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  • In this lecture, we will discuss about various issues related to the design of structural systems from damping perspective specially for materials with damping index, n > 2
  • Consider a beam subjected to pure bending and having a symmetric cross-section with respect to y and z axes as shown in the figure below.

Design for Enhanced Material Damping - Mechanical Engineering

Following simple theory of bending one can write

Design for Enhanced Material Damping - Mechanical Engineering

where Mx= bending moment amplitude at the section, t = depth of the beam, Design for Enhanced Material Damping - Mechanical Engineering maximum bending stress amplitude at the section (i.e., in the fibre at a distance t/2 from the neutral axis), and  ax= bending stress amplitude in the fibre at a distance from the neutral axis where the width of the beam is b(y). The maximum elastic energy stored in the beam for a complete cycle of vibration may be expressed as

Design for Enhanced Material Damping - Mechanical Engineering

where l = length of the beam and E = Young's modulus. Substituting eqn. (11.1) in eqn. (11.2), we obtain

Design for Enhanced Material Damping - Mechanical Engineering

Using the damping-stress amplitude relationship, we get the energy dissipated per cycle from the entire beam as

Design for Enhanced Material Damping - Mechanical Engineering

Hence, the overall loss factor  Design for Enhanced Material Damping - Mechanical Engineering may be written as

 

Design for Enhanced Material Damping - Mechanical Engineering
 

Design for Enhanced Material Damping - Mechanical Engineering

 

Note  Design for Enhanced Material Damping - Mechanical Engineering , the endurance strength against fatigue is introduced for nondimensionalization of the maximum stress.

the first factor on the right-hand side, namely,  Design for Enhanced Material Damping - Mechanical Engineering depends only on the material properties, and is therefore called the material factor.

 

The second factor, i.e.Design for Enhanced Material Damping - Mechanical Engineering is governed by the bending stress distribution along the beam length. This is called the longitudinal stress distribution factor.

 

The third factor, namely,  Design for Enhanced Material Damping - Mechanical Engineering depends only on the crosssection shape and is referred to as the cross-sectional shape factor

 

For the same material and loading condition, different cross sections result in varying values of and, hence, of ns . The following table shows the value of Bcfor three different cross-sections, each having the same depth t,

Design for Enhanced Material Damping - Mechanical Engineering

It should be noted that, for n= 2 , Bc = 2 for all the cross-sections since, for uniaxial loading of a hysteretic material. Design for Enhanced Material Damping - Mechanical Engineering . Any section having more material away from the neutral axis has a better damping capacity than a section in which most of the material is near the neutral axis.

Based on the expression of overall loss factor, it can be inferred that another way to increase the same is by increasing the maximum stress at the outer layers. Indeed, it has been shown that by using a series of cylindrical inserts one can enhance damping. If the inserts are made of high damping material the effect is further enhanced.

 

Design for Enhanced Material Damping - Mechanical Engineering

 

The method of enhancing damping capacity of a structure by high-damping inserts can be extended to design composite materials with high-damping spherical inclusions, which has a good balance of stiffness and damping. Composites of viscoelastic materials with suitable choices for relaxation times of the constituents can also be designed, which can maintain high damping over a wide frequency range.

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