Armature Reaction in a DC Generator
Definition and Magnetic Field Effects of Armature Reaction
Definition: Armature reaction fundamentally describes the interaction between the armature magnetic field and the main field, specifically characterizing how the armature flux influences the main field flux. The armature magnetic field is generated by current-carrying armature conductors, while the main field is excited by magnetic poles. The armature flux exerts two primary effects on the main field flux:
Magnetic Field Distribution in a Two-Pole DC Generator Under No-Load Condition
Consider the two-pole DC generator shown in the figure below. When the generator operates under no-load conditions (i.e., armature current is zero), only the magnetomotive force (MMF) of the main poles exists within the machine. The magnetic flux generated by the main poles' MMF is uniformly distributed along the magnetic axis, which is defined as the centerline between the north and south poles. The arrow in the figure indicates the direction of the main magnetic flux Φₘ. The magnetic neutral axis (or plane) is perpendicular to the axis of this magnetic flux.
The MNA coincides with the geometrical neutral axis (GNA). The brushes of the DC machines are always placed in this axis, and hence this axis is called the axis of commutation.
Magnetic Field Analysis of Current-Carrying Armature Conductors
Consider a scenario where only armature conductors carry current, with no current in the main poles. The current direction is uniform for all conductors under a single pole. The direction of induced current in conductors is determined by Fleming's Right-Hand Rule, while the direction of flux generated by conductors follows the Corkscrew Rule.
Current in left-side armature conductors flows into the paper (denoted by a cross inside a circle). The magnetomotive forces (MMFs) of these conductors combine to generate a downward resultant flux through the armature. Similarly, right-side conductors carry current flowing out of the paper (denoted by a dot inside a circle), with their MMFs also combining to produce downward flux. Thus, MMFs from both sides of the conductors combine such that their resultant flux is directed downward, as indicated by the arrow for armature-conductor-induced flux Φₐ in the figure above.
The figure below illustrates the condition where both field current and armature current act on the conductors simultaneously.
Armature Reaction Effects in Electrical Machines
Under no-load operation, the machine exhibits two magnetic fluxes: armature flux (generated by currents in armature conductors) and field pole flux (produced by main field poles). These fluxes combine to form a resultant flux Φᵣ, as illustrated in the figure above.
When field flux interacts with armature flux, distortion occurs: flux density increases at the upper tip of the N-pole and lower tip of the S-pole, while decreasing at the lower tip of the N-pole and upper tip of the S-pole. The resultant flux shifts in the direction of generator rotation, with the magnetic neutral axis (MNA)—always perpendicular to the resultant flux—moving correspondingly.
Key Effects of Armature Reaction:
