Statics, Study notes of Statics

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 - Lecture - April 9 , 

• Chap 10.1, 10.2, 10.4, 10.
• Statics - TAM

Announcements

 No class Wednesday April 11

 No office hours for Prof. H-W on Wednesday April 11

Upcoming deadlines:

 Tuesday (4/10)  PL HW 12  Thursday (4/12)  WA 5 due  Monday (4/16)  Mastering Engineering Tutorial 14

Goals and Objectives

• Understand the term “moment” as used in this chapter
• Determine and know the differences between
  • First/second moment of area
  • Moment of inertia for an area
  • Polar moment of inertia
  • Mass moment of inertia
• Introduce the parallel-axis theorem.
• Be able to compute the moments of inertia of composite areas.

Why do they usually not have solid rectangular, square, or circular cross sectional areas? What primary property of these members influences design decisions? Many structural members like beams and columns have cross sectional shapes like an I, H, C, etc. Applications These are aside notes from in- class discussion

 The first moment of the area A with respect to the x-axis is given by  The first moment of the area A with respect to the y-axis is given by  The centroid of the area A is defined as the point C of coordinates and , which satisfies the relation  In the case of a composite area, we divide the area A into parts , , Recap: First moment of an area (centroid of an area)

Terminology: the term moment in this module refers to the mathematical sense of different “measures” of an area or volume.  The zeroth moment is the total mass.  The first moment (a single power of position) gave us the centroid.  The second moment will allow us to describe the “width.”  An analogy that may help: in probability the first moment gives you the mean (the center of the distribution), and the second is the standard deviation (the width of the distribution).

Determine the moment of inertia for the rectangular area shown w.r.t. the centroidal axis 𝑥 ′ .

 Often, the moment of inertia of an area is known for an axis passing through the centroid ; e.g., x’ and y’ :  The moments around other axes can be computed from the known Ix’ and Iy’ :

Parallel axis theorem

Note: the integral over y’ gives zero when done through the centroid axis.

Area Moments of Inertia for common shapes

• If individual bodies making up a composite body have individual areas A and moments of inertia I computed through their centroids, then the composite area and moment of inertia is a sum of the individual component contributions.
• This requires the parallel axis theorem
• Remember:
  • The position of the centroid of each component must be defined with respect to the same origin.
  • It is allowed to consider negative areas in these expressions. Negative areas correspond to holes/missing area. This is the one occasion to have negative moment of inertia.

Moment of inertia of composite

Mass Moment of Inertia

• Mass moment of inertia is the mass property of a rigid body that determines the torque T needed for a desired angular acceleration (𝛼) about an axis of rotation.
• A larger mass moment of inertia around a given axis requires more torque to increase the rotation, or to stop the rotation, of a body about that axis
• Mass moment of inertia depends on the shape and density of the body and is different around different axes of rotation. http://ffden- 2.phys.uaf.edu/webproj/211_fall_2014/Ari el_Ellison/Ariel_Ellison/Angular.html

Mass Moment of Inertia

𝐼𝑧𝑧 = න 𝜌 𝑟 2 𝑑𝑉 𝑇 = 𝐼 𝛼 Mass moment of inertia for a disk: Torque-acceleration relation: where the mass moment of inertia is defined as 𝛼𝑧 𝑟

English units (inches)

Metric units (mm)