Electronic ignition systems have many
advantages over breaker point ignition systems.
High Secondary Voltages
Electronic ignition systems can carry the
increased primary current needed to produce the higher secondary system voltages
needed to ignite leaner air/fuel mixtures.
The primary circuit in most breaker point
systems carried 3.5 to 4.0 amperes. When the breaker points opened, this current
tried to arc across the points. Point arcing caused electrolysis and corrosion
on the metal surface of the contacts. When primary current increases above 4
amperes, point life begins to decrease at an increased rate, resulting in every
limited point life. Faster wearing points require extra maintenance and result
in an ever-decreasing dwell period, which in turn decreases the potential
voltage induced in the secondary system. Dwell is the period of time that
current flows through the primary circuit.
Better High-Speed Performance
Another handicap of the old breaker point
system was that as engine speed increased, the dwell time decreased. This, in
turn, decreases the output of the coil. From the ignition coil to generate
maximum secondary voltage, maximum primary current flow must be flowing through
the primary winding before the field is collapsed. In a breaker point system,
the length of time the primary circuit is closed is controlled by the speed of
the breaker cam. This period of time is called dwell angle and is expressed in a
number of degrees of distributor shaft rotation. For example, many V-8 engines
have a dwell angle of 30 degrees during which time the points are closed and
current builds in the primary winding. This dwell angle remains constant
regardless of engine speed; but as engine rpm increases, the actual time, in
seconds, the points are closed decreases. Any increase in engine speed above a
specific rpm reduces the saturation time of the ignition coil, causing the
available voltage to decrease.
This phenomenon is due to the fact that the
current in the coil does not instantaneously reach its maximum value when the
contact points close. Current in the coil must build for several milliseconds
for this value to be reached. At 1,000 rpm, the distributor shaft rotates once
every 0.12 second. Of this time, the points are closed for 0.10 second, or 10
milliseconds, for every cylinder of an 8-cylinder engine. This is sufficient
time for saturation of the primary winding.
When the engine speed increases to 2,000 rpm,
the time that the points are closed for each plug firing is reduced to 5
milliseconds. A dwell period of 5 milliseconds allows the primary current to
build to 3.8 amperes. At 3,000rpm, the dwell period drops to 3.3 milliseconds
and the current drops to 3.2 amperes. The reduced saturation time lowers the
available secondary voltage. This can result in a misfire as there may be less
voltage available than is needed to fire the plug. This increases exhaust
emissions and decreases fuel economy and engine performance.
An electronic ignition system, however, is not
limited by a fixed dwell angle. The system's control unit can vary the on-time
of the primary circuit based on engine speed, load, and temperature. Because
coil primary current levels are not limited by breaker points, low resistant
coils are used in the electronic ignition system. By decreasing the resistance
in the primary circuit, the required saturation time of the coil is greatly
reduced. It takes 10 milliseconds for the current to reach maximum saturation in
a coil with a resistance of 2.6 ohms. In a coil used in electronic ignition
systems, the primary winding can have a resistance as low as 0.5 ohm. This
allows full current to be reached in about 3.4 milliseconds. Because it takes
less time to reach full current, coil saturation can be obtained at much higher
engine speeds. For example, the HEI system developed by General Motors in 1974
is able to generate 35,000 volts at engine speeds above 3,000 rpm. A typical
breaker point system, on the other hand, developed a maximum of 20,000 volts at
1,000 rpm. Above this speed, the voltage dropped off.