Double-motor-driven spatial motion vibration crusher and parameter determination method thereof
A technology of space movement and dual-machine drive, applied in complex mathematical operations, electrical digital data processing, CAD numerical modeling, etc., can solve problems such as low crushing efficiency, high processing costs, and equipment failures, and achieve improved crushing and production efficiency , improve synchronization stability and improve service life
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Embodiment 1
[0192] In this case study h 1 , h 2 Influence on the system, introduce parameter η, defined as η=h 2 / h 1 , where h 1 is the distance between the center of mass of the pendulum and the midpoint of the line connecting the centers of rotation of the two exciters, h 2 is the distance between the center of mass of the body and the center of mass of the pendulum. Parameters of the assumed vibration system: M 1 =550kg, M 2 =1600kg, m 0 = 30kg, l 0 = h 3 =0.3m,J ψx =J ψy =500kg·m 2 , J ψz =300kg·m 2 , r=0.15m, k x =k y =k z =10KN / m,k 1θ =k 2θ =10KN / m.
[0193] (a)h 1 The effect of and η on the stable phase difference
[0194] figure 2 Indicates the stable phase difference curve of the system. It can be seen from the figure that at h 1 Under changing conditions, the stable phase difference of the system is not affected by η, that is, the system is in the three cases (h 1 =0.4~0.6), the stable phase difference 2α is approximately 0°, and the two exciters move ...
Embodiment 2
[0206] In order to judge the correctness of the differential equations derived in the previous section, and to initially study the possible kinematics and dynamics of the space-moving two-machine-driven single pendulum system, this example uses the fourth-order Runge-Kutta program to simulate the vibration system. The parameters in the simulation program are the same as those in the numerical analysis of the previous example. This example will give 4 groups of simulations.
[0207] (a) h 1 =0.4m, simulation under the condition of η=1.3
[0208] Figure 7 Indicates the simulation results of group A. from Figure 7 It can be seen from (a) that when the system starts to work, since the two exciters are identical, the acceleration of the two motors is the same. When the system reaches synchronous operation, the speed of the two motors is stable. At time 40s, motor 2 was disturbed by π / 6, and the rotational speeds of the two motors fluctuated, but eventually returned to stabi...
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