MolaKule
Staff member
Physic of the Gap – Spark Plugs, That is! Part II (by permission by the author)
As we stated in Part I, today’s spark plugs operate in a very hostile environment and can continue to operate to over 100,000 miles due to advanced gap materials.
An overview of ignition systems can be found at:
http://www.jetav8r.com/Vision/Ignition/CDI.html
In Part II, we examine the nuances and the timing of events in the spark itself. We will not discuss the spark timing with relation to piston position, which is today determined by various sensors, such as crankshaft sensors and lookup tables in the ECU’s software.
In a typical spark discharge system, the electrical field is increased until the voltage across the electrode gap breaks down the cylinder’s gaseous mixture. The impedance of the gap decreases when a streamer reaches the opposite electrode. Ionizing streamers then give rise to a current which increases rapidly.
There are three stages to this process: The breakdown phase, the arc phase, and the glow discharge phase.
All of these phases happen within window of about 2.0 milliseconds.
In the breakdown phase, the voltage rises until current flows through the ionizing mixture, which can be as high as 200 Amps. But this high current only lasts about 10 nanoseconds. The ionization channel is a cylinder of about 40 micrometers. The temperature in this ionization column gets to 60,000 degrees Kelvin. A shock wave is also created with a pressure of about 250 atmospheres (3, 625 PSI). As the shock or blast wave propagates outward, the temperature and pressure of the ionization channel falls rapidly. The current then drops rapidly to the arc phase.
During the arc phase, the voltage drops to about 150 volts but the current is still up around 100 Amps, and the temperature of the ionization channel drops to about 6,000 degrees Kelvin. The arc increases in size due to heat conduction and mass diffusion. It is during this phase that much of electrode material is eroded away from the center electrode.
A glow discharge period occurs when the current reaches about 300 milliAmps and the temperature drops to 3,000 degrees Kelvin. It is during this phase that most electrode material is eroded away from the center electrode. The glow discharge phase lasts longer than do the previous two phases.
The material eroded away during each spark is very minute, but does add up over time, which is why replacement is necessary. As material is eroded away of course, the plug gap increases.
At about 2 miiliseconds, the current and voltage have decayed to zero.
The total amount of energy supplied to the spark is about 70 milliJoules.
During the breakdown phase, an energy of 10 milliJoules is distributed as follows: Plasma energy – 94%, Heat loss to electrodes – 6%.
During the arc phase, an energy of 10 millijoules is distributed as follows: Plasma energy – 55%, Heat loss to electrodes – 45%.
During the glow phase, an energy of 50 milliJoules is distributed as follows: Plasma energy – 30%, Heat loss to electrodes – 70%.
So, give thanks for this device that works so hard in such a high temperature, high pressure environment.
As we stated in Part I, today’s spark plugs operate in a very hostile environment and can continue to operate to over 100,000 miles due to advanced gap materials.
An overview of ignition systems can be found at:
http://www.jetav8r.com/Vision/Ignition/CDI.html
In Part II, we examine the nuances and the timing of events in the spark itself. We will not discuss the spark timing with relation to piston position, which is today determined by various sensors, such as crankshaft sensors and lookup tables in the ECU’s software.
In a typical spark discharge system, the electrical field is increased until the voltage across the electrode gap breaks down the cylinder’s gaseous mixture. The impedance of the gap decreases when a streamer reaches the opposite electrode. Ionizing streamers then give rise to a current which increases rapidly.
There are three stages to this process: The breakdown phase, the arc phase, and the glow discharge phase.
All of these phases happen within window of about 2.0 milliseconds.
In the breakdown phase, the voltage rises until current flows through the ionizing mixture, which can be as high as 200 Amps. But this high current only lasts about 10 nanoseconds. The ionization channel is a cylinder of about 40 micrometers. The temperature in this ionization column gets to 60,000 degrees Kelvin. A shock wave is also created with a pressure of about 250 atmospheres (3, 625 PSI). As the shock or blast wave propagates outward, the temperature and pressure of the ionization channel falls rapidly. The current then drops rapidly to the arc phase.
During the arc phase, the voltage drops to about 150 volts but the current is still up around 100 Amps, and the temperature of the ionization channel drops to about 6,000 degrees Kelvin. The arc increases in size due to heat conduction and mass diffusion. It is during this phase that much of electrode material is eroded away from the center electrode.
A glow discharge period occurs when the current reaches about 300 milliAmps and the temperature drops to 3,000 degrees Kelvin. It is during this phase that most electrode material is eroded away from the center electrode. The glow discharge phase lasts longer than do the previous two phases.
The material eroded away during each spark is very minute, but does add up over time, which is why replacement is necessary. As material is eroded away of course, the plug gap increases.
At about 2 miiliseconds, the current and voltage have decayed to zero.
The total amount of energy supplied to the spark is about 70 milliJoules.
During the breakdown phase, an energy of 10 milliJoules is distributed as follows: Plasma energy – 94%, Heat loss to electrodes – 6%.
During the arc phase, an energy of 10 millijoules is distributed as follows: Plasma energy – 55%, Heat loss to electrodes – 45%.
During the glow phase, an energy of 50 milliJoules is distributed as follows: Plasma energy – 30%, Heat loss to electrodes – 70%.
So, give thanks for this device that works so hard in such a high temperature, high pressure environment.
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