Skip to main content
Futurologist's user avatar
Futurologist's user avatar
Futurologist's user avatar
Futurologist
  • Member for 9 years, 5 months
  • Last seen more than a month ago
comment
A generalization of the Tucker circle theorem and the Thomsen theorem associated with a conic
@ĐàoThanhOai Hi, yes I agree. Let me know what information you would need from me.
awarded
comment
Why is every Hamiltonian system locally integrable?
@issoroloap I have a feeling that Fan Zheng may have a point. If you look at the proof of Darboux's theorem in Arnold's book on mechanics, the symplectically "flat" coordinates there seem to have been constructed exactly by finding the local Hamitonians in involution that generate the local tangent Lagrangian submanifold.
awarded
comment
Geometric properties of solutions of Hamiltonian system
So basically you have a time-dependent periodic perturbation of a integrable Hamiltonian written in action-angle coordinates? And you want to apply some averaging technique? By the way, the homogeneity of the Hamiltonian suggests a conservation law, which leads to another Hamiltonian that commutes with this one, so you may be able to reduce the system a bit... What does Arnold's book on mechanics say? He has discussed averaging there...
comment
Geometric properties of solutions of Hamiltonian system
If $\dot{\phi} = \omega(q)$ doesn't that imply that $K$ does not depend on $p_{\phi}$? Isn't your Hamiltonian $H(q,\phi, p, p_{\phi}) = p_{\phi} \omega(q) + K(q,\phi, p)$?
revised
Convergence of Discrete Geodesic
added some missing symbols in the partrial derivatives
Loading…
comment
Clarification on tetrad indices
No, I think such index "commutativity" does not hold in general. I simply mean that the notation is, as you said it yourself, taking the $k$-th component of the covariant derivative $(\nabla_{F_4}F_3)^k = (F_4^l \nabla_l F_3)^k = F_4^l (\nabla_l F_3)^k$ is written as $F_4^l \nabla_l F_3^{\, k}$. Simply the parentheses are omitted. In general $$(\nabla_l v)^k \partial_k = \nabla_l ( v^k ) \partial_k + v^j \Gamma_{ l j }^k \partial_k$$
answered
Loading…
comment
Gauss' theorem for null boundaries
I am not convinced about the vector field decomposition $X = \langle X, N \rangle N + Y$ because, if I understand correctly, $N$ is not Lorentz orthogonal to your frame of vectors $e_1,..,e_{n-1}$. I would say $X = \lambda N + Y$ where $Y$ is light-like. Then $\langle X, Y \rangle = \lambda \langle N, Y \rangle + \langle Y, Y \rangle = \lambda \langle N, Y \rangle $ and solve for $\lambda$.
revised
Loading…
Loading…
revised
approaches to Apollonius circle problems
added 649 characters in body
Loading…
comment
approaches to Apollonius circle problems
I don't know if it helps but these chains can be transformed to Poncelet's porism: the points of tangencies between pairs of black circles lie on a common circle orthogonal to all black ones. Furthermore the centers of the black circles lie on an ellipse. So the poligonal line formed by connecting pairs of centers of adjacent black circles is inscribed in the ellipse and tangent to the orthogonal circle.
comment
approaches to Apollonius circle problems
Yeah, the philosophy is somewhat similar, when you think of Veronese embedding as a tool for studying incidence between points and conics... I guess...
answered
Loading…
awarded
comment
Bending Beltrami Pseudosphere
It seems to me that you shouldn't have points like S and maybe R (if I'm seeing the picture correctly) because the curvature of the surface at those points will be positive after adding the transverse vertical circles...
Loading…
revised
Convergence of Discrete Geodesic
added 2 characters in body
Loading…