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Case 1 (row ~t<br />

(al N" 3<br />

-1 '" 25 + 1- 1- '" 245 3 + 65<br />

Y 35 +45 1252 +1<br />

Ih) N = 4<br />

z '" 25 + -.L -.L 1- = 1205 4 + 365 2 + 1<br />

3s+45+5560s3 +85<br />

'~<br />

2 4<br />

T_3__T~<br />

Case 2 (low pa55l<br />

(a) N 3<br />

z-t "25 + 1- -.L '" 245 3 + 65<br />

35+ 45 12s2 +1<br />

(b) N = 4<br />

111 1205 4 +365 2 +1<br />

y"25+ 3S +45 +SS= 60s3 +85<br />

Case 3 (high pa55)<br />

(a) N 3<br />

--H<br />

1 + 185 2 2<br />

_ 1 1 1<br />

y-l~<br />

Y 1 = 25 + l73S + 1/45 = 25 + 245 3<br />

~3<br />

~J<br />

Ih) N = 4 ---H<br />

1 1 1 ~l -t 385 2 + 1205 4 2 4<br />

1<br />

,~<br />

z = 2S + 1/35 + 1/45 + 1/55 '"<br />

25 + 645 3<br />

~3<br />

Il<br />

~5<br />

Case 4 (high pa5s)<br />

ta) N 3<br />

z-l = ~5 + l/~S + 1/~5 '" 25 + 245 3<br />

' + 185 2 3<br />

Z-l~<br />

Il<br />

~2 ~4<br />

Ih) N = 4<br />

1 1 1 1 1 + 385 2 + 1205 4 3<br />

y= y~<br />

25 + 1/35 + 1/45 + 1/55 =<br />

25 + 645 3<br />

Figure 3.5.<br />

~2<br />

Some continued fraction expansions.<br />

Il<br />

~4 ~1<br />

53

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