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Latvian Maritime academy

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u U<br />

n<br />

0<br />

U i max<br />

* sin( i t i<br />

)<br />

i1<br />

<br />

; (6)<br />

i I I *sin( i t <br />

) . (7)<br />

0 i max<br />

i i<br />

The basic task of the investigation of the processes in air gap is the determination of the currents in<br />

the machine windings at a changing operation mode (space oscillation of the rotor) that requires the<br />

solution of the system of equations of emf balance in the electrical circuits of the machine. The<br />

complexity and accuracy of the investigation and the mathematical model as well usually increase with<br />

the increasing of the number of factors taken into account and depend on the types of these factors and<br />

methods of the investigation. All the equations in the system are in the relative units or p.u. system with<br />

equal resistances of the mutual inductance and magnetization forces [7, 10].<br />

The mathematical model of induction motor in d, q, 0 - axes.<br />

(10)<br />

dcd<br />

ucd<br />

rci<br />

cd<br />

cq;<br />

dt<br />

dcq<br />

ucq<br />

rci<br />

cq<br />

cd ;<br />

dt<br />

dpd<br />

u<br />

pd<br />

rpi<br />

pd<br />

pq<br />

k<br />

;<br />

dt<br />

dpq<br />

u<br />

pq<br />

rpi<br />

pq<br />

pd<br />

k<br />

<br />

(11)<br />

dt<br />

The flux linkages for all the loops of the machine in d, q 0 - axes contain only the constant<br />

inductivities not depending on time:<br />

x i x i ;<br />

<br />

cd<br />

cq<br />

c cd<br />

x i<br />

c cq<br />

x<br />

ad<br />

ad<br />

i<br />

pd<br />

pq;<br />

x i x i ;<br />

(12)<br />

<br />

pd<br />

pq<br />

x<br />

ad<br />

i<br />

cd<br />

ad cq<br />

x<br />

p pd<br />

. pipq The equation of motion is shown by Formula 13.<br />

d<br />

J M out<br />

M c<br />

dt<br />

. (13)<br />

where: J- is the moment of inertia of the rotor and load mechanism;<br />

M out – rotating torque on the shaft;<br />

M c – resistive torque.<br />

When the rotor is oscillating the kinetic energy is converted into the energy of electromagnetic field<br />

and vice versa. In this case along with the constant component M out 0 the rotating torque of the motor<br />

contains also the torques of the harmonic components M out ν .<br />

M<br />

<br />

M M cos( t<br />

)<br />

out out 0<br />

out m<br />

. (14)<br />

<br />

The electromagnetic torque of the motor is related to the magnetic flux with the equation<br />

M CI<br />

2s<br />

cos<br />

2s<br />

;<br />

(15)<br />

where: С- is a constructive constant of electric motor;<br />

13

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