What is Vector Area of an object?

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Discussion Overview

The discussion revolves around the concept of vector area, particularly in relation to its definition, differences from surface area, and its physical significance in contexts such as fluid dynamics. Participants explore theoretical aspects, mathematical representations, and practical applications of vector areas.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants describe vector area as a vector whose length equals the area of a surface and whose direction is perpendicular to that surface.
  • Others argue that only portions of a plane have a unique normal direction, while curved surfaces can be discussed in terms of differential vector areas.
  • A participant provides a mathematical example involving a sphere and discusses the calculation of the differential vector area using parametric equations and cross products.
  • Another participant explains the relationship between fluid velocity and differential vector area, emphasizing that only the component of velocity perpendicular to the surface contributes to flow through the surface.
  • Some participants seek simpler explanations of the concept, indicating a desire for clarification on the technical details presented.
  • One participant compares the concept of adding infinitesimal areas to adding infinitesimal vectors to obtain a total vector, highlighting the importance of understanding the infinitesimal in integrals.
  • A metaphor involving rain and windows is used to illustrate how the angle of a surface affects the amount of flow through it, linking back to the concept of vector area.

Areas of Agreement / Disagreement

Participants express various interpretations and applications of vector area, with no clear consensus on its significance or the best way to explain it. Some seek clarification while others provide technical details, indicating a mix of understanding and confusion.

Contextual Notes

Some discussions include assumptions about the nature of surfaces and fluid dynamics that may not be universally applicable. The mathematical steps involved in deriving vector areas are not fully resolved, leaving some aspects open to interpretation.

Who May Find This Useful

This discussion may be useful for students and professionals interested in fluid dynamics, vector calculus, and the mathematical representation of physical concepts related to surfaces.

kashan123999
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I read about them in Topic of FLUX,what are vector areas,how they are different from surface areas,apart from the fact that they are perpendicular to the surface area,but why is that so? and what is the physical significance of them? why they are used so?
 
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The "vector area" of a portion of a surface (not every "object" has "area" much less "vector area!) is a vector whose length is equal to the area of the surface and whose direction is perpendicular to the surface.

Strictly speaking, only a portion of a plane has a "vector area" since only a plane would have a unique normal direction. But given any curved surface we can talk about the "differential vector area" a "vector" whose length is the differential of area at a given point on the surface and whose direction is that of the normal vector at that point.

For example, the sphere with radius R and center at the origin can be written in parametric equations as
x= Rcos(\theta)sin(\phi), y= Rsin(\theta)sin(\phi) and z= Rcos(\phi).
That is the same as saying that the "position vector" or any point on surface is
\vec{v}= Rcos(\theta)sin(\phi)\vec{i}+ Rsin(\theta)sin(\phi)\vec{j}+ Rcos(\phi)\vec{k}

The derivatives with respect to \theta and \phi,
\vec{v}_\theta= -Rsin(\theta)sin(\phi)\vec{i}+ Rcos(\phi)sin(\phi)\vec{j}
and
\vec{v}_\phi= Rcos(\theta)cos(\phi)\vec{i}+ Rsin(\theta)cos(\phi)\vec{j}- Rsin(\phi)\vec{k}
are vectors lying in the tangent plane to the surface at each point.

Their cross product (I'll leave it to you to calculate that) is a vector perpendicular to both and so perpendicular to the tangent plane and perpendicular to the sphere at each point. Its length is the "differential of area" for the sphere and so the vector itself is the "vector differential of area".
 
kashan123999 said:
I read about them in Topic of FLUX,what are vector areas,how they are different from surface areas,apart from the fact that they are perpendicular to the surface area,but why is that so? and what is the physical significance of them? why they are used so?
If you have a 2D curved surface S, you can focus on a differential element of area within the surface dA. The differential vector area associated with this differential element of area is defined as dA=ndA , where n is a unit normal to the surface. Suppose you have a fluid with velocity v flowing at the surface. If the fluid is not flowing normal to the surface, then the component of velocity tangent to the surface does not result in any flow through the surface. Only the component of velocity perpendicular to the surface results in fluid flow through the surface. The volumetric flow rate of fluid through the differential area element dA is equal to the velocity vector v dotted with the normal to the surface n times the differential area dA. But this is the same as the velocity vector v dotted with the differential vector area dA.
 
Chestermiller said:
If you have a 2D curved surface S, you can focus on a differential element of area within the surface dA. The differential vector area associated with this differential element of area is defined as dA=ndA , where n is a unit normal to the surface. Suppose you have a fluid with velocity v flowing at the surface. If the fluid is not flowing normal to the surface, then the component of velocity tangent to the surface does not result in any flow through the surface. Only the component of velocity perpendicular to the surface results in fluid flow through the surface. The volumetric flow rate of fluid through the differential area element dA is equal to the velocity vector v dotted with the normal to the surface n times the differential area dA. But this is the same as the velocity vector v dotted with the differential vector area dA.

please can you explain it in lay-man's terms please :(
 
Just like you can add infinitesimal areas to get a total area, you can add infinitesimal vectors over a region to get a total vector as a result.

Its knowing what the infinitesimal is and what you are actually adding with regard to the integral that is key in understanding the above statement.
 
kashan123999 said:
please can you explain it in lay-man's terms please :(

Imagine that it is raining out, and that there is no wind, so the rain is falling straight down. You have left three identical windows open, one on a vertical wall, one on a flat roof, and one on a slanted roof. The normal to the window on the vertical wall is also perpendicular to the direction the rain is falling, and no rain comes in that window. The normal to the window on the roof is parallel to the direction the rain is falling, and a maximum amount of rain comes in that window. The normal to the window on the slanted roof is at an angle to the direction that the rain is falling (neither parallel nor perpendicular), and an in-between amount of rain come in that window.

Chet
 
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