Moments of Inertia (Composite Areas)      Click here for Parallel Axis Theorem

 

 

Key Concepts:  A composite area is one that can be partitioned into a collection of known areas such as rectangles, triangles, trapezoids, and circles as well as voids of the same shapes.  Voids are taken as negative contributions. 

 

 

In a Nutshell:  The strategy to calculate the moment of inertia for a composite area is:

 

First

Identify each part, its area, its centroid, and its centroidal axes.

Second

Obtain the moment of inertia for each part (by calculation or by table).

Third

Apply the parallel axis theorem if needed to transfer from the centroidal

axes to the desired parallel axes.

Fourth

Sum the contribution for each individual part as shown in the table below.

 

 

 

Calculation of Areas, First Moment, and Moments of Inertia

Area, A

 A  =  Σ Ai  =  A1 ± A2 ± A3 ± . . . .

First Moment  ybar A

ybar A = y1bar A1 ± y2bar A2 ± y3bar A3 ± . . . .

Second Moment,   Iyy

Iyy  =   Iyy1 ± Iyy2 ± Iyy3 ± . . . .

Second Moment,   Izz

Izz  =   Izz1 ± Izz2 ± Izz3 ± . . . .

Polar Moment,   IP

IP  =   IP1 ± IP2 ± IP3 ± . . . .

 

 

Note the negative signs appearing in the table above apply with voids.  As an example, the

cross-hatched composite area on the left can be partitioned into two separate rectangular areas designated as 1 and 2 in the figure on the right.  Another option would be to consider a large rectangular area encompassing 1 and 2 and then subtract rectangles above and below 2.

 

 

                  

 

Click here for an example.

 



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