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ANALYSIS OF SURFACES AT SMALL DEFORMATIONS<br />

For this surface we have:<br />

1<br />

11 = 1 22 =<br />

41<br />

1 + 4 2 1 + 42 2 ; 2 11 = 2 22 =<br />

b11 = b22 =<br />

1<br />

12 = 2 12 = 0;<br />

2<br />

p<br />

1 + 4 2 1 + 42<br />

From (14), (15) and (16) we have = and<br />

@<br />

@2<br />

@<br />

@1 + @<br />

@2<br />

For y 1<br />

, respectively y 2<br />

we get<br />

respectively<br />

42<br />

1 + 4 2 1 + 42 2 ;<br />

; b12 = 0:<br />

@<br />

= 0; (19)<br />

@1<br />

= 0: (20)<br />

@y<br />

@1 = @r<br />

@1 + @r<br />

@2 = (; ; 2 1 22);<br />

@y<br />

@2 = @r<br />

@1<br />

Hence it follows<br />

@r<br />

@2 = (; ; 2 1 + 22):<br />

dy = @y<br />

@1 d 1+ @y<br />

@2 d 2 = (; ; 21 22)d1+(; ; 21+22)d2:<br />

By integrating, we get the rotation eld of hyperbolic paraboloid<br />

in the form<br />

y(1; 2) = (y1(1; 2); y2(1; 2); y2(1; 2)).<br />

Now we determine the innitesimal deformations eld of elliptic<br />

paraboloid. It appears, that<br />

dz = y ¢ dr =<br />

<br />

e1 e2 e3<br />

y1(1; 2) y2(1; 2) y3(1; 2)<br />

d1 d2 21d1 22d2<br />

= ( 2y2(1; 2)1; y3(1; 2) + 2y1(1; 2)1; y2(1; 2))d1+<br />

+( 2y2(1; 2)2 y3(1; 2); 2y1(1; 2)2; y1(1; 2))d2:<br />

By integrating, we get the innitesimal deformations eld of elliptic<br />

paraboloid<br />

z(1; 2) = (z1(1; 2); z2(1; 2); z3(1; 2)).<br />

=<br />

63

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