Polar moment of inertia/polar radius of gyration via integration

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The discussion focuses on calculating the polar moment of inertia and polar radius of gyration for a given area with respect to point P. The equations provided include Jp = Ix + Iy, with Ix and Iy defined as integrals involving y^2 and x^2, respectively. A user expresses difficulty in performing the integration for Ix and seeks clarification on how to express y and dA in terms of the independent variable. Another participant suggests using the boundaries of the shape to define the width as a function of height, leading to the formulation of dA as the difference between the right and left boundaries multiplied by dy. The integration of y^2 dA is to be conducted within the specified limits to find the desired values.
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Homework Statement



Determine the polar moment of inertia and the polar radius of gyration of the shaded area shown with respect to point P.

http://imgur.com/8Kc1S

Homework Equations



Jp = Ix + Iy
Ix = &int y^2dA
Iy = &int X^2dA

The Attempt at a Solution



A = 2(a/2)(a) + (2)(1/2)(a/2)(a) = 3a^2/2

Jp = Ix + Iy

Ix = &int y^2dA = ? I am having trouble with this next step. If someone could please help me with it and explain to me what's suppose to integrated I would be eternally grateful

I have 2 &int a-0
 
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Firstly be warned are specific to planar objects of unit area or density 1/area.

Integrating y^2 dA involves expressing y and dA in terms of your independent variable (variable of integration) and its differential.

Looking at your region (a trapazoid?) it would appear that your best bet is to express the width at a point as a function of height i.e. express left and right line boundaries in terms of x as a function of y.

Left boundary x =f(y)= p y + q,
Right boundary x = g(y) = r y + s.

You are basically, in the Riemann sum, slicing the object up into horizontal strips with thickness dy and width x_right - x_left = g(y)-f(y), and so its area is:

dA = [g(y)-f(y)] dy

With this integrate y^2 dA between the appropriate limits.
 

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