SELF

90

S.B. Karavashkin, O.N. Karavashkina

3. 1D homogeneous elastic lumped system with equal longitudinal and transverse stiffness coefficients

This model can be helpful in studying the problems reduced to the infinitesimally thin rods, homogeneous, isotropic materials and so on. The typical form of the model is shown in Fig. 2. As we proved in the theorem, in this case we can disregard the angle alphacut.gif (839 bytes)   in the modelling system of differential equations, so the system will take the following form:

fig2.gif (3931 bytes)

Fig. 2. The calculation scheme of 1D homogeneous elastic line having a bend at the kth element with the bend angle alphacut.gif (839 bytes) and equal coefficients of longitudinal and transverse stiffnesses

for the x-component

(8)

and for the y-component

(9)

where psi.gif (848 bytes) is the angle of an external force inclination to the axis x, and F(t) = F0Image539.gif (923 bytes) is the external force acting on the start of line.

Using the results presented in [20], we can write the solutions for (8) and (9).

At the subcritical band (periodical vibration regime) at omegacut.gif (838 bytes) < omegacut.gif (838 bytes)0

for the x-component

(10)

for the y-component

(11)

where Image542.gif (959 bytes), Image543.gif (1041 bytes), i = 1, 2, 3, ....

At the overcritical band (aperiodical vibration regime) at  omegacut.gif (838 bytes) > omegacut.gif (838 bytes)0

for the x-component

(12)

for the y-component

(13)

where Image438.gif (1028 bytes).

At the critical frequency (critical vibration regime) at  omegacut.gif (838 bytes) = omegacut.gif (838 bytes)0  

for the x-component

(14)

for the y-component

(15)

Contents: / 86 / 87 / 88 / 89 / 90 / 91 / 92 / 93 / 94 / 95 / 96 / 97 / 98 / 99 / 100 /

Hosted by uCoz