Geodesic curvature, normal curvature, and geodesic torsion

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SUMMARY

The discussion focuses on the definitions and relationships between geodesic curvature, normal curvature, and geodesic torsion in the context of differential geometry. Participants clarify the definitions of the unit normal field N(s) and the normal vector n(s) associated with a curve α. They analyze the derivatives of the tangent vector T, normal vector N, and normal vector n, leading to the conclusion that the second fundamental form is defined as II(T,T) = k_{n} and II(T,n) = τ_{g}. The importance of sign conventions in these definitions is also emphasized, particularly regarding the relationship between N'·n and N'·N.

PREREQUISITES
  • Differential geometry concepts, particularly geodesic curvature and torsion
  • Understanding of the Darboux frame and its definitions
  • Familiarity with vector calculus and derivatives in the context of curves on surfaces
  • Knowledge of the second fundamental form and its applications
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  • Explore the definitions and properties of geodesic curvature and torsion in detail
  • Investigate the second fundamental form and its role in curvature analysis
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Demon117
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I am struggling to make sense out some things. Hopefully someone can help or at least offer some different point of view. Let's examine a differential curve parameterized by arc length that maps some interval into an oriented surface (lets call it N(s)). The surface has a unit normal field restricted to the curve \alpha. Also, let n(s):=N(s)\wedge T(s) where T(s)=\alpha '(s).

If we define the derivatives of T, N, and n as the following

T'=-k_{g}n+k_{n}N
n'=k_{g}T+\tau_{g}N
N'=-k_{n}T-\tau_{g}n

then we should have N'\cdot T = -k_{n} and the second fundamental form is given by II(T,T) = k_{n} while N'\cdot n=-\tau_{g} so that the second fundamental form is given by II(T,n)=\tau_{g}.

This seems pretty clear to me, unless I have my definitions mixed up some how. Does this seem correct?
 
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Demon117 said:
I am struggling to make sense out some things. Hopefully someone can help or at least offer some different point of view. Let's examine a differential curve parameterized by arc length that maps some interval into an oriented surface (lets call it N(s)). The surface has a unit normal field restricted to the curve \alpha. Also, let n(s):=N(s)\wedge T(s) where T(s)=\alpha '(s).

Hmm. I'm not sure what your ##N(s)## is supposed to be. Is ##N(s)## the normal of the surface at point ##\alpha(s)##?

If we define the derivatives of T, N, and n as the following

T'=-k_{g}n+k_{n}N
n'=k_{g}T+\tau_{g}N
N'=-k_{n}T-\tau_{g}n

I get some sign differences. I think you should see http://en.wikipedia.org/wiki/Darboux_frame for the correct definitions.

the second fundamental form is given by II(T,T) = k_{n} while N'\cdot n=-\tau_{g} so that the second fundamental form is given by II(T,n)=\tau_{g}.

Not sure where this comes from. Could you clarify?
 
micromass said:
Hmm. I'm not sure what your ##N(s)## is supposed to be. Is ##N(s)## the normal of the surface at point ##\alpha(s)##?

Yes that is correct. I made a mistake in my initial statement. N(s) is the unit normal field to the surface at \alpha(s). Thanks for allowing me to clarify this. That means n(s) is the normal to the curve \alpha.

I get some sign differences. I think you should see http://en.wikipedia.org/wiki/Darboux_frame for the correct definitions.

I will look into this.

Not sure where this comes from. Could you clarify?

The second fundamental form defined by II(v,v)=-\left\langle dN_{p}v,v\right\rangle for any v in the tangent plane at a point p of S.
 
Demon117 said:
The second fundamental form defined by II(v,v)=-\left\langle dN_{p}v,v\right\rangle for any v in the tangent plane at a point p of S.

I agree with that then, up to signs. (Not that signs are all that important)
 
micromass said:
I agree with that then, up to signs. (Not that signs are all that important)

That is interesting, because I spoke with a professor recently about this and his claim was that the geodesic torsion was defined by II(T,N)=\tau_{g}. But by inspection this wouldn't make sense. I'm just confused a little I guess.
 
Demon117 said:
That is interesting, because I spoke with a professor recently about this and his claim was that the geodesic torsion was defined by II(T,N)=\tau_{g}. But by inspection this wouldn't make sense. I'm just confused a little I guess.

Signs are not so important anyway. If he defines his geodesic torsion like that, then I don't think it'll make a lot of difference. It'll yield the same theory up to sign.
 
micromass said:
Signs are not so important anyway. If he defines his geodesic torsion like that, then I don't think it'll make a lot of difference. It'll yield the same theory up to sign.

I agree with the sign issue but I think it does make a huge difference because N'\cdot n \ne N'\cdot N by definition of the Darboux frame, and by that same definition N'\cdot n=\tau_{g}. So II(T,N)\ne \tau_{g}.
 

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