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RULED SURFACES WITH CONSTANT PARAMETER OF ...

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210 E. Kasap, M. Masal<br />

From (2.2), a ruled surface M with constant distribution parameter has the<br />

following differential equation:<br />

x2x ′ 3 − x3x ′ 2 + (1 − x21 )τ − x1x3κ<br />

<br />

<br />

= C X ′<br />

<br />

<br />

, φ(s) = 0,<br />

where C is a constant. Hence, we have<br />

<br />

x1 = x2κds + c1,<br />

<br />

x3 = x2( C|| X ′ || 2<br />

1 − x2 1<br />

x 2 1 + x22 + x23 = 1.<br />

2<br />

− τ)ds + c2,<br />

(2.3)<br />

The second equation of the triple (2.3) is an integral equation for the unknown<br />

x3 = x3(s). Therefore, if x2 = x2(s) is given, we obtain x1 = x1(s) and<br />

x3 = x3(s). Thus, we have the following theorem.<br />

Theorem 2.1. The range of existence of ruled surfaces M with constant<br />

distribution parameter comprises within one arbitrary function of one variable.<br />

From the equalities<br />

<br />

<br />

λ X ′ + v X ′ ∧ <br />

<br />

X<br />

2<br />

= λ 2<br />

<br />

<br />

X ′<br />

<br />

<br />

and <br />

<br />

X ′<br />

∧ X<br />

<br />

= X ′<br />

<br />

<br />

,<br />

2<br />

+ v 2<br />

<br />

<br />

X ′ ∧ <br />

<br />

X<br />

the unit normal vectors to the ruled surface M at (s , v ) and (s , o) are<br />

n(s , v ) = λ ℓ(s) + v ℓ(s) ∧ X(s)<br />

√ v 2 + λ 2<br />

References<br />

2<br />

, n(s , o) = ℓ(s) = X ′ (s)<br />

<br />

<br />

X ′ <br />

<br />

.<br />

(s) <br />

[1] M. Chasles, Corresp. Mathem. et Phys. De Quetelet, 11 (1839).<br />

[2] M.P. Docarmo, Differential Geometry of Curves and Surfaces, Prentice-<br />

Hall, Englewood Cliffs (1976).<br />

[3] W.L. Edge, The Theory of Ruled Surfaces, Cambridge Univ. Press., Cambridge,<br />

UK (1931)

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