A planar lamina is defined as a figure (a closed set) D of a finite area in a plane, with some mass m.2
This is useful in calculating moments of inertia or center of mass for a constant density, because the mass of a lamina is proportional to its area. In a case of a variable density, given by some (non-negative) surface density function ρ ( x , y ) , {\displaystyle \rho (x,y),} the mass m {\displaystyle m} of the planar lamina D is a planar integral of ρ over the figure:3
The center of mass of the lamina is at the point
where M y {\displaystyle M_{y}} is the moment of the entire lamina about the y-axis and M x {\displaystyle M_{x}} is the moment of the entire lamina about the x-axis:
with summation and integration taken over a planar domain D {\displaystyle D} .
Find the center of mass of a lamina with edges given by the lines x = 0 , {\displaystyle x=0,} y = x {\displaystyle y=x} and y = 4 − x {\displaystyle y=4-x} where the density is given as ρ ( x , y ) = 2 x + 3 y + 2 {\displaystyle \rho \ (x,y)\,=2x+3y+2} .
For this the mass m {\displaystyle m} must be found as well as the moments M y {\displaystyle M_{y}} and M x {\displaystyle M_{x}} .
Mass is m = ∬ D ρ ( x , y ) d x d y {\displaystyle m=\iint _{D}\rho (x,y)\,dx\,dy} which can be equivalently expressed as an iterated integral:
The inner integral is:
Plugging this into the outer integral results in:
Similarly are calculated both moments:
with the inner integral:
which makes:
and
Finally, the center of mass is
Atkins, Tony; Escudier, Marcel (2013), "Plane lamina", A Dictionary of Mechanical Engineering (1 ed.), Oxford University Press, doi:10.1093/acref/9780199587438.001.0001, ISBN 9780199587438, retrieved 2021-06-08 9780199587438 ↩
"Planar Laminae", WolframAlpha, retrieved 2021-03-09 https://www.wolframalpha.com/examples/mathematics/geometry/plane-geometry/planar-laminae/ ↩
"Lamina". MathWorld. Retrieved 2021-03-09. https://mathworld.wolfram.com/Lamina.html ↩