Licchavi Lyceum

ll

Licchavi Lyceum

Winding Factor in Alternator

The winding factor is an important concept in the analysis and design of an alternator (synchronous generator). It accounts for the effect of distribution of windings and short-pitching (chording) on the generated EMF. Since practical windings are not concentrated in a single slot and are often short-pitched, the actual induced EMF is less than the ideal EMF. The winding factor helps in quantify this reduction.

Definition of Winding Factor

The winding factor (\(k_w\)) is defined as the ratio of the actual induced EMF in the winding to the EMF that would be induced if all conductors were concentrated in one slot and were full-pitched.

\[
k_w = \frac{\text{Actual EMF}}{\text{Maximum possible EMF}}
\]

Components of Winding Factor

The winding factor is the product of two factors:

\[
k_w = k_p \times k_d
\]

  • \(k_p\) = pitch factor (chording factor)
  • \(k_d\) = distribution factor (breadth factor)

Pitch Factor (Chording Factor)

The pitch factor accounts for the effect of short-pitching of the coil.

If a coil is short-pitched by an angle \(\alpha\), then

\[
k_p = \cos\left(\frac{\alpha}{2}\right)
\]

where

  • \(\alpha\) = chording angle (electrical degrees)

Key Points

  • For full-pitch winding, \(\alpha = 0\), so
    \[
    k_p = 1
    \]
  • For short-pitch winding, \(k_p < 1\)

Short-pitching reduces certain harmonics and improves waveform quality.

Distribution Factor (Breadth Factor)

The distribution factor accounts for the distribution of conductors in
multiple slots per pole per phase.

\[
k_d = \frac{\sin\left(\frac{m\beta}{2}\right)}{m \sin\left(\frac{\beta}{2}\right)}
\]

where

  • \(m\) = number of slots per pole per phase
  • \(\beta\) = slot angle (electrical degrees)

Key Points

  • If all conductors are concentrated in one slot, \(k_d = 1\)
  • In distributed windings, \(k_d < 1\)

Overall Winding Factor

\[
k_w = k_p \times k_d
\]

Since both \(k_p\) and \(k_d\) are less than or equal to 1,

\[
k_w < 1
\]

Typical values:

\[
k_w \approx 0.85 \text{ to } 0.95
\]

EMF Equation of Alternator

The generated EMF per phase in an alternator is given by

\[
E = 4.44 f \phi T k_w
\]

  • \(E\) = induced EMF per phase
  • \(f\) = frequency
  • \(\phi\) = flux per pole
  • \(T\) = number of turns per phase
  • \(k_w\) = winding factor

Importance of Winding Factor

The winding factor is important because it:

  • Determines the actual EMF generated
  • Affects the efficiency and performance of the alternator
  • Helps in harmonic reduction
  • Improves the waveform of generated voltage

Advantages of Short-Pitch and Distributed Windings

  • Reduction of harmonics
  • Improvement in sinusoidal waveform
  • Reduction in copper usage
  • Better machine performance

Important Points

  • \(k_w = k_p \times k_d\)
  • \(k_p = \cos(\alpha/2)\)
  • \(k_d = \dfrac{\sin(m\beta/2)}{m\sin(\beta/2)}\)
  • \(k_w < 1\)
  • EMF equation:
    \[
    E = 4.44 f \phi T k_w
    \]