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 (\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).
For a solid body, we can treat this like a continuous distribution of matter of little mass elements dm.The above becomes (\frac{1}{M} \int x dm,\frac{1}{M} \int y dm,\frac{1}{M} \int z dm).
My question is: I also have a definition of centre of mass using the double integral, that is, for the x coordinate say, x_{com} = \frac{1}{M} \int\int x \rho\, dA, where dm = \rho\, dA 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, \small Area(R) = \int\int_R dA, but I also know that the volume of space below a curve z = f(x,y) in a region R is given by \int\int_R f(x,y) dA. 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
For a solid body, we can treat this like a continuous distribution of matter of little mass elements dm.The above becomes (\frac{1}{M} \int x dm,\frac{1}{M} \int y dm,\frac{1}{M} \int z dm).
My question is: I also have a definition of centre of mass using the double integral, that is, for the x coordinate say, x_{com} = \frac{1}{M} \int\int x \rho\, dA, where dm = \rho\, dA 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, \small Area(R) = \int\int_R dA, but I also know that the volume of space below a curve z = f(x,y) in a region R is given by \int\int_R f(x,y) dA. 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