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Planar lamina

In mathematics, a planar lamina (or plane lamina[1]) is a figure representing a thin, usually uniform, flat layer of the solid. It serves also as an idealized model of a planar cross section of a solid body in integration.

Planar laminas can be used to determine moments of inertia, or center of mass of flat figures, as well as an aid in corresponding calculations for 3D bodies.

Definition

Basically, 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   the mass   of the planar lamina D is a planar integral of ρ over the figure:[3]

 

Properties

The center of mass of the lamina is at the point

 

where   is the moment of the entire lamina about the y-axis and   is the moment of the entire lamina about the x-axis:

 
 

with summation and integration taken over a planar domain  .

Example

 

Find the center of mass of a lamina with edges given by the lines     and   where the density is given as  .

For this the mass   must be found as well as the moments   and  .

Mass is   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

 

References

  1. ^ 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
  2. ^ "Planar Laminae", WolframAlpha, retrieved 2021-03-09
  3. ^ "Lamina". MathWorld. Retrieved 2021-03-09.

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This article has multiple issues Please help improve it or discuss these issues on the talk page Learn how and when to remove these template messages This article needs additional citations for verification Please help improve this article by adding citations to reliable sources Unsourced material may be challenged and removed Find sources Planar lamina news newspapers books scholar JSTOR October 2021 Learn how and when to remove this template message This article may be too technical for most readers to understand Please help improve it to make it understandable to non experts without removing the technical details October 2015 Learn how and when to remove this template message Learn how and when to remove this template message In mathematics a planar lamina or plane lamina 1 is a figure representing a thin usually uniform flat layer of the solid It serves also as an idealized model of a planar cross section of a solid body in integration Planar laminas can be used to determine moments of inertia or center of mass of flat figures as well as an aid in corresponding calculations for 3D bodies Contents 1 Definition 2 Properties 3 Example 4 ReferencesDefinition EditBasically 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 r x y displaystyle rho x y the mass m displaystyle m of the planar lamina D is a planar integral of r over the figure 3 m D r x y d x d y displaystyle m iint D rho x y dx dy Properties EditThe center of mass of the lamina is at the point M y m M x m displaystyle left frac M y m frac M x m right 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 M y lim m n i 1 m j 1 n x i j r x i j y i j D D D x r x y d x d y displaystyle M y lim m n to infty sum i 1 m sum j 1 n x ij rho x ij y ij Delta D iint D x rho x y dx dy M x lim m n i 1 m j 1 n y i j r x i j y i j D D D y r x y d x d y displaystyle M x lim m n to infty sum i 1 m sum j 1 n y ij rho x ij y ij Delta D iint D y rho x y dx dy with summation and integration taken over a planar domain D displaystyle D Example Edit 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 r 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 r x y d x d y displaystyle m iint D rho x y dx dy which can be equivalently expressed as an iterated integral m x 0 2 y x 4 x 2 x 3 y 2 d y d x displaystyle m int x 0 2 int y x 4 x 2x 3y 2 dy dx The inner integral is y x 4 x 2 x 3 y 2 d y displaystyle int y x 4 x 2x 3y 2 dy 2 x y 3 y 2 2 2 y y x 4 x displaystyle qquad left left 2xy frac 3y 2 2 2y right right y x 4 x 2 x 4 x 3 4 x 2 2 2 4 x 2 x x 3 x 2 2 2 x displaystyle qquad left 2x 4 x frac 3 4 x 2 2 2 4 x right left 2x x frac 3 x 2 2 2 x right 4 x 2 8 x 32 displaystyle qquad 4x 2 8x 32 Plugging this into the outer integral results in m x 0 2 4 x 2 8 x 32 d x 4 x 3 3 4 x 2 32 x x 0 2 112 3 displaystyle begin aligned m amp int x 0 2 left 4x 2 8x 32 right dx amp left left frac 4x 3 3 4x 2 32x right right x 0 2 amp frac 112 3 end aligned Similarly are calculated both moments M y D x r x y d x d y x 0 2 y x 4 x x 2 x 3 y 2 d y d x displaystyle M y iint D x rho x y dx dy int x 0 2 int y x 4 x x 2x 3y 2 dy dx with the inner integral y x 4 x x 2 x 3 y 2 d y displaystyle int y x 4 x x 2x 3y 2 dy 2 x 2 y 3 x y 2 2 2 x y y x 4 x displaystyle qquad left left 2x 2 y frac 3xy 2 2 2xy right right y x 4 x 4 x 3 8 x 2 32 x displaystyle qquad 4x 3 8x 2 32x which makes M y x 0 2 4 x 3 8 x 2 32 x d x x 4 8 x 3 3 16 x 2 x 0 2 80 3 displaystyle begin aligned M y amp int x 0 2 4x 3 8x 2 32x dx amp left left x 4 frac 8x 3 3 16x 2 right right x 0 2 amp frac 80 3 end aligned and M x D y r x y d x d y x 0 2 y x 4 x y 2 x 3 y 2 d y d x 0 2 x y 2 y 3 y 2 y x 4 x d x 0 2 2 x 3 4 x 2 40 x 80 d x x 4 2 4 x 3 3 20 x 2 80 x x 0 2 248 3 displaystyle begin aligned M x amp iint D y rho x y dx dy int x 0 2 int y x 4 x y 2x 3y 2 dy dx amp int 0 2 xy 2 y 3 y 2 Big y x 4 x dx amp int 0 2 2x 3 4x 2 40x 80 dx amp left left frac x 4 2 frac 4x 3 3 20x 2 80x right right x 0 2 amp frac 248 3 end aligned Finally the center of mass is M y m M x m 80 3 112 3 248 3 112 3 5 7 31 14 displaystyle left frac M y m frac M x m right left frac frac 80 3 frac 112 3 frac frac 248 3 frac 112 3 right left frac 5 7 frac 31 14 right References Edit 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 Planar Laminae WolframAlpha retrieved 2021 03 09 Lamina MathWorld Retrieved 2021 03 09 Retrieved from https en wikipedia org w index php title Planar lamina amp oldid 1049386266, wikipedia, wiki, book, books, library,

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