The difference between the continued fraction and the n^{th} convergent

1 a_{n+2}

is less than ------------, and greater than ------------. These limits

q_{n}q_{n+1} q_{n}q_{n+2}

may be replaced by the following, which, though not so close, are

1 1

simpler, viz. ------- and ------------------ .

q^{2}_n q_n(q_n + q_{n+1})

Every simple continued fraction must converge to a definite limit; for

its value lies between that of the first and second convergents and,

since

p_n p_{n-1} 1 p_n p_{n-1}

--- ~ ------- = ------------, Lt. ----- = Lt. -------,

q_n q_{n-1} q_{n}q_{n-1} q_n q_{n-1}

so that its value cannot oscillate.

The chief practical use of the simple continued fraction is that by

means of it we can obtain rational fractions which approximate to any

quantity, and we can also estimate the error of our approximation. Thus

a continued fraction equivalent to [pi] (the ratio of the circumference

to the diameter of a circle) is

1 1 1 1 1 1

3 + - -- -- --- -- --

7 + 15 + 1 + 292 + 1 + 1 + ...

of which the successive convergents are

3 22 333 355 103993

--, --, ---, ---, ------, &c.,

1 7 106 113 33102

the fourth of which is accurate to the sixth decimal place, since the

error lies between 1/q4q5 or .0000002673 and a6/q4q6 or .0000002665.

Similarly the continued fraction given by Euler as equivalent to

1/2(e -1) (e being the base of Napierian logarithms), viz.

1 1 1 1 1

-- -- -- -- --

1 + 6 + 10 + 14 + 18 + ...,

may be used to approximate very rapidly to the value of e.

For the application of continued fractions to the problem "To find the

fraction, whose denominator does not exceed a given integer D, which

shall most closely approximate (by excess or defect, as may be assigned)

to a given number commensurable or incommensurable," the reader is

referred to G. Chrystal's _Algebra_, where also may be found details of

the application of continued fractions to such interesting and important

problems as the recurrence of eclipses and the rectification of the

calendar (q.v.).

Lagrange used simple continued fractions to approximate to the solutions

of numerical equations; thus, if an equation has a root between two

integers a and a + 1, put x = a + 1/y and form the equation in y; if the

equation in y has a root between b and b + 1, put y = b + 1/z, and so

on. Such a method is, however, too tedious, compared with such a method

as Homer's, to be of any practical value.

The solution in integers of the indeterminate equation ax + by = c may

be effected by means of continued fractions. If we suppose a/b to be

converted into a continued fraction and p/q to be the penultimate

convergent, we have aq - bp = +1 or -1, according as the number of

convergents is even or odd, which we can take them to be as we please.

If we take aq-bp = +1 we have a general solution in integers of ax + by

= c, viz. x = cq - bt, y = at - cp; if we take aq - bp = -1, we have x =

bt - cq, y = cp - at.

An interesting application of continued fractions to establish a unique

correspondence between the elements of an aggregate of m dimensions and

an aggregate of n dimensions is given by G. Cantor in vol. 2 of the

_Acta Mathematica_.

Applications of simple continued fractions to the theory of numbers, as,

for example, to prove the theorem that a divisor of the sum of two

squares is itself the sum of two squares, may be found in J. A. Serret's

_Cours d'Algebre Superieure_.

2. _Recurring Simple Continued Fractions._--The infinite continued

fraction

1 1 1 1 1 1 1 1 1 1

a1 + -- -- --- -- -- --- -- -- --- --

a2 + a3 ... + a_n + b1 + b2 ... + b_n + b1 + b2 ... + b_n + b1 + ...,

where, after the n^{th} partial quotient, the cycle of partial quotients

b1, b2, ..., b_n recur in the same order, is the type of a recurring

simple continued fraction.

The value of such a fraction is the positive root of a quadratic

equation whose coefficients are real and of which one root is negative.

Since the fraction is infinite it cannot be commensurable and therefore

its value is a quadratic surd number. Conversely every positive

quadratic surd number, when expressed as a simple continued fraction,

will give rise to a recurring fraction. Thus

__ 1 1 1 1 1

2 - \/ 3 = -- -- -- -- --

3 + 1 + 2 + 1 + 2 + ...,

___ 1 1 1 1 1 1 1 1

\/ 28 = 5 + -- -- -- -- -- -- -- --

3 + 2 + 3 + 10 + 3 + 2 + 3 + 10 + ...

The second case illustrates a feature of the recurring continued

fraction which represents a complete quadratic surd. There is only one

non-recurring partial quotient a1. If b1, b2, ..., b_n is the cycle of

recurring quotients, then b_n = 2a1, b1 = b_{n-1}, b2 = b_{n-2}, b3 =

b_{n-3}, &c.

In the case of a recurring continued fraction which represents [sqr]N,

where N is an integer, if n is the number of partial quotients in the

recurring cycle, and p_{nr}/q_{nr} the nr^{th} convergent, then p^2_{nr}

-Nq^2_{nr} = (-1)^{nr}, whence, if n is odd, integral solutions of the

indeterminate equation x squared - Ny squared = +-1 (the so-called Pellian equation)

can be found. If n is even, solutions of the equation x squared -Ny squared = +1 can

be found.

The theory and development of the simple recurring continued fraction is

due to Lagrange. For proofs of the theorems here stated and for

applications to the more general indeterminate equation x squared -Ny squared = H the

reader may consult Chrystal's _Algebra_ or Serret's _Cours d'Algebre

Superieure_; he may also profitably consult a tract by T. Muir, _The

Expression of a Quadratic Surd as a Continued Fraction_ (Glasgow, 1874).

_The General Continued Fraction._

1. _The Evaluation of Continued Fractions._--The numerators and

denominators of the convergents to the general continued fraction both

satisfy the difference equation u_n = a_{n}u_{n-1} + b_{n}u_{n-2}. When

we can solve this equation we have an expression for the n^{th}

convergent to the fraction, generally in the form of the quotient of two

series, each of n terms. As an example, take the fraction (known as

Brouncker's fraction, after Lord Brouncker)

1 1 squared 3 squared 5 squared 7 squared

-- -- -- -- --

1 + 2 + 2 + 2 + 2 + ...

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