Surface parametrization and its differential

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Discussion Overview

The discussion revolves around the parametrization of a surface defined by the intersection of a plane and a cylinder, exploring the differential of the parametrized surface and the calculation of normal vectors. Participants engage in technical reasoning regarding the implications of their parametrization and the mathematical processes involved.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant proposes a parametrization of the surface using cylindrical coordinates, expressing the surface in vector notation and attempting to calculate the normal vector through tangent vectors and cross products.
  • Another participant challenges the initial parametrization, arguing that it does not describe a surface but rather the intersection of two surfaces, which is typically a one-dimensional object.
  • A later reply clarifies that the cylinder is solid, suggesting that the intersection forms a two-dimensional object, specifically an inclined circle.
  • One participant questions the necessity of multiplying the modulus of the cross product of tangent vectors by the differentials ds and dt when calculating the area of the parametrized surface.
  • Another participant responds by explaining that the modulus of the tangent vectors indicates the distance moved with parameter changes, and thus the area is proportional to these changes.
  • Further discussion includes a reference to line integrals, emphasizing the relationship between tangent vectors and parameter changes.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the parametrization and whether it adequately describes a surface. There is no consensus on the interpretation of the intersection of the plane and cylinder, nor on the necessity of certain calculations in determining the area of the parametrized surface.

Contextual Notes

Participants express uncertainty regarding the implications of their calculations and the definitions of the objects involved, particularly concerning the nature of the intersection and the role of differentials in surface parametrization.

jonjacson
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I will use an example:

-The surface is given by the intersection of the plane:

y+z=2

-And the infinite cilinder:

x2+y2<=1

We want to parametrize this surface, it could be done easily with:

x=r cosθ
y=r sin θ
z=2 - r cos θ

Then this surface could be written using vector notation:

S= r cosθ i + r sin θ j + (2 - r sin θ)k

I understand that these are a set of vectors starting from the origin and ending at the surface, so nothing has changed here, it is just a compact form of the same surface.

Then the normal vector is calculated first finding the tangent vectors on r and θ and then taking the cross product and multiplying this by dr dθ.

What I don't understand is, if I simply differenciate S, Why don't I get the same dS?

I will show what I mean.
1.- Using the first method:

Sr =(cos θ, sin θ,-sin θ)
Sθ =(-sinθ r, r cosθ, -r cos θ)

After doing the cross product I get:

Sr x Sθ
= r j + r k

This vector is normal to the surface, and it must be multiplied by dr dθ.

2.- WHat if I simply differenciate S? Shouldn't I get the same result as in part 1?

The differential of the vectors i, j, k is zero because they don't change.

We had S= r cosθ i + r sin θ j + (2 - r sin θ)k, so:

dS= (dr cos θ - sin θ dθ r) i + ...

I don't need to continue since the i part is not zero, but in the previous calculation it was zero. What is wrong with the normal process of differenciation? Shouldn't it give us a differential of surface?
I thought the differential of a parametrized surface is just the differential of its components but I don't know what to think now.
 
Last edited:
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jonjacson said:
I will use an example:

-The surface is given by the intersection of the plane:

y+z=2

-And the infinite cilinder:

x2+y2=1

We want to parametrize this surface, it could be done easily with:

x=r cosθ
y=r sin θ
z=2 - r cos θ

This is not describing a surface. It is the intersection between two two-dimensional surfaces in three dimensions - which is typically a one-dimensional object.
 
Orodruin said:
This is not describing a surface. It is the intersection between two two-dimensional surfaces in three dimensions - which is typically a one-dimensional object.

Maybe I didn't explain it well.

The cilinder is solid, is not empty, so the intersection is a kind of inclined circle.
 
I add a question.

If we have an area in the plane, the differential of this area is simply ds * dt, if there is a parametrized surface that arises from this plane area to form a 2d manifold in 3d space, the surface corresponding to ds * dt is:

Modulus (Tangent vector to s x Tangent vector to t) * ds * dt

Where x is the cross product.

What I don't understand is, Why is it not enough with the modulus of the cross product? Why do we multiply by ds and dt?

If I calculate the tangent vectors at a point and I calculate the cross product I get an area right?
 
In other words, Why tangent vectors are not divided by their own modulus so their modulus becomes 1?
 
jonjacson said:
In other words, Why tangent vectors are not divided by their own modulus so their modulus becomes 1?

Because the modulus of the tangent vectors tell you how far you move when the parameters change and the area you get by a certain parameter change is proportional to how far the parameter change takes you.

It is the same reason that you get
$$
d\vec x = \frac{d\vec x}{dt} dt
$$
in a line integral.
 
Orodruin said:
Because the modulus of the tangent vectors tell you how far you move when the parameters change and the area you get by a certain parameter change is proportional to how far the parameter change takes you.

It is the same reason that you get
$$
d\vec x = \frac{d\vec x}{dt} dt
$$
in a line integral.
I understand, the tangent vectors are the rate of change, multiplied by a dx you get a dy.

Thanks
 

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