Double Integrals - application to centre of mass.

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Discussion Overview

The discussion centers on the application of double integrals in calculating the center of mass (C.O.M) for two-dimensional objects, contrasting it with the approach used for three-dimensional bodies. Participants explore the necessity of double integrals in the context of continuous mass distributions and varying densities.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant states that the C.O.M for a system of particles can be expressed as a sum for discrete masses and transitions to a continuous distribution using integrals.
  • Another participant points out the confusion between 2D and 3D contexts, emphasizing that the transition from discrete to continuous requires integration over area or volume, thus necessitating double or triple integrals.
  • A later reply clarifies that for a planar object with a density function, the C.O.M is calculated using double integrals, questioning the need for double integrals when single integrals are used for solid bodies.
  • Another participant highlights that the double integral represents integration over two dimensions (dx and dy), while in three dimensions, it extends to include dz, reinforcing the need for dimensionality in the integration process.

Areas of Agreement / Disagreement

Participants express differing views on the necessity and interpretation of double integrals in the context of C.O.M calculations, indicating that the discussion remains unresolved regarding the clarity and application of these concepts.

Contextual Notes

There is an implicit assumption that the density may vary across the object, which influences the need for double integrals. The discussion also reflects a potential misunderstanding of dimensionality in the context of mass distribution.

CAF123
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I know that for a system of particles, the x, y and z coordinates of the centre of mass are given by [tex](\frac{1}{M} \sum_{i = 1}^{n} m_i x_i, \frac{1}{M} \sum_{i = 1}^{n} m_i y_i,\frac{1}{M} \sum_{i = 1}^{n} m_i z_i).[/tex]
For a solid body, we can treat this like a continuous distribution of matter of little mass elements [itex]dm.[/itex]The above becomes [tex](\frac{1}{M} \int x dm,\frac{1}{M} \int y dm,\frac{1}{M} \int z dm).[/tex]
My question is: I also have a definition of centre of mass using the double integral, that is, for the x coordinate say, [tex]x_{com} = \frac{1}{M} \int\int x \rho\, dA,[/tex] where [itex]dm = \rho\, dA[/itex] for 2 dimensional objects.
Why do we need the double integral?

As an aside, I also have in my notes that the area of a region R, [itex]\small Area(R) = \int\int_R dA,[/itex] but I also know that the volume of space below a curve [itex]z = f(x,y)[/itex] in a region [itex]R[/itex] is given by [itex]\int\int_R f(x,y) dA.[/itex] Just to check: The reason why the former describes an area, while the latter a volume is because we have some projection up the z axis, ie f(x,y).

Many thanks
 
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Your question is a little confusing. At times you are talking about 3 dimensions, other times 2 dimensions.

In any case, using the sum over discrete masses being treated as points, space dimensions don't play a role. Your going from discrete to continuous misses the point in that dm = ρdA (2-d) or dm = ρdV (3-d) cannot be viewed as a 1-d integral.

Therefore when talking about real objects, spatially spread out, it is necessary to integrate over the area (2-d) or volume (3-d), so the integral is 2 or 3 dimensional.
 
Last edited:
Ok thanks.
For a planar object with density [itex]\rho(x,y)[/itex], the C.O.M is given by, [tex](\frac{1}{M} \int\int x\,\rho\, dA, \frac{1}{M} \int\int y\,\rho\, dA).[/tex]
If this object is two dimensional, why the need for a double integral?. In my post previously, the C.O.M coordinates for a solid body (3D) were given as single integrals?As far as I understand from my text, the reason is to do with the density not being uniform in the former case?
 
The essentail point is that the integral with respect to dA means the integral over dxdy.
In three dimensions dV=dxdydz. When you use dm, it is an abstraction - you need to convert to ρdA or ρdV.
 

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