensurable root of π(π₯). Diminish the roots of π(π₯) by π. Take the reciprocal of the resulting equation. Let π be the greates integer less than a positive root of this equation. Diminish the roots of this equation by π, and proceed as before. 526 Let π, π, π, β―, be the quantities thus determined; then, an approximation to the incommensurable root of π(π₯) will be the continued fraction π₯=π+1π+ 1π+527 Newton's method of approximation: If π1 be a quantity a little less than that one of the roots of the equation π(π₯)=0, so that π(π1+β)=0; then π1 is a first approximation to thevalue of the root. Also because π(π1+β)=π(π1)+βπβ²(π1)+ β2|2πβ³(π1)+β―426 and β is but small, a second approximation to the root will be π1β π(π1)πβ²(π1)=π2 In the same way a third approximation may be obtained from π2 and so on. 528 Fourier's limitation of Newton's method: To ensure that π1, π2, π3, β― shall successively increase up to the value π1+β without passing beyond it, it is necessary for all values of π₯ between π1 and π1+β. (i.) That π(π₯) and πβ²(π₯) should have contrary signs (ii.) That π(π₯) and πβ³(π₯) should have same signs fig. A proof may be obtained from the figure. Draw the curve π¦=π(π₯). Let ππ be a root of the equation, ππ=π1; draw the successive ordinates and tangents ππ, ππ, ππ , β―. Then ππ=π2, ππ=π3 and so on. Fig. (2) represents π2>ππ, and the subsequent approximations decreasing towards the root. 530 Newton's Rule for Limits of the Roots: Let the coefficients of π(π₯) be respectively divided by the Binomial coefficients, and let π0, π1, π2, β―, ππ, be the quotients, so that π(π₯)=π0π₯π+ππ1π₯πβ1+ π(πβ1)1β 2π2π₯πβ2+β―+πππβ1π₯+ππ Let π΄1, π΄2, π΄3, β―, π΄π, be formed by the law π΄π=π2πβππβ1ππ+1. Write the first series of quantities over the second, in the following manner: π0π1π2π3β―ππβ1ππ π΄0π΄1π΄2π΄3β―π΄πβ1π΄π Whenever two adjacent terms in the first series have the same sign, and the two corresponding terms below them in the second series also the same sign; let this be called a double permancence. When the two adjacent terms above have different signs, and the two below the same sign, let this be known as a variation-permancence. 531 Rule: The number of double permancences in the associated series is a superior limit to the number of negative roots of π(π₯). The number of variation-permancences is a superior limit to the number of positive roots. The number of imaginary roots cannot be less than the number of variations of sign in the second series. 532 Sylvester's Theorem: Let π(π₯+π) be expanded by (426) in powers of π₯, and let the two series be formed as in Newton's Rule (530). Let π(π) denote the number of double permanences. Then π(π)~π(π) is either equal to the number of roots of π(π₯), or surpasses that number by an even integer. Note: The first series may be multiplied by |π, and will then stand thus, ππ(π), ππβ1(π), |2ππβ2(π), |3ππβ3(π), β―, |ππ(π) The second series may be reduced to πΊπ(π), πΊπβ1(π), πΊπβ2(π),β―, πΊ(π), where πΊπ(π)β‘{ππ(π)}2β πβπ+1πβπππβ1(π)ππ+1(π) 533 Horner's Method: To find the numerical values of the roots of an equation. Take, for example, the equation π₯4β4π₯3+π₯2+6π₯+2=0 and find limits of the roots by Sturm's Method or otherwise. It has been shewn in (517) that this equation has two incommensurable roots between 2 and 3. The process of calculating the least of these roots is here exhibited.
β4
+1
+6
+2(2.414213
2
β4
β6
0
β2
β3
0
π΄120000
2
0
β6
β19584
0
β3
π΅1β6000
π΄24160000
2
4
1104
β2955839
2
πΆ1100
β4806
π΄312041610000
2
176
1872
β11437245184
π·140
276
π΅2β3024000
π΄4604364816
4
192
68161
β566003348
44
468
β2955839
π΄538361468
4
208
68723
β28285470
48
πΆ267600
π΅3β2887116000
π΄610075998
4
561
27804704
β 8485368
52
68161
β2859311296
π΄71590630
4
562
27895072
π·2560
68723
π΅4β2831446224
1
563
139918
282843)1590630(562372
561
πΆ36928600
β283001674
1414215
1
22576
139970
28284)176415
562
6951176
π΅5β282861704
169706
1
22592
700
2828) 6709
563
6973768
β28285470
5657
1
22608
700
282) 1052
π·35640
πΆ46996376
π΅6β28284770
848
4
11
21
28) 204
5644
69974
β2828456
197
4
11
21
2) 7
5648
69985
π΅7β2828435
5
14
11
2
5652
πΆ569996
4
πΆ67
π·45656
Root=2.414213562372
Method: Diminish the roots by 2 in the manner of (427).
The resulting coefficients are indicated by π΄1, π΅1, πΆ1, π·1.
By Newton's rule (527), βπ(π)πβ²(π), that is, β π΄1π΅1is an approximation to the remaining part of the root. This gives β 3 for the next figure; β 4 will be found to be the correct one. The highest figure must be taken which will not change the sign of π΄. Diminish the roots by β 4. This is accomplished most easily by affixingt ciphers to π΄1, π΅1, πΆ1, π·1, in the manner shewn, and then employing 4 instead of β 4. Having obtained π΄2 and observing that its sign is +, retrace the steps, trying 5 instead of 4. This gives π΄2 with a minus sign, thereby proving the existence of a root between 2β 4 and 2β 5. The new coefficients are π΄2, π΅2, πΆ2, π·2. β π΄2π΅2gives 1 for the next figure of the root. Affix ciphers as before, and diminish the roots by 1, distinguishin the new coefficients as π΄3, π΅3, πΆ3, π·1=3. Note that at every stage of the work π΄ and π΅ must preserve their signs unchanged. If a change of sign takes place it shews that tow large a figure has been tried. To abridge the calculation proceed thus: After a certain number of figures of the root have been obtained (in this example four), instead of adding ciphers cut off one digit from π΅4, two from πΆ4 and three from π·4. This amounts to the same thing as addign the ciphers, and then dividing each number by 10000. Continue the work with the numbers so reduced, and cut off digits in like manner at each stage until the π· and πΆ columns have disappeared. π΄7 and π΅7 now alone remain, and six additional figures of the root are determined correctly by the division of π΄7 and π΅7. To find the other root which lies between 2 and 3, we proceed as follows: After diminishing the roots by 2, try 6 for the next figure. This gives π΄2 negative; 7 does the same, but 8 makes π΄2 positive. That is to say, π(2β 7) is negative, and π(2β 8) positive. Therefore a root exists between 2β 7 and 2β 8, and its value may be approximated to, in the manner shewn. Throughout this last calculation π΄ will preserve the negative sign. Observe also that the trial number for the next figure of the root given at each stage of the process by the formula β π(π)πβ²(π), will in this case be always too great, as in the former case it was always too small. Sources and Referenceshttps://archive.org/details/synopsis-of-elementary-results-in-pure-and-applied-mathematics-pdfdriveΒ©sideway ID: 210800015 Last Updated: 8/15/2021 Revision: 0 Ref: References
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