Why are DC generator loops wired in a non-traditional manner?

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SUMMARY

The discussion centers on the wiring configuration of DC generator loops, specifically addressing why multiple loops are connected in a non-traditional manner. In a typical setup, the terminals of each loop are positioned at opposite sides of the armature; however, in practical applications, the ends of the loops are staggered, such as connecting one end at 12 o'clock and the other at 1 o'clock on a clock face. This configuration results in a more consistent rectified DC waveform and affects the voltage generation, leading to a more regular supply of pulses at the brushes. The analysis of voltage generation remains straightforward, but the staggered connection enhances performance.

PREREQUISITES
  • Understanding of DC generator principles
  • Familiarity with armature windings and commutators
  • Knowledge of waveform characteristics in electrical engineering
  • Basic concepts of magnetic fields in generators
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  • Research the impact of armature winding configurations on voltage output
  • Study the function and design of commutators in DC generators
  • Explore the principles of rectification in electrical circuits
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Electrical engineers, students studying generator design, and professionals involved in optimizing DC generator performance will benefit from this discussion.

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Given a simple DC generator with a single loop in the presence of a magnetic field such as the one below, typically, the analysis involves how each rectangular loop's terminal ends up on opposite sides of an armature housing each of the coils.
fig4fwd.gif
The analysis is fairly straightforward to then extend to a second loop positioned perpendicular to the first loop. The result is also a rectified / pulsed DC waveform at the brushes, except there will be a more regular supply of pulses than in the case with one loop. The two coils are connected to a commutator such that opposite ends of each loop's terminals go to opposite ends of the commutator. This is conceptually straightforward as well.

All of this is fine, but in real life, generators with many such armature windings / loops are wired such that the opposite ends of a loop are connected as follows.
commutator.jpg
In other words, given 6 loops, instead of the first loop having one end at 12 o'clock on a clock and the other end at 6 o'clock on a clock, the ends are at 12 o'clock and 1 o'clock. Can someone help me understand why? How does the analysis change, if at all at that point, as far as how much voltage is generated?

Thanks in advanced.
 
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The relevant lecture that shows the origin of the confusion: starting at around 18-20.
 
Most likely this can only be answered by an "old timer". I am making measurements on an uA709 op amp (metal can). I would like to calculate the frequency rolloff curves (I can measure them). I assume the compensation is via the miller effect. To do the calculations I would need to know the gain of the transistors and the effective resistance seen at the compensation terminals, not including the values I put there. Anyone know those values?

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