Dimensionality of the Poincare section?
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Consider the Poincare map $P$, for which we place the Poincare section transverse to the trajectories and it intersects at various points which forms a set of discrete points.
For $dotx = f(x)$ where $x$ is an $n$ dimensional vector, why the section $S$ is an $n-1$ dimensional surface? How can I visualize this?
dynamical-systems dimensional-analysis
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Consider the Poincare map $P$, for which we place the Poincare section transverse to the trajectories and it intersects at various points which forms a set of discrete points.
For $dotx = f(x)$ where $x$ is an $n$ dimensional vector, why the section $S$ is an $n-1$ dimensional surface? How can I visualize this?
dynamical-systems dimensional-analysis
add a comment |Â
up vote
1
down vote
favorite
up vote
1
down vote
favorite
Consider the Poincare map $P$, for which we place the Poincare section transverse to the trajectories and it intersects at various points which forms a set of discrete points.
For $dotx = f(x)$ where $x$ is an $n$ dimensional vector, why the section $S$ is an $n-1$ dimensional surface? How can I visualize this?
dynamical-systems dimensional-analysis
Consider the Poincare map $P$, for which we place the Poincare section transverse to the trajectories and it intersects at various points which forms a set of discrete points.
For $dotx = f(x)$ where $x$ is an $n$ dimensional vector, why the section $S$ is an $n-1$ dimensional surface? How can I visualize this?
dynamical-systems dimensional-analysis
asked Jul 31 at 14:34
BAYMAX
2,43121021
2,43121021
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1 Answer
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Two angles for explanation:
The Poincaré map is supposed to remove exactly one dimension from the dynamics: The one corresponding to time. All other dimensions must still be present in the Poincaré map. Hence itâÂÂs state space must have dimension $n-1$. As the state space consists of points of the Poincaré section, the section also must have dimension $n-1$.
For most applications, you want the Poincaré map to have one iteration per oscillationù. Hence, the Poincaré section has to be frequently intersected. Now, very loosely speaking, a trajectory segment (a one-dimensional object) has a probability of zero to hit any object (the Poincaré section) with dimension $n-2$ or lower, while it cannot miss an $n-1$-dimensional object. Of course, for some dynamics you may carefully place an $n-2$-dimensional section such that it is hit for sure, but this would mean that your dynamics has a spurious dimension.
ùâ¯otherwise itâÂÂs every other oscillation, every high-amplitude oscillation, or similar, but the argument stays essentially the same
How the Poincare map removes exactly one dimension(the time) from the dynamics? is it because the map is time independent? like $x_n+1 = f(x_n)$? where as its continous version still has time like $fracdxdt=f(x)$ ?
â BAYMAX
Aug 1 at 9:09
@BAYMAX: I am not sure I get your question here, but the question in your comment seems to be asked the wrong way around. The Poincaré map removes one dimension because $S$ is $n-1$-dimensional. $S$ is chosen this way because otherwise we wouldnâÂÂt get a useful map. (Also see my edit.)
â Wrzlprmft
Aug 1 at 9:25
add a comment |Â
1 Answer
1
active
oldest
votes
1 Answer
1
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
2
down vote
accepted
Two angles for explanation:
The Poincaré map is supposed to remove exactly one dimension from the dynamics: The one corresponding to time. All other dimensions must still be present in the Poincaré map. Hence itâÂÂs state space must have dimension $n-1$. As the state space consists of points of the Poincaré section, the section also must have dimension $n-1$.
For most applications, you want the Poincaré map to have one iteration per oscillationù. Hence, the Poincaré section has to be frequently intersected. Now, very loosely speaking, a trajectory segment (a one-dimensional object) has a probability of zero to hit any object (the Poincaré section) with dimension $n-2$ or lower, while it cannot miss an $n-1$-dimensional object. Of course, for some dynamics you may carefully place an $n-2$-dimensional section such that it is hit for sure, but this would mean that your dynamics has a spurious dimension.
ùâ¯otherwise itâÂÂs every other oscillation, every high-amplitude oscillation, or similar, but the argument stays essentially the same
How the Poincare map removes exactly one dimension(the time) from the dynamics? is it because the map is time independent? like $x_n+1 = f(x_n)$? where as its continous version still has time like $fracdxdt=f(x)$ ?
â BAYMAX
Aug 1 at 9:09
@BAYMAX: I am not sure I get your question here, but the question in your comment seems to be asked the wrong way around. The Poincaré map removes one dimension because $S$ is $n-1$-dimensional. $S$ is chosen this way because otherwise we wouldnâÂÂt get a useful map. (Also see my edit.)
â Wrzlprmft
Aug 1 at 9:25
add a comment |Â
up vote
2
down vote
accepted
Two angles for explanation:
The Poincaré map is supposed to remove exactly one dimension from the dynamics: The one corresponding to time. All other dimensions must still be present in the Poincaré map. Hence itâÂÂs state space must have dimension $n-1$. As the state space consists of points of the Poincaré section, the section also must have dimension $n-1$.
For most applications, you want the Poincaré map to have one iteration per oscillationù. Hence, the Poincaré section has to be frequently intersected. Now, very loosely speaking, a trajectory segment (a one-dimensional object) has a probability of zero to hit any object (the Poincaré section) with dimension $n-2$ or lower, while it cannot miss an $n-1$-dimensional object. Of course, for some dynamics you may carefully place an $n-2$-dimensional section such that it is hit for sure, but this would mean that your dynamics has a spurious dimension.
ùâ¯otherwise itâÂÂs every other oscillation, every high-amplitude oscillation, or similar, but the argument stays essentially the same
How the Poincare map removes exactly one dimension(the time) from the dynamics? is it because the map is time independent? like $x_n+1 = f(x_n)$? where as its continous version still has time like $fracdxdt=f(x)$ ?
â BAYMAX
Aug 1 at 9:09
@BAYMAX: I am not sure I get your question here, but the question in your comment seems to be asked the wrong way around. The Poincaré map removes one dimension because $S$ is $n-1$-dimensional. $S$ is chosen this way because otherwise we wouldnâÂÂt get a useful map. (Also see my edit.)
â Wrzlprmft
Aug 1 at 9:25
add a comment |Â
up vote
2
down vote
accepted
up vote
2
down vote
accepted
Two angles for explanation:
The Poincaré map is supposed to remove exactly one dimension from the dynamics: The one corresponding to time. All other dimensions must still be present in the Poincaré map. Hence itâÂÂs state space must have dimension $n-1$. As the state space consists of points of the Poincaré section, the section also must have dimension $n-1$.
For most applications, you want the Poincaré map to have one iteration per oscillationù. Hence, the Poincaré section has to be frequently intersected. Now, very loosely speaking, a trajectory segment (a one-dimensional object) has a probability of zero to hit any object (the Poincaré section) with dimension $n-2$ or lower, while it cannot miss an $n-1$-dimensional object. Of course, for some dynamics you may carefully place an $n-2$-dimensional section such that it is hit for sure, but this would mean that your dynamics has a spurious dimension.
ùâ¯otherwise itâÂÂs every other oscillation, every high-amplitude oscillation, or similar, but the argument stays essentially the same
Two angles for explanation:
The Poincaré map is supposed to remove exactly one dimension from the dynamics: The one corresponding to time. All other dimensions must still be present in the Poincaré map. Hence itâÂÂs state space must have dimension $n-1$. As the state space consists of points of the Poincaré section, the section also must have dimension $n-1$.
For most applications, you want the Poincaré map to have one iteration per oscillationù. Hence, the Poincaré section has to be frequently intersected. Now, very loosely speaking, a trajectory segment (a one-dimensional object) has a probability of zero to hit any object (the Poincaré section) with dimension $n-2$ or lower, while it cannot miss an $n-1$-dimensional object. Of course, for some dynamics you may carefully place an $n-2$-dimensional section such that it is hit for sure, but this would mean that your dynamics has a spurious dimension.
ùâ¯otherwise itâÂÂs every other oscillation, every high-amplitude oscillation, or similar, but the argument stays essentially the same
edited Aug 1 at 9:21
answered Jul 31 at 19:24
Wrzlprmft
2,62111032
2,62111032
How the Poincare map removes exactly one dimension(the time) from the dynamics? is it because the map is time independent? like $x_n+1 = f(x_n)$? where as its continous version still has time like $fracdxdt=f(x)$ ?
â BAYMAX
Aug 1 at 9:09
@BAYMAX: I am not sure I get your question here, but the question in your comment seems to be asked the wrong way around. The Poincaré map removes one dimension because $S$ is $n-1$-dimensional. $S$ is chosen this way because otherwise we wouldnâÂÂt get a useful map. (Also see my edit.)
â Wrzlprmft
Aug 1 at 9:25
add a comment |Â
How the Poincare map removes exactly one dimension(the time) from the dynamics? is it because the map is time independent? like $x_n+1 = f(x_n)$? where as its continous version still has time like $fracdxdt=f(x)$ ?
â BAYMAX
Aug 1 at 9:09
@BAYMAX: I am not sure I get your question here, but the question in your comment seems to be asked the wrong way around. The Poincaré map removes one dimension because $S$ is $n-1$-dimensional. $S$ is chosen this way because otherwise we wouldnâÂÂt get a useful map. (Also see my edit.)
â Wrzlprmft
Aug 1 at 9:25
How the Poincare map removes exactly one dimension(the time) from the dynamics? is it because the map is time independent? like $x_n+1 = f(x_n)$? where as its continous version still has time like $fracdxdt=f(x)$ ?
â BAYMAX
Aug 1 at 9:09
How the Poincare map removes exactly one dimension(the time) from the dynamics? is it because the map is time independent? like $x_n+1 = f(x_n)$? where as its continous version still has time like $fracdxdt=f(x)$ ?
â BAYMAX
Aug 1 at 9:09
@BAYMAX: I am not sure I get your question here, but the question in your comment seems to be asked the wrong way around. The Poincaré map removes one dimension because $S$ is $n-1$-dimensional. $S$ is chosen this way because otherwise we wouldnâÂÂt get a useful map. (Also see my edit.)
â Wrzlprmft
Aug 1 at 9:25
@BAYMAX: I am not sure I get your question here, but the question in your comment seems to be asked the wrong way around. The Poincaré map removes one dimension because $S$ is $n-1$-dimensional. $S$ is chosen this way because otherwise we wouldnâÂÂt get a useful map. (Also see my edit.)
â Wrzlprmft
Aug 1 at 9:25
add a comment |Â
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