The primary
ignition is so called as it forms the first part of the
ignition circuit. The primary circuit is used to provide the
initial stage towards the secondarys High Tension (HT)
output.
The primary circuit has evolved from the basic contact
breaker points and condenser, to the distributorless and
coil per cylinder systems in common use today. The basic
origin of all of these systems evolves around the magnetic
inductance principal. The only system to differ from this
principal is capacitive discharge, whose operation will be
detailed in a later topic.
This principle is based
around a magnetic field (or flux) being produced when the
coil's earth circuit is completed by either the contacts or
the amplifier providing the coil negative terminal with a
path to earth. When this circuit is complete, a magnetic
field is produced and builds until the coil's magnetic field
becomes maximised or saturated. At the predetermined point
of ignition, the coil's earth is removed and the magnetic
field or flux collapses across the coils 250 to 350 primary
windings, which in turn induces a voltage of 200 to 350
Volts.
This induced voltage will
be determined by the following factors:
- The number of turns in
the coils primary winding
- The strength of the
magnetic field
- The rate of collapse,
which is determined by the speed of the switching of the
earth path
The number of turns within
the coils primary is preset from manufacture, however the
strength of the magnetic field which is proportionate to the
current within the circuit and the speed of the switching,
can be seen in Fig 1.0
Figure 1.0
The current
within the electronic ignition example shown sharply rises
to 6 Amps, at which point the current is held until the
earth circuit is removed. The switching speed can be seen by
the angle of the vertical line at the end of the trace, any
delay or slow switching will be seen as a sloping line. Any
compromise in the switching speed will result in a lower
induced voltage.
The height of the induced
voltage line can be seen in Fig 1.1, in this particular
instance its maximum voltage is 326 Volts. This is a result
of the magnetic flux passing quickly across the coils
primary windings. It is important to test this voltage as a
low secondary HT output could result from a low primary
voltage.
Figure 1.1
Dwell Period
Dwell is measured as an
angle: with contact ignition, the points gap determines the
dwell angle. The definition of contact ignition dwell is:
‘the number of degrees of distributor rotation with the
contacts in the closed position’. As an example, a 4
cylinder engine will have a dwell of approximately 45
degrees, which is 50% of one cylinders complete primary
cycle.
Figure 1.2
One of the many
compromises with contact ignition is the fact that the coils
saturation time will reduce with increasing engine speed. In
the illustration shown in Fig 1.2, the engine is running at
approximately 1000 rpm and the points are closed for 16.3
milliseconds. This results in an induced voltage of 286.3
Volts. As the engine speed is increased to 3000 rpm the
coils available time to fully ‘saturate’ will be reduced
pro-rata. Illustration Fig 1.3 shows that the time available
to charge the coil has now been reduced to 5.6 milliseconds.
As a result, the induced voltage has been reduced to 275.4
Volts and the coils HT output reduced accordingly.
Figure 1.3
The dwell
period on an engine with electronic ignition is controlled
by the current limiting circuit within the amplifier or
Electronic Control Module (ECM). The dwell on a variable
dwell or constant energy system will be seen to expand as
the engine speed increases, compensating for the shorter
time period.
The term ‘constant energy’
refers to the available voltage produced by the coil. This,
regardless of engine speed, will remain constant as opposed
to contact ignition where an increase in engine speed means
the contacts are closed for a shorter time period. The coils
saturation time can be seen in Fig 1.4, where the time
available to saturate the coil is a constant 3.0
milliseconds regardless of the engine speed. The saturation
time is considerably lower than that of a contact system due
to the coils supply voltage being approximately double that
of a ballasted contact system and the coils primary
resistance approximately halved. This will result in a far
higher current, saturating the coil with amperage that would
not be possible on a contact system.
Figure 1.4
As with all
electrical circuits it is important for the technician to
check the condition of the earth circuit, this cannot
however be done by simply checking for good continuity using
a multimeter. As an example, imagine an earth wire that has
broken and is down to the last strand of copper wire. When
testing for continuity it will show next to zero resistance,
pass a current along the wire and the result is a different
matter. This simple example shows the importance of testing
any switching circuit's earth path with the aid of an
oscilloscope. An ideal earth would show an almost flat line,
however in practical terms the voltage may creep up as high
as 0.3 Volts. An old electrical law stated that we can loose
up to 0.5 Volts on any live circuit while the earth must
remain below 0.25 Volts. In all practicality, common sense
must prevail so try to minimise the dynamic resistance in
any important earth return circuit.
Figure 1.5
In Fig 1.5 we
can see that while the coils earth circuit is complete (the
length of the dwell period) there is a small volt drop that
increases as the current builds, in this example the circuit
is increasing in current until the earth is removed. A poor
earth will result in an increase in height to the earth
‘ramps’ and a decision must be made as to whether the earth
circuit requires and remedial rectification.
All the example waveforms
used were recorded using a
PC based automotive oscilloscope loaned by
Pico . Other
manufacturers' equipment will have different voltage ranges
but the resultant picture should be very similar. Please
remember that using a higher voltage range will result in
the waveform appearing to have a lower amplitude, although
the overall voltage will be the same.