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Latvian Maritime academy

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the machine, combination and technological harmonics. The latter are caused by the technological<br />

parameters - axis misalignment of the rotor and stator, tapering and ellipse form of rotor, eccentricity of<br />

the stator bore, defects of the bearing units.<br />

The mathematical description of the magnetic field in the air gap of electric machine<br />

The investigation of the influence of the above mentioned defects of bearing units on the magnetic<br />

field of induction machine was based on the calculation of stationary magnetic field system of the electric<br />

machine.<br />

<br />

rotH<br />

<br />

<br />

divB<br />

0 ,<br />

<br />

<br />

B H<br />

where:<br />

H - the intensity of magnetic field;<br />

- density of electrical current;<br />

B - the induction of magnetic field;<br />

- the magnetic permeability of steel<br />

The Poisson equation mathematical description is considered for the calculation of three-dimension<br />

stationary magnetic field [8]:<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

Ay<br />

<br />

y x<br />

<br />

<br />

<br />

z<br />

A<br />

<br />

x z<br />

<br />

<br />

<br />

<br />

<br />

Az<br />

y<br />

x<br />

where:<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

z<br />

Ax<br />

<br />

x y<br />

<br />

<br />

<br />

<br />

<br />

Az<br />

x<br />

A<br />

<br />

y<br />

z<br />

y<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

y<br />

A<br />

<br />

z<br />

z<br />

<br />

<br />

<br />

<br />

<br />

Ax<br />

y<br />

y<br />

Az<br />

<br />

x x<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

z<br />

Ay<br />

<br />

x x<br />

<br />

<br />

<br />

y<br />

<br />

<br />

<br />

<br />

<br />

<br />

A<br />

z<br />

x<br />

Az<br />

y<br />

<br />

<br />

x<br />

<br />

<br />

<br />

y<br />

<br />

<br />

<br />

z<br />

<br />

(1)<br />

, (2)<br />

A x , A y , A z , x , y , z<br />

– the components of the vector magnetic potential and current density<br />

vector along axes x, y, z correspondingly.<br />

On the basis of the system of pre-set currents and magnetic parameters of different space sectors it is<br />

necessary to calculate the space distribution of vector A, meeting the equations of the system (2) and<br />

boundary conditions of the space size.<br />

The task of calculation of the magnetic field is solved minimizing the functional:<br />

F <br />

<br />

V<br />

<br />

1<br />

<br />

<br />

<br />

<br />

B<br />

0<br />

x<br />

<br />

By<br />

1<br />

BxdBx<br />

Ax<br />

<br />

x<br />

<br />

BydBy<br />

<br />

<br />

<br />

0<br />

1<br />

A <br />

y<br />

<br />

y<br />

<br />

<br />

<br />

B<br />

0<br />

z<br />

<br />

<br />

BzdBz<br />

Az<br />

z<br />

dV.<br />

<br />

<br />

<br />

(3)<br />

For the minimization of functional (3) the investigated size is divided into the set of finite elements.<br />

The finite element is selected as a tetrahedron.<br />

Minimum of functional (3) is found solving the equations system:<br />

16

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