Easy examples of correspondence between global and local, as preparation for Gauss's theorem and Stokes's theoremApplications of Vector Calculus to Economics/FinanceHands-on demonstration ideas for multivariate calculusSurfaces and volumes for vector calculusOpen Source Math Software in Multivariate CalculusAdvanced Calculus vs. Analysis for a first proof-based courseDifferential forms in mechanics?How can we focus students on the various data types in multivariable calculus?In a typical 3rd-semester multivariate calculus course in the US, what kind of area integrals do students actually learn to do?
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Easy examples of correspondence between global and local, as preparation for Gauss's theorem and Stokes's theorem
Applications of Vector Calculus to Economics/FinanceHands-on demonstration ideas for multivariate calculusSurfaces and volumes for vector calculusOpen Source Math Software in Multivariate CalculusAdvanced Calculus vs. Analysis for a first proof-based courseDifferential forms in mechanics?How can we focus students on the various data types in multivariable calculus?In a typical 3rd-semester multivariate calculus course in the US, what kind of area integrals do students actually learn to do?
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I'm teaching freshman electricity and magnetism this semester, and as usual in this type of course, I will need to teach my students a lot of vector calculus before they see it in a math course. The usual way this works in most curricula in my country (US) is that students only learn the integral form of Maxwell's equations. This semester, I'm attempting to do more of a balanced presentation, so that students will have some clue as to the local form of these equations, and of the correspondence between the differential and integral forms. This is meant to be mostly at a pretty simple level, without a lot of emphasis on coordinate-based calculations. They will see Gauss's law next week (the second week of the semester), but will not see Stokes's theorem until the very last week of the semester.
In this context, I'm looking for simple, easy examples of this kind of interplay of global and local perspectives in math. The simplest example I've come up with, to get across the idea that there can be local statements and global ones, is a linguistic one:
There are three errors in the sentence, only one of which can be detected if you're looking through a keyhole and can only see one letter.
A second example would be that if one of the kitchen staff at a fancy restaurant is stealing the gold-plated silverware, you can detect it either by seeing them put it in their pocket, or by seeing that the count of pieces at the end of the day is short. This is the discrete analog of the fundamental theorem of calculus.
As a third, visual example very specifically applied to Gauss's law, I have this picture:
Here a vector field in two dimensions is represented by field lines. If this is a vacuum, then Gauss's law is being violated. Such a violation at the global level (line escaping the large square) can always also be detected at the local level as well (line escaping the small square).
I feel like there ought to be a nice example from some branch of mathematics that would interpolate between examples 2 and 3 in terms of obviousness or surprisingness. Basically I would like an example that is sort of interesting in its own right, and easy to verify once you see it, but that isn't like the silverware example in being kind of trivial and uninteresting.
It seems like Euler's polyhedral formula is exactly right in spirit, and maintains some simplicity because it's entirely discrete. However, I feel like I would probably need too big a chunk of a class session to do justice to this example. Is there some simpler example from geometry or topology that demonstrates the ideas without getting into calculus?
examples vector-calculus
$endgroup$
add a comment |
$begingroup$
I'm teaching freshman electricity and magnetism this semester, and as usual in this type of course, I will need to teach my students a lot of vector calculus before they see it in a math course. The usual way this works in most curricula in my country (US) is that students only learn the integral form of Maxwell's equations. This semester, I'm attempting to do more of a balanced presentation, so that students will have some clue as to the local form of these equations, and of the correspondence between the differential and integral forms. This is meant to be mostly at a pretty simple level, without a lot of emphasis on coordinate-based calculations. They will see Gauss's law next week (the second week of the semester), but will not see Stokes's theorem until the very last week of the semester.
In this context, I'm looking for simple, easy examples of this kind of interplay of global and local perspectives in math. The simplest example I've come up with, to get across the idea that there can be local statements and global ones, is a linguistic one:
There are three errors in the sentence, only one of which can be detected if you're looking through a keyhole and can only see one letter.
A second example would be that if one of the kitchen staff at a fancy restaurant is stealing the gold-plated silverware, you can detect it either by seeing them put it in their pocket, or by seeing that the count of pieces at the end of the day is short. This is the discrete analog of the fundamental theorem of calculus.
As a third, visual example very specifically applied to Gauss's law, I have this picture:
Here a vector field in two dimensions is represented by field lines. If this is a vacuum, then Gauss's law is being violated. Such a violation at the global level (line escaping the large square) can always also be detected at the local level as well (line escaping the small square).
I feel like there ought to be a nice example from some branch of mathematics that would interpolate between examples 2 and 3 in terms of obviousness or surprisingness. Basically I would like an example that is sort of interesting in its own right, and easy to verify once you see it, but that isn't like the silverware example in being kind of trivial and uninteresting.
It seems like Euler's polyhedral formula is exactly right in spirit, and maintains some simplicity because it's entirely discrete. However, I feel like I would probably need too big a chunk of a class session to do justice to this example. Is there some simpler example from geometry or topology that demonstrates the ideas without getting into calculus?
examples vector-calculus
$endgroup$
$begingroup$
Interesting question. I'm stuck on why the picture is a "violation" of Gauss's law. I mean, Gauss's law says that field lines start at charges, so, I would just think there is a charge inside the little black box...
$endgroup$
– James S. Cook
8 hours ago
$begingroup$
@JamesS.Cook: Good point, I just mean that it's a violation of Gauss's law in a vacuum.
$endgroup$
– Ben Crowell
7 hours ago
add a comment |
$begingroup$
I'm teaching freshman electricity and magnetism this semester, and as usual in this type of course, I will need to teach my students a lot of vector calculus before they see it in a math course. The usual way this works in most curricula in my country (US) is that students only learn the integral form of Maxwell's equations. This semester, I'm attempting to do more of a balanced presentation, so that students will have some clue as to the local form of these equations, and of the correspondence between the differential and integral forms. This is meant to be mostly at a pretty simple level, without a lot of emphasis on coordinate-based calculations. They will see Gauss's law next week (the second week of the semester), but will not see Stokes's theorem until the very last week of the semester.
In this context, I'm looking for simple, easy examples of this kind of interplay of global and local perspectives in math. The simplest example I've come up with, to get across the idea that there can be local statements and global ones, is a linguistic one:
There are three errors in the sentence, only one of which can be detected if you're looking through a keyhole and can only see one letter.
A second example would be that if one of the kitchen staff at a fancy restaurant is stealing the gold-plated silverware, you can detect it either by seeing them put it in their pocket, or by seeing that the count of pieces at the end of the day is short. This is the discrete analog of the fundamental theorem of calculus.
As a third, visual example very specifically applied to Gauss's law, I have this picture:
Here a vector field in two dimensions is represented by field lines. If this is a vacuum, then Gauss's law is being violated. Such a violation at the global level (line escaping the large square) can always also be detected at the local level as well (line escaping the small square).
I feel like there ought to be a nice example from some branch of mathematics that would interpolate between examples 2 and 3 in terms of obviousness or surprisingness. Basically I would like an example that is sort of interesting in its own right, and easy to verify once you see it, but that isn't like the silverware example in being kind of trivial and uninteresting.
It seems like Euler's polyhedral formula is exactly right in spirit, and maintains some simplicity because it's entirely discrete. However, I feel like I would probably need too big a chunk of a class session to do justice to this example. Is there some simpler example from geometry or topology that demonstrates the ideas without getting into calculus?
examples vector-calculus
$endgroup$
I'm teaching freshman electricity and magnetism this semester, and as usual in this type of course, I will need to teach my students a lot of vector calculus before they see it in a math course. The usual way this works in most curricula in my country (US) is that students only learn the integral form of Maxwell's equations. This semester, I'm attempting to do more of a balanced presentation, so that students will have some clue as to the local form of these equations, and of the correspondence between the differential and integral forms. This is meant to be mostly at a pretty simple level, without a lot of emphasis on coordinate-based calculations. They will see Gauss's law next week (the second week of the semester), but will not see Stokes's theorem until the very last week of the semester.
In this context, I'm looking for simple, easy examples of this kind of interplay of global and local perspectives in math. The simplest example I've come up with, to get across the idea that there can be local statements and global ones, is a linguistic one:
There are three errors in the sentence, only one of which can be detected if you're looking through a keyhole and can only see one letter.
A second example would be that if one of the kitchen staff at a fancy restaurant is stealing the gold-plated silverware, you can detect it either by seeing them put it in their pocket, or by seeing that the count of pieces at the end of the day is short. This is the discrete analog of the fundamental theorem of calculus.
As a third, visual example very specifically applied to Gauss's law, I have this picture:
Here a vector field in two dimensions is represented by field lines. If this is a vacuum, then Gauss's law is being violated. Such a violation at the global level (line escaping the large square) can always also be detected at the local level as well (line escaping the small square).
I feel like there ought to be a nice example from some branch of mathematics that would interpolate between examples 2 and 3 in terms of obviousness or surprisingness. Basically I would like an example that is sort of interesting in its own right, and easy to verify once you see it, but that isn't like the silverware example in being kind of trivial and uninteresting.
It seems like Euler's polyhedral formula is exactly right in spirit, and maintains some simplicity because it's entirely discrete. However, I feel like I would probably need too big a chunk of a class session to do justice to this example. Is there some simpler example from geometry or topology that demonstrates the ideas without getting into calculus?
examples vector-calculus
examples vector-calculus
edited 7 hours ago
Ben Crowell
asked 9 hours ago
Ben CrowellBen Crowell
7,77822 silver badges58 bronze badges
7,77822 silver badges58 bronze badges
$begingroup$
Interesting question. I'm stuck on why the picture is a "violation" of Gauss's law. I mean, Gauss's law says that field lines start at charges, so, I would just think there is a charge inside the little black box...
$endgroup$
– James S. Cook
8 hours ago
$begingroup$
@JamesS.Cook: Good point, I just mean that it's a violation of Gauss's law in a vacuum.
$endgroup$
– Ben Crowell
7 hours ago
add a comment |
$begingroup$
Interesting question. I'm stuck on why the picture is a "violation" of Gauss's law. I mean, Gauss's law says that field lines start at charges, so, I would just think there is a charge inside the little black box...
$endgroup$
– James S. Cook
8 hours ago
$begingroup$
@JamesS.Cook: Good point, I just mean that it's a violation of Gauss's law in a vacuum.
$endgroup$
– Ben Crowell
7 hours ago
$begingroup$
Interesting question. I'm stuck on why the picture is a "violation" of Gauss's law. I mean, Gauss's law says that field lines start at charges, so, I would just think there is a charge inside the little black box...
$endgroup$
– James S. Cook
8 hours ago
$begingroup$
Interesting question. I'm stuck on why the picture is a "violation" of Gauss's law. I mean, Gauss's law says that field lines start at charges, so, I would just think there is a charge inside the little black box...
$endgroup$
– James S. Cook
8 hours ago
$begingroup$
@JamesS.Cook: Good point, I just mean that it's a violation of Gauss's law in a vacuum.
$endgroup$
– Ben Crowell
7 hours ago
$begingroup$
@JamesS.Cook: Good point, I just mean that it's a violation of Gauss's law in a vacuum.
$endgroup$
– Ben Crowell
7 hours ago
add a comment |
2 Answers
2
active
oldest
votes
$begingroup$
Here are two similar ideas.
(1) The shortest geodesic between two points on the surface of a polyhedron (generally) bends as it crosses edges, when viewed
globally in $mathbbR^3$, but from the local point of view of an ant walking along the path, it is straight, i.e., straight when each crossed edge is unfolded flat.
This is commonly illustrated on a cube.
Here is a more complex example.
Shortest paths from upper left corner to each vertex. Image from here.
(2) Imagine an ant walking around the apex vertex in the left image
below. Locally it has no way of knowing whether it is exploring
a protrusion, or a dent (right image). The curvature is the same
at that central vertex, but the embeddings in $mathbbR^3$ are different.
Image from Discrete & Computational Geometry, p.177.
A bit of a stretch, but you could connect this to the difficulty
we have understanding the geometric shape of the universe.
$endgroup$
add a comment |
$begingroup$
One idea that comes to mind is the fact that a connected graph has a Eulerian circuit if and only if every vertex has even degree.
Another idea that comes to mind is just the Fundamental Theorem of Calculus. If you have a rather boring video of a car's speedometer as the car travels from A to B, then you can figure out the total distance the car has traveled in getting from A to B. The "list" of speeds read off from the speedometer is local/instantaneous information. The net distance traveled is a global quantity.
$endgroup$
add a comment |
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2 Answers
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2 Answers
2
active
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votes
$begingroup$
Here are two similar ideas.
(1) The shortest geodesic between two points on the surface of a polyhedron (generally) bends as it crosses edges, when viewed
globally in $mathbbR^3$, but from the local point of view of an ant walking along the path, it is straight, i.e., straight when each crossed edge is unfolded flat.
This is commonly illustrated on a cube.
Here is a more complex example.
Shortest paths from upper left corner to each vertex. Image from here.
(2) Imagine an ant walking around the apex vertex in the left image
below. Locally it has no way of knowing whether it is exploring
a protrusion, or a dent (right image). The curvature is the same
at that central vertex, but the embeddings in $mathbbR^3$ are different.
Image from Discrete & Computational Geometry, p.177.
A bit of a stretch, but you could connect this to the difficulty
we have understanding the geometric shape of the universe.
$endgroup$
add a comment |
$begingroup$
Here are two similar ideas.
(1) The shortest geodesic between two points on the surface of a polyhedron (generally) bends as it crosses edges, when viewed
globally in $mathbbR^3$, but from the local point of view of an ant walking along the path, it is straight, i.e., straight when each crossed edge is unfolded flat.
This is commonly illustrated on a cube.
Here is a more complex example.
Shortest paths from upper left corner to each vertex. Image from here.
(2) Imagine an ant walking around the apex vertex in the left image
below. Locally it has no way of knowing whether it is exploring
a protrusion, or a dent (right image). The curvature is the same
at that central vertex, but the embeddings in $mathbbR^3$ are different.
Image from Discrete & Computational Geometry, p.177.
A bit of a stretch, but you could connect this to the difficulty
we have understanding the geometric shape of the universe.
$endgroup$
add a comment |
$begingroup$
Here are two similar ideas.
(1) The shortest geodesic between two points on the surface of a polyhedron (generally) bends as it crosses edges, when viewed
globally in $mathbbR^3$, but from the local point of view of an ant walking along the path, it is straight, i.e., straight when each crossed edge is unfolded flat.
This is commonly illustrated on a cube.
Here is a more complex example.
Shortest paths from upper left corner to each vertex. Image from here.
(2) Imagine an ant walking around the apex vertex in the left image
below. Locally it has no way of knowing whether it is exploring
a protrusion, or a dent (right image). The curvature is the same
at that central vertex, but the embeddings in $mathbbR^3$ are different.
Image from Discrete & Computational Geometry, p.177.
A bit of a stretch, but you could connect this to the difficulty
we have understanding the geometric shape of the universe.
$endgroup$
Here are two similar ideas.
(1) The shortest geodesic between two points on the surface of a polyhedron (generally) bends as it crosses edges, when viewed
globally in $mathbbR^3$, but from the local point of view of an ant walking along the path, it is straight, i.e., straight when each crossed edge is unfolded flat.
This is commonly illustrated on a cube.
Here is a more complex example.
Shortest paths from upper left corner to each vertex. Image from here.
(2) Imagine an ant walking around the apex vertex in the left image
below. Locally it has no way of knowing whether it is exploring
a protrusion, or a dent (right image). The curvature is the same
at that central vertex, but the embeddings in $mathbbR^3$ are different.
Image from Discrete & Computational Geometry, p.177.
A bit of a stretch, but you could connect this to the difficulty
we have understanding the geometric shape of the universe.
answered 7 hours ago
Joseph O'RourkeJoseph O'Rourke
16.6k3 gold badges36 silver badges88 bronze badges
16.6k3 gold badges36 silver badges88 bronze badges
add a comment |
add a comment |
$begingroup$
One idea that comes to mind is the fact that a connected graph has a Eulerian circuit if and only if every vertex has even degree.
Another idea that comes to mind is just the Fundamental Theorem of Calculus. If you have a rather boring video of a car's speedometer as the car travels from A to B, then you can figure out the total distance the car has traveled in getting from A to B. The "list" of speeds read off from the speedometer is local/instantaneous information. The net distance traveled is a global quantity.
$endgroup$
add a comment |
$begingroup$
One idea that comes to mind is the fact that a connected graph has a Eulerian circuit if and only if every vertex has even degree.
Another idea that comes to mind is just the Fundamental Theorem of Calculus. If you have a rather boring video of a car's speedometer as the car travels from A to B, then you can figure out the total distance the car has traveled in getting from A to B. The "list" of speeds read off from the speedometer is local/instantaneous information. The net distance traveled is a global quantity.
$endgroup$
add a comment |
$begingroup$
One idea that comes to mind is the fact that a connected graph has a Eulerian circuit if and only if every vertex has even degree.
Another idea that comes to mind is just the Fundamental Theorem of Calculus. If you have a rather boring video of a car's speedometer as the car travels from A to B, then you can figure out the total distance the car has traveled in getting from A to B. The "list" of speeds read off from the speedometer is local/instantaneous information. The net distance traveled is a global quantity.
$endgroup$
One idea that comes to mind is the fact that a connected graph has a Eulerian circuit if and only if every vertex has even degree.
Another idea that comes to mind is just the Fundamental Theorem of Calculus. If you have a rather boring video of a car's speedometer as the car travels from A to B, then you can figure out the total distance the car has traveled in getting from A to B. The "list" of speeds read off from the speedometer is local/instantaneous information. The net distance traveled is a global quantity.
answered 5 hours ago
user52817user52817
3,7449 silver badges20 bronze badges
3,7449 silver badges20 bronze badges
add a comment |
add a comment |
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$begingroup$
Interesting question. I'm stuck on why the picture is a "violation" of Gauss's law. I mean, Gauss's law says that field lines start at charges, so, I would just think there is a charge inside the little black box...
$endgroup$
– James S. Cook
8 hours ago
$begingroup$
@JamesS.Cook: Good point, I just mean that it's a violation of Gauss's law in a vacuum.
$endgroup$
– Ben Crowell
7 hours ago