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2018 | OriginalPaper | Buchkapitel

13. Constant Frequency Voltage Supply of Rotating Field Machines

verfasst von : Jan A Melkebeek

Erschienen in: Electrical Machines and Drives

Verlag: Springer International Publishing

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Abstract

For rotating field machines supplied by a constant frequency supply, there are almost no acceptable means of speed control (and none whatsoever for synchronous machines). This section will mainly focus on starting, accelerating and braking, and speed control will be discussed in later chapter. Pure synchronous machines fed from a constant frequency supply cannot start and accelerate, as should be clear from Chap. 5 in Part 1. However, when starting and accelerating is required, the damper winding of a synchronous machine (which is usually required for stability) can be adapted to give a starting and accelerating torque, operating as an asynchronous machine. When approaching synchronous speed, the DC supply of the field winding can be switched on and the machine will synchronise when the load is not too large. The asynchronous starting, accelerating and braking discussed in the first section below is therefore also important for synchronous machines which are not too large. In the next section, speed control and cascade connections for slip-ring induction motors are reviewed. Other sections discuss the behaviour of rotating field machines at voltage variations and power-electronic voltage control for rotating field machines.

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Fußnoten
1
The inertia varies with the fifth power of the pole pitch, while the rated torque varies with approximately the fourth power of the pole pitch.
 
2
Prove this with the definition of \(P_{nom}=\varOmega _{sy}T_{nom}\) and the expression for \(\tau _{nom}\).
 
3
Prove that, if \(\alpha \) is the ratio between the lowest and highest pole number, the power loss is reduced to a fraction \(\alpha ^{2}+(1-\alpha )^{2}\).
 
4
It can be shown that this self-excitation is in fact a limit cycle of this non-linear system; when a linearised model is used, there is a zero in the origin which corresponds to a non-existing degree of freedom for the amplitudes.
 
5
Note that the URS is used for the primary, while the GRS is used for the secondary.
 
6
As is illustrated, the pull-out torque values are not constant, however.
 
7
Prove the signs of the power flows and explain.
 
8
Note that also a wind turbine with a synchronous machine as generator requires an inverter to adapt the generator output to the grid frequency.
 
9
Why?
 
10
Note that the (pull-out) torque of an induction machine varies with the square of the voltage; a voltage dip to 70% may lead to a maximum torque below the rated torque.
 
11
Prove this.
 
Metadaten
Titel
Constant Frequency Voltage Supply of Rotating Field Machines
verfasst von
Jan A Melkebeek
Copyright-Jahr
2018
DOI
https://doi.org/10.1007/978-3-319-72730-1_13