MEL’NICK V.M.

 

NATIONAL TECHNICAL UNIVERSITY OF UKRAINE "IGOR SIKORSKY KYIV POLYTECHNIC INSTITUTE"


MANIFESTATION OF THE SELECTIVITY EFFECT OF THE QUANTUM OF KINEMATIC AND ACOUSTIC DISTURBANCES

 

An integrating gyroscope is intended for measuring the turning angle of the aircraft in relation to the measuring (ingoing) axis of the device. Unlike the angle rate sensor, it does not contain a spring, and the functions of damper are performed by a liquid-and-static constituent of the gimbal.

The equations of the first and second approximations can be obtained from the corresponding equations of ÄÓÑÓ, if we can take up in them -

      

In other words

                      (1)

                      (2)

The solution of these equations for the synchronous and asynchronous harmonic oscillations of the aircraft can be obtained from the previously obtained results. For the synchronous oscillations of the fuselage - are expressions and, for the asynchronous oscillations of the aircraft - are expressions  and  :

                                                                                         (3)

    

     

                           (4)

where            1,2,3.

The second approximation is  written down analogically for the synchronous and asynchronous tossing.

From the given correlations it is following, that at the compatible action of kinematics and acoustic inciting on the device , even in the first approximation it is possible to find out the systematic drift of the initial signal of the gyroscope. It takes place at the equality of frequencies of kinematic and acoustic inciting, in other words at the implementation of  condition .  Systematic drift of the axis of the device takes place both at synchronous and asynchronous tossing of the aircraft fuselage [1, 2].

The stable constituents in the right part of the expressions (3) and (4) are of great practical interest. The stable value of the initial signal of the device will equal

;  

We will find out the stable constituent  C.  Averaging in time will be denoted by the symbol. Then in the right part of the expression (4) we will distinguish the stable values, in other words we will carry out the following procedure -

As a result we have for synchronous oscillations -

                                              (5)

Analogical for asynchronous oscillations -

    

                                         (6)