Geodesic curvature, normal curvature, and geodesic torsion

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Discussion Overview

The discussion revolves around the concepts of geodesic curvature, normal curvature, and geodesic torsion in the context of differential geometry. Participants examine the definitions and relationships between various derivatives of curves and surfaces, specifically focusing on the second fundamental form and its implications.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents a set of equations defining the derivatives of the tangent vector T, the normal vector N, and the normal vector n, questioning their correctness.
  • Another participant seeks clarification on the definition of N(s), confirming it as the unit normal field to the surface at the point α(s).
  • There are noted sign differences in the definitions of the derivatives, with a suggestion to refer to the Darboux frame for clarification.
  • Participants discuss the second fundamental form, with one stating it is defined as II(v,v)=-⟨dNₚv,v⟩ for any v in the tangent plane, agreeing on this definition but noting potential sign discrepancies.
  • One participant expresses confusion regarding a professor's claim that geodesic torsion is defined by II(T,N)=τ₍g₎, suggesting it does not make sense by inspection.
  • Another participant acknowledges that sign differences may not be significant but emphasizes that they could lead to different interpretations of the relationships between the vectors.
  • There is a contention that N'·n ≠ N'·N by the definition of the Darboux frame, leading to the assertion that II(T,N) ≠ τ₍g₎.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of the second fundamental form and geodesic torsion, indicating that multiple competing interpretations exist without a clear consensus.

Contextual Notes

Participants highlight potential sign differences in definitions and relationships, which may affect the interpretation of the second fundamental form and geodesic torsion. There is also mention of reliance on specific definitions, such as those from the Darboux frame.

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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