Following simple theory of bending one can write
where Mx= bending moment amplitude at the section, t = depth of the beam, 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
where l = length of the beam and E = Young's modulus. Substituting eqn. (11.1) in eqn. (11.2), we obtain
Using the damping-stress amplitude relationship, we get the energy dissipated per cycle from the entire beam as
Hence, the overall loss factor may be written as
Note , the endurance strength against fatigue is introduced for nondimensionalization of the maximum stress.
the first factor on the right-hand side, namely, depends only on the material properties, and is therefore called the material factor.
The second factor, i.e. is governed by the bending stress distribution along the beam length. This is called the longitudinal stress distribution factor.
The third factor, namely, 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,
It should be noted that, for n= 2 , Bc = 2 for all the cross-sections since, for uniaxial loading of a hysteretic material. . 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.
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.