Finding the Moment of Inertia for a Rectangular Sheet

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SUMMARY

The moment of inertia (MOI) for a rectangular sheet with dimensions 2A (horizontal) and B (vertical) around the z-axis at the midpoint (0,0) is determined using the parallel axis theorem. The formula I = Icm + mr² is essential, where Icm is the moment of inertia about the center of mass and r is the distance from the center of mass to the axis of rotation. For part a, the MOI calculation involves integrating over the mass distribution, while for part b, the MOI is zero since the axis of rotation coincides with the center of mass, resulting in I = 0 + m(0) = 0.

PREREQUISITES
  • Understanding of moment of inertia concepts
  • Familiarity with the parallel axis theorem
  • Basic knowledge of integration techniques in physics
  • Ability to apply geometric properties to physical systems
NEXT STEPS
  • Study the derivation of moment of inertia for various geometric shapes
  • Learn about the application of the parallel axis theorem in different contexts
  • Explore integration methods for calculating moments of inertia
  • Investigate the impact of mass distribution on rotational dynamics
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Students in physics or engineering, particularly those studying mechanics, as well as educators looking to enhance their understanding of rotational motion and moment of inertia calculations.

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Homework Statement


The horizontal side (x-axis) is length 2A and the vertical side (y-axis at x=+-A) is length B. The mass is uniform throughout the sheet so that the center of mass is at the center of the rectangle. What is the moment of inertia for. the rotation around the z-axis at the midpoint of the horizontal side, coordinate (0,0) in terms of A,B and/or mass? The z-axis at the center of mass (hint: use parallel axis)?

Homework Equations


I=Icm+mr^2 where Icm is the center of mass moment and r is the distance to center of mass.

The Attempt at a Solution


For part a, the moment of inertia for a point mass is just I=mr^2, so since the center of mass is (B/2) away from the axis, then I=m*(B/2)^2. However, shouldn't we use parallel axis for part a and not part b, in contrary to the hint for part b?
For part b, the moment of inertia would just be zero? This is because lcm=0 as the axis is at the center of mass and r=0 as the point is also at the center of mass, so I=Icm+mr^2=0+m(0)=0.

Is this the correct way to get both or did I miss something?
 
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For moments of inertia the geometry of the object is important. Mass elements that are further from the axis of rotation have a greater impact on the total, and elements closer have less of an impact. Because the contributions vary as the square of the distance you can't just lump the mass at the center of gravity and use the point mass formula on it. You'll have to do the integration over the object.

Once you've established the MOI about one axis though, you can use the parallel axis theorem to "move it" to any parallel axis.
 
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