Electrical Machines · DC Machines

Losses & Efficiency in DC Machines

Dr. Mithun Mondal BITS Pilani, Hyderabad Campus Electrical Machines

Demonstrative Video

Losses in DC Machines

losses dc
Losses Dc
Copper Losses:

Generally occurs due to current in the various windings:
\[\left.\begin{array}{ll}\mathrm{Armature~copper~loss}=I_{a}^{2}R_{a}\cdots3-6\%\\\mathrm{Shunt~field~copper~loss}&=I_{sh}^{2}R_{sh}\\\mathrm{Series~field~copper~loss}&=I_{se}^{2}R_{se}\end{array}\right\}\mathrm{1-5\%}\]

Additionally loss due to brush contact resistance enclosed in armature copper loss

Iron Losses:

Loss within the armature due its rotation within the magnetic field of the poles.

\[\text{Hysteresis loss}=K_hB_{max}^{1.6}fV\\\text{Eddy Current loss}=K_eB_{max}^2f^2V\]

Mechanical (Rotational) Losses

3-15%

  • Friction: in bearings, brushes, etc.

  • Windage: air friction of rotating coil

Losses rely on the speed of the machine.

Stray Losses:

1% of FL Output Power

Miscellaneous losses occurs due to

  • Distortion of flux because of armature reaction

  • Short circuit currents in the coil, undergoing commutation

Very difficult to determine a reasonable value is assigned

Constant Losses:

  • Iron losses

  • Mechanical losses

  • Shunt field losses

Variable Losses:

  • Copper loss in armature

  • Copper loss in series field

\[\boxed{\mathrm{Total~losses}=\mathrm{Constant~Losses~+~Variable~Losses}}\]
SECTION 01

Power Flow in DC Machines

power flow
Power Flow
SECTION 02

Power Stages and Efficiency

dcgen power
Dcgen Power
SECTION 03

Condition for Maximum Efficiency

\[\begin{aligned} \mbox{Generator output} & =VI\\ \mbox{Generator input} & =\mbox{output+losses} =VI+I_{a}^{2}R_{a}+W_{c}\\ & =VI+I_{a}^{2}R_{a}+W_{c}\\ & =VI+\left(I+I_{sh}\right)^{2}R_{a}+W_{c} \end{aligned}\]
is negligible as compared to load current, then
Key Concepts
\[\begin{aligned} \dfrac{d}{dI}\left(\dfrac{IR_{a}}{V}+\dfrac{W_{c}}{VI}\right) & = 0\\ \dfrac{R_a}{V} - \dfrac{W_c}{VI^2} & = 0\\ I^2R_a & = W_c \end{aligned}\]
\[\begin{aligned} I^2R_a & = W_c\\ &\boxed{I = \sqrt{\dfrac{W_c}{R_a}}} \end{aligned}\]
\[\boxed{\mbox{Variable loss = constant loss}}\]
Now, efficiency is maximum when denominator is minimum i.e. when
SECTION 04

Efficiency Curve Vs Load Current

efficiency dc
Efficiency Dc