AeroElectric-List Digest Archive

Fri 01/19/18


Total Messages Posted: 13



Today's Message Index:
----------------------
 
     1. 08:00 AM - Re: diode on starter contactor (Robert L. Nuckolls, III)
     2. 08:08 AM - Re: diode on starter contactor (Robert L. Nuckolls, III)
     3. 08:45 AM - Re: diode on starter contactor (Ken Ryan)
     4. 08:57 AM - Re: diode on starter contactor (Bob Verwey)
     5. 09:14 AM - Re: diode on starter contactor (C&K)
     6. 09:22 AM - Re: diode on starter contactor (Charlie England)
     7. 09:42 AM - Re: diode on starter contactor (Eric Jones)
     8. 10:03 AM - Re: diode on starter contactor (Ken Ryan)
     9. 10:32 AM - Re: diode on starter contactor (Robert L. Nuckolls, III)
    10. 10:43 AM - Re: diode on starter contactor (Robert L. Nuckolls, III)
    11. 10:53 AM - Re: diode on starter contactor (Robert L. Nuckolls, III)
    12. 12:05 PM - suppression diodes (Alec Myers)
    13. 07:13 PM - Re: diode on starter contactor (Sebastien)
 
 
 


Message 1


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    Time: 08:00:45 AM PST US
    From: "Robert L. Nuckolls, III" <nuckolls.bob@aeroelectric.com>
    Subject: Re: diode on starter contactor
    At 04:37 PM 1/18/2018, you wrote: > >I=99m trying to work out why a diode has *any* >significant effect on release time compared to a >tranzorb or similar, and if it did, why you might care. >Also, why should it have any effect on relay life reduction =85? >My skeptical self needs help to get beyond >merely =9Cmore expensive therefore must be better=9D. When mechanical contacts are opened, an electric arc forms in the air gap. With low voltages and currents, the fire may be small, but it is never zero. In one of my articles, I mentioned and experiment when a microswitch was biased up with a dry cell and resistor. The contacts were observed through a microscope in the dark (the side was opened up on the switch for the experiment). Even at these very low power levels, a BLUE arc could be observed. The temperature of blue is HOT. This suggests that no matter what the power level, every opening even will transfer molecules of metal between contacts. Again, not a lot of metal but never zero. As energy levels go up and particularly at higher voltages, the intensity and DURATION of the arcing event increases. This is an expected condition. Relays are designed to meet life cycle ratings at specific power levels and circuit characteristics by adjusting contact material, closing forces, opening velocities, opening gaps, etc. Conditions are important . . . switches and relays will have AC, DC and LAMP ratings applied to their service life limits. https://goo.gl/CPtPYJ If you've ever tried to do any stick-welding, you understand the need for (1) making initial cold contact, (2) breaking that contact to form an arc, then maintaining an optimum distance between rod and work-piece to achieve a SUSTAINED fire at a temperature conducive to the TRANSFER of metal from rod to work-piece. If the contacts of a switch or relay do not spread fast enough, wide enough and with sufficient thermal mass in contacts, then the TRANSFER of metal will exceed that which meets design goals for service life. This lays the groundwork for a notion that relay contacts will accelerate open at some rate which is a function of spring, mass and decay of the magnetic field which was originally applied to close the contacts. It's easily demonstrated that rate of decay for this magnetic field is strongly influenced by the choice of suppression for energy stored in the coil at the time it is de-energized. A totally open-circuit coil is the fastest, but transient voltage during field collapse is greatest. You can drive a coil with a current limited source and the throw a dead short across the coil, reducing its excitation current to zero thus initiating the contact opening sequence. In this condition, the field collapse transient voltage will be zero and time to decay will be a whole lot longer. Hence, there is a range of decay rates offered by the array of suppression techniques. I've have yet to discover a paper that describes the behavior of relay magnetic holding force in detail . . . many papers that jump to an 'obvious' conclusion that if decay rate in the coil is extended by factors of 10 or more, then opening velocity of the contacts is similarly depressed. What I observed (in 45 years of herding electrons in airplanes and conducting numerous relay and switch failure studies) is that as a relay closes, the CONTACTS CLOSE before the magnetic armature BOTTOMS OUT. There is a spring rate associated with this extra motion that sets the contact closed holding force. This leads us to the idea that as the magnetic field in the device decays, there is a period of time from first motion the of armature off the bottomed-out position until closing force on the contacts drops to zero and they begin to move. This means that there is a GROWING AIR GAP in the magnetic circuit holding the contacts closed. This air gap has a profound suppressing effect on that magnetic force. It's an effect that grossly over-rides the decay rate of the magnetic from the coil. Magnetic decay rate does indeed affect drop-out time for the relay . . . this was demonstrated in the data collected during my bench-top experiments. Decay rate adds a time delay between de-energizing of the coil and first opening of the contacts. However, by the time the contacts see first motion, the magnetic air gap is established and growing. The air gap has much more control over contact acceleration than does coil current. Hence, the duration of arc between spreading contacts showed only a slight difference between diode-suppressed and non-suppressed contactor. The case for 'supper suppressors' is further weakened by the fact that starter and battery contactors on our airplanes are considered very busy if they get a few operations per week. The average light aircraft flies 50 hours a year. If you install switches and relay rated for tens of thousands of operations, it stands to reason that benefits gained by going-the-extra-mile on coil suppression yields no measurable benefit. Then, there is the study of contact erosion during closure as influenced by the physics of the switched circuit. This is due to arcing that occurs during contact BOUNCE. Many closures and openings per operation . . . much smaller gap during the bounce . . . but exceedingly unfriendly to relay life under some conditions. But that's a totally different story . . . Bob . . .


    Message 2


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    Time: 08:08:04 AM PST US
    From: "Robert L. Nuckolls, III" <nuckolls.bob@aeroelectric.com>
    Subject: Re: diode on starter contactor
    At 07:09 PM 1/18/2018, you wrote: >Last year I put a lighter AGM battery in my aircraft and moved it to >the firewall along with the master contactor and made some new >diodes for the contactors (one was broken). Saved about 4 pounds in >wiring alone! Only problem afterwards was that if the battery was >even slightly down sometimes the starter would turn a split second >and then nothing. Repeated attempts usually ended up with the >starter eventually running fine until the engine started. Putting a >voltmeter on the starter confirmed that the problem was a lack of >power to the starter, not the starter itself. I had a battery >problem later on and replaced the battery, no change. Thinking I had >messed up the starter contactor while tightening nuts on it I >swapped it out, no change. At this point I started to suspect my >diode so I disconnected it: Problem gone! I suspect I installed it >backwards. Going to make the new one with clear shrinkwrap tubing so >it can't happen again. If your diode is installed backwards, it will conduct HARD while the starter button is depressed. Plastic diodes generally smoke for a few seconds and split, some will literally explode. I've seen a few cases where they simply fused short and tripped the starter control circuit breaker. If removing the diode cured your problem, then it probably was 'backwards'. Do you have a breaker or fuse on your starter control line? That shorted condition should have opened the circuit protection. Bob . . .


    Message 3


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    Time: 08:45:25 AM PST US
    From: Ken Ryan <keninalaska@gmail.com>
    Subject: Re: diode on starter contactor
    I'm confused. It seems like you are now saying that because the relays are rated for far more cycles than they will ever see, there is no reason to bother with diodes. Sent from my Android. Sorry Steve. On Jan 19, 2018 7:06 AM, "Robert L. Nuckolls, III" < nuckolls.bob@aeroelectric.com> wrote: > At 04:37 PM 1/18/2018, you wrote: > > > I=C3=A2=82=AC=84=A2m trying to work out why a diode has *any* signi ficant effect on > release time compared to a tranzorb or similar, and if it did, why you > might care. > Also, why should it have any effect on relay life reduction ? > My skeptical self needs help to get beyond merely =C3=A2=82=AC=C5=93mo re expensive > therefore must be better=C3=A2=82=AC . > > > When mechanical contacts are opened, an electric > arc forms in the air gap. With low voltages and > currents, the fire may be small, but it is never > zero. In one of my articles, I mentioned and experiment > when a microswitch was biased up with a dry cell > and resistor. The contacts were observed > through a microscope in the dark (the side was opened > up on the switch for the experiment). > > Even at these very low power levels, a BLUE arc > could be observed. The temperature of blue is > HOT. This suggests that no matter what the power > level, every opening even will transfer molecules > of metal between contacts. > > Again, not a lot of metal but never zero. > > As energy levels go up and particularly > at higher voltages, the intensity and DURATION > of the arcing event increases. This is an expected > condition. Relays are designed to meet life cycle > ratings at specific power levels and circuit > characteristics by adjusting contact material, > closing forces, opening velocities, opening > gaps, etc. Conditions are important . . . switches > and relays will have AC, DC and LAMP ratings > applied to their service life limits. > > https://goo.gl/CPtPYJ > > If you've ever tried to do any stick-welding, you > understand the need for (1) making initial cold > contact, (2) breaking that contact to form an > arc, then maintaining an optimum distance between > rod and work-piece to achieve a SUSTAINED fire > at a temperature conducive to the TRANSFER > of metal from rod to work-piece. > > If the contacts of a switch or relay do not spread > fast enough, wide enough and with sufficient > thermal mass in contacts, then the TRANSFER of > metal will exceed that which meets design goals > for service life. > > This lays the groundwork for a notion that relay > contacts will accelerate open at some rate which is > a function of spring, mass and decay of the > magnetic field which was originally applied to > close the contacts. > > It's easily demonstrated that rate of decay for > this magnetic field is strongly influenced by > the choice of suppression for energy stored in > the coil at the time it is de-energized. > > A totally open-circuit coil is the fastest, but > transient voltage during field collapse is greatest. > You can drive a coil with a current limited source > and the throw a dead short across the coil, reducing > its excitation current to zero thus initiating > the contact opening sequence. In this condition, > the field collapse transient voltage will be zero > and time to decay will be a whole lot longer. > Hence, there is a range of decay rates offered by > the array of suppression techniques. > > I've have yet to discover a paper that describes > the behavior of relay magnetic holding force > in detail . . . many papers that jump to an > 'obvious' conclusion that if decay rate in > the coil is extended by factors of 10 or more, > then opening velocity of the contacts is similarly > depressed. > > What I observed (in 45 years of herding electrons > in airplanes and conducting numerous relay and > switch failure studies) is that as a relay closes, > the CONTACTS CLOSE before the magnetic armature > BOTTOMS OUT. There is a spring rate associated > with this extra motion that sets the contact > closed holding force. > > This leads us to the idea that as the magnetic > field in the device decays, there is a period > of time from first motion the of armature off > the bottomed-out position until closing force > on the contacts drops to zero and they begin > to move. This means that there is a GROWING > AIR GAP in the magnetic circuit holding the > contacts closed. > > This air gap has a profound suppressing effect > on that magnetic force. It's an effect that > grossly over-rides the decay rate of the magnetic > from the coil. > > Magnetic decay rate does indeed affect drop-out > time for the relay . . . this was demonstrated in > the data collected during my bench-top experiments. > Decay rate adds a time delay between de-energizing > of the coil and first opening of the contacts. > However, by the time the contacts see first motion, > the magnetic air gap is established and growing. > > The air gap has much more control over contact > acceleration than does coil current. Hence, the > duration of arc between spreading contacts showed > only a slight difference between diode-suppressed > and non-suppressed contactor. > > The case for 'supper suppressors' is further > weakened by the fact that starter and battery > contactors on our airplanes are considered very > busy if they get a few operations per week. > The average light aircraft flies 50 hours > a year. If you install switches and relay rated > for tens of thousands of operations, it stands to > reason that benefits gained by going-the-extra-mile > on coil suppression yields no measurable benefit. > > Then, there is the study of contact erosion during > closure as influenced by the physics of the switched > circuit. This is due to arcing that occurs during > contact BOUNCE. Many closures and openings per > operation . . . much smaller gap during the bounce . . . > but exceedingly unfriendly to relay life under > some conditions. > > But that's a totally different story . . . > > > Bob . . . >


    Message 4


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    Time: 08:57:08 AM PST US
    From: Bob Verwey <bob.verwey@gmail.com>
    Subject: Re: diode on starter contactor
    Does the risk not lie in having contacts that weld together or overheat? On 19 Jan 2018 6:49 PM, "Ken Ryan" <keninalaska@gmail.com> wrote: > I'm confused. It seems like you are now saying that because the relays ar e > rated for far more cycles than they will ever see, there is no reason to > bother with diodes. > > Sent from my Android. Sorry Steve. > > On Jan 19, 2018 7:06 AM, "Robert L. Nuckolls, III" < > nuckolls.bob@aeroelectric.com> wrote: > >> At 04:37 PM 1/18/2018, you wrote: >> >> >> I=C3=A2=82=AC=84=A2m trying to work out why a diode has *any* sign ificant effect on >> release time compared to a tranzorb or similar, and if it did, why you >> might care. >> Also, why should it have any effect on relay life reduction ? >> My skeptical self needs help to get beyond merely =C3=A2=82=AC=C5=93m ore expensive >> therefore must be better=C3=A2=82=AC . >> >> >> >> When mechanical contacts are opened, an electric >> arc forms in the air gap. With low voltages and >> currents, the fire may be small, but it is never >> zero. In one of my articles, I mentioned and experiment >> when a microswitch was biased up with a dry cell >> and resistor. The contacts were observed >> through a microscope in the dark (the side was opened >> up on the switch for the experiment). >> >> Even at these very low power levels, a BLUE arc >> could be observed. The temperature of blue is >> HOT. This suggests that no matter what the power >> level, every opening even will transfer molecules >> of metal between contacts. >> >> Again, not a lot of metal but never zero. >> >> As energy levels go up and particularly >> at higher voltages, the intensity and DURATION >> of the arcing event increases. This is an expected >> condition. Relays are designed to meet life cycle >> ratings at specific power levels and circuit >> characteristics by adjusting contact material, >> closing forces, opening velocities, opening >> gaps, etc. Conditions are important . . . switches >> and relays will have AC, DC and LAMP ratings >> applied to their service life limits. >> >> https://goo.gl/CPtPYJ >> >> If you've ever tried to do any stick-welding, you >> understand the need for (1) making initial cold >> contact, (2) breaking that contact to form an >> arc, then maintaining an optimum distance between >> rod and work-piece to achieve a SUSTAINED fire >> at a temperature conducive to the TRANSFER >> of metal from rod to work-piece. >> >> If the contacts of a switch or relay do not spread >> fast enough, wide enough and with sufficient >> thermal mass in contacts, then the TRANSFER of >> metal will exceed that which meets design goals >> for service life. >> >> This lays the groundwork for a notion that relay >> contacts will accelerate open at some rate which is >> a function of spring, mass and decay of the >> magnetic field which was originally applied to >> close the contacts. >> >> It's easily demonstrated that rate of decay for >> this magnetic field is strongly influenced by >> the choice of suppression for energy stored in >> the coil at the time it is de-energized. >> >> A totally open-circuit coil is the fastest, but >> transient voltage during field collapse is greatest. >> You can drive a coil with a current limited source >> and the throw a dead short across the coil, reducing >> its excitation current to zero thus initiating >> the contact opening sequence. In this condition, >> the field collapse transient voltage will be zero >> and time to decay will be a whole lot longer. >> Hence, there is a range of decay rates offered by >> the array of suppression techniques. >> >> I've have yet to discover a paper that describes >> the behavior of relay magnetic holding force >> in detail . . . many papers that jump to an >> 'obvious' conclusion that if decay rate in >> the coil is extended by factors of 10 or more, >> then opening velocity of the contacts is similarly >> depressed. >> >> What I observed (in 45 years of herding electrons >> in airplanes and conducting numerous relay and >> switch failure studies) is that as a relay closes, >> the CONTACTS CLOSE before the magnetic armature >> BOTTOMS OUT. There is a spring rate associated >> with this extra motion that sets the contact >> closed holding force. >> >> This leads us to the idea that as the magnetic >> field in the device decays, there is a period >> of time from first motion the of armature off >> the bottomed-out position until closing force >> on the contacts drops to zero and they begin >> to move. This means that there is a GROWING >> AIR GAP in the magnetic circuit holding the >> contacts closed. >> >> This air gap has a profound suppressing effect >> on that magnetic force. It's an effect that >> grossly over-rides the decay rate of the magnetic >> from the coil. >> >> Magnetic decay rate does indeed affect drop-out >> time for the relay . . . this was demonstrated in >> the data collected during my bench-top experiments. >> Decay rate adds a time delay between de-energizing >> of the coil and first opening of the contacts. >> However, by the time the contacts see first motion, >> the magnetic air gap is established and growing. >> >> The air gap has much more control over contact >> acceleration than does coil current. Hence, the >> duration of arc between spreading contacts showed >> only a slight difference between diode-suppressed >> and non-suppressed contactor. >> >> The case for 'supper suppressors' is further >> weakened by the fact that starter and battery >> contactors on our airplanes are considered very >> busy if they get a few operations per week. >> The average light aircraft flies 50 hours >> a year. If you install switches and relay rated >> for tens of thousands of operations, it stands to >> reason that benefits gained by going-the-extra-mile >> on coil suppression yields no measurable benefit. >> >> Then, there is the study of contact erosion during >> closure as influenced by the physics of the switched >> circuit. This is due to arcing that occurs during >> contact BOUNCE. Many closures and openings per >> operation . . . much smaller gap during the bounce . . . >> but exceedingly unfriendly to relay life under >> some conditions. >> >> But that's a totally different story . . . >> >> >> >> >> Bob . . . >> >


    Message 5


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    Time: 09:14:15 AM PST US
    Subject: Re: diode on starter contactor
    From: C&K <yellowduckduo@gmail.com>
    For all intents and purposes the diode ONLY protects the switch that controls the relay. So it does improve system reliability. Ken On 19/01/2018 11:44 AM, Ken Ryan wrote: > I'm confused. It seems like you are now saying that because the relays > are rated for far more cycles than they will ever see, there is no > reason to bother with diodes.


    Message 6


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    Time: 09:22:05 AM PST US
    Subject: Re: diode on starter contactor
    From: Charlie England <ceengland7@gmail.com>
    I think y'all are a bit confused on what the diodes actually do. The diode across the relay coil is there to protect the controlling *switch's* low current contacts; not the relay contacts. Now, since TANSTAFL (there's no such thing as a free lunch), the downside (of questionable significance) to the diode being in the circuit is that it *can* slow the collapse of the magnetic field in the relay, leading some to think (evidenced by the link to back-to-back zeners) that it puts the *relay* contacts at more risk. Not to speak for Bob, but his latest post(s) address that slowing of the magnetic field collapse (of questionable significance), and tell us that his testing has shown that with most relays, the contacts don't actually start to separate until after that slowed magnetic field decay isn't having any influence. So....The bottom line is that the diode *is* needed to protect *switch* contacts, and its presence has *minimal to zero* real world impact on the *relay's* contacts. The takeaway is that you do need the diode, and nothing more elaborate than a standard diode is needed. Those of us who made our living playing with these components have an easy time seeing what he's describing. It might serve you well to visit some appliance/electrical repair facility & talk them out of a couple of open frame relays so you can play with them & see what he's describing. On 1/19/2018 10:56 AM, Bob Verwey wrote: > Does the risk not lie in having contacts that weld together or overheat? > > On 19 Jan 2018 6:49 PM, "Ken Ryan" <keninalaska@gmail.com > <mailto:keninalaska@gmail.com>> wrote: > > I'm confused. It seems like you are now saying that because the > relays are rated for far more cycles than they will ever see, > there is no reason to bother with diodes. > > Sent from my Android. Sorry Steve. > > On Jan 19, 2018 7:06 AM, "Robert L. Nuckolls, III" > <nuckolls.bob@aeroelectric.com > <mailto:nuckolls.bob@aeroelectric.com>> wrote: > > At 04:37 PM 1/18/2018, you wrote: >> <alec@alecmyers.com <mailto:alec@alecmyers.com>> >> >> Im trying to work out why a diode has *any* significant >> effect on release time compared to a tranzorb or similar, and >> if it did, why you might care. >> Also, why should it have any effect on relay life reduction ? >> My skeptical self needs help to get beyond merely more >> expensive therefore must be better . > > > When mechanical contacts are opened, an electric > arc forms in the air gap. With low voltages and > currents, the fire may be small, but it is never > zero. In one of my articles, I mentioned and experiment > when a microswitch was biased up with a dry cell > and resistor. The contacts were observed > through a microscope in the dark (the side was opened > up on the switch for the experiment). > > Even at these very low power levels, a BLUE arc > could be observed. The temperature of blue is > HOT. This suggests that no matter what the power > level, every opening even will transfer molecules > of metal between contacts. > > Again, not a lot of metal but never zero. > > As energy levels go up and particularly > at higher voltages, the intensity and DURATION > of the arcing event increases. This is an expected > condition. Relays are designed to meet life cycle > ratings at specific power levels and circuit > characteristics by adjusting contact material, > closing forces, opening velocities, opening > gaps, etc. Conditions are important . . . switches > and relays will have AC, DC and LAMP ratings > applied to their service life limits. > > https://goo.gl/CPtPYJ > > If you've ever tried to do any stick-welding, you > understand the need for (1) making initial cold > contact, (2) breaking that contact to form an > arc, then maintaining an optimum distance between > rod and work-piece to achieve a SUSTAINED fire > at a temperature conducive to the TRANSFER > of metal from rod to work-piece. > > If the contacts of a switch or relay do not spread > fast enough, wide enough and with sufficient > thermal mass in contacts, then the TRANSFER of > metal will exceed that which meets design goals > for service life. > > This lays the groundwork for a notion that relay > contacts will accelerate open at some rate which is > a function of spring, mass and decay of the > magnetic field which was originally applied to > close the contacts. > > It's easily demonstrated that rate of decay for > this magnetic field is strongly influenced by > the choice of suppression for energy stored in > the coil at the time it is de-energized. > > A totally open-circuit coil is the fastest, but > transient voltage during field collapse is greatest. > You can drive a coil with a current limited source > and the throw a dead short across the coil, reducing > its excitation current to zero thus initiating > the contact opening sequence. In this condition, > the field collapse transient voltage will be zero > and time to decay will be a whole lot longer. > Hence, there is a range of decay rates offered by > the array of suppression techniques. > > I've have yet to discover a paper that describes > the behavior of relay magnetic holding force > in detail . . . many papers that jump to an > 'obvious' conclusion that if decay rate in > the coil is extended by factors of 10 or more, > then opening velocity of the contacts is similarly > depressed. > > What I observed (in 45 years of herding electrons > in airplanes and conducting numerous relay and > switch failure studies) is that as a relay closes, > the CONTACTS CLOSE before the magnetic armature > BOTTOMS OUT. There is a spring rate associated > with this extra motion that sets the contact > closed holding force. > > This leads us to the idea that as the magnetic > field in the device decays, there is a period > of time from first motion the of armature off > the bottomed-out position until closing force > on the contacts drops to zero and they begin > to move. This means that there is a GROWING > AIR GAP in the magnetic circuit holding the > contacts closed. > > This air gap has a profound suppressing effect > on that magnetic force. It's an effect that > grossly over-rides the decay rate of the magnetic > from the coil. > > Magnetic decay rate does indeed affect drop-out > time for the relay . . . this was demonstrated in > the data collected during my bench-top experiments. > Decay rate adds a time delay between de-energizing > of the coil and first opening of the contacts. > However, by the time the contacts see first motion, > the magnetic air gap is established and growing. > > The air gap has much more control over contact > acceleration than does coil current. Hence, the > duration of arc between spreading contacts showed > only a slight difference between diode-suppressed > and non-suppressed contactor. > > The case for 'supper suppressors' is further > weakened by the fact that starter and battery > contactors on our airplanes are considered very > busy if they get a few operations per week. > The average light aircraft flies 50 hours > a year. If you install switches and relay rated > for tens of thousands of operations, it stands to > reason that benefits gained by going-the-extra-mile > on coil suppression yields no measurable benefit. > > Then, there is the study of contact erosion during > closure as influenced by the physics of the switched > circuit. This is due to arcing that occurs during > contact BOUNCE. Many closures and openings per > operation . . . much smaller gap during the bounce . . . > but exceedingly unfriendly to relay life under > some conditions. > > But that's a totally different story . . . > > > Bob . . . > --- This email has been checked for viruses by Avast antivirus software. https://www.avast.com/antivirus


    Message 7


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    Time: 09:42:48 AM PST US
    Subject: Re: diode on starter contactor
    From: Eric Jones <emjones@charter.net>
    I am reluctant to get into another long discussion on the subject of coil suppression but I encourage Googling the various extensive resources on this subject. Note that there are many techniques tuned to specific application on this subject, but three things are true: 1) The use of a simple diode is contraindicated. 2) The use of a simple bidirectional zener is a good way to go. 3) MOVs are a good way to go, but they have a discrete lifetime...I was never comfortable with that. MOVs are usually what fails in surge-suppression computer multi-outlets. One COULD use a zener and a regular diode in series, but a bidirectional zener is polarity insensitive and stone simple. Kilovac and Gigavac both use bidirectional zeners inside their contactors for coil supression. What does these people know that you don't? Eric


    Message 8


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    Time: 10:03:27 AM PST US
    From: Ken Ryan <keninalaska@gmail.com>
    Subject: Re: diode on starter contactor
    Thanks Charlie. That does clear things up for me as to what Bob was saying. I am no longer confused (temporary condition I am sure). Sent from my Android. Sorry Steve. On Jan 19, 2018 8:26 AM, "Charlie England" <ceengland7@gmail.com> wrote: > I think y'all are a bit confused on what the diodes actually do. The diod e > across the relay coil is there to protect the controlling *switch's* low > current contacts; not the relay contacts. Now, since TANSTAFL (there's no > such thing as a free lunch), the downside (of questionable significance) > to the diode being in the circuit is that it *can* slow the collapse of t he > magnetic field in the relay, leading some to think (evidenced by the link > to back-to-back zeners) that it puts the *relay* contacts at more risk. > > Not to speak for Bob, but his latest post(s) address that slowing of the > magnetic field collapse (of questionable significance), and tell us that > his testing has shown that with most relays, the contacts don't actually > start to separate until after that slowed magnetic field decay isn't havi ng > any influence. > > So....The bottom line is that the diode *is* needed to protect *switch* > contacts, and its presence has *minimal to zero* real world impact on the > *relay's* contacts. The takeaway is that you do need the diode, and nothi ng > more elaborate than a standard diode is needed. > > Those of us who made our living playing with these components have an eas y > time seeing what he's describing. It might serve you well to visit some > appliance/electrical repair facility & talk them out of a couple of open > frame relays so you can play with them & see what he's describing. > > On 1/19/2018 10:56 AM, Bob Verwey wrote: > > Does the risk not lie in having contacts that weld together or overheat? > > On 19 Jan 2018 6:49 PM, "Ken Ryan" <keninalaska@gmail.com> wrote: > >> I'm confused. It seems like you are now saying that because the relays >> are rated for far more cycles than they will ever see, there is no reaso n >> to bother with diodes. >> >> Sent from my Android. Sorry Steve. >> >> On Jan 19, 2018 7:06 AM, "Robert L. Nuckolls, III" < >> nuckolls.bob@aeroelectric.com> wrote: >> >>> At 04:37 PM 1/18/2018, you wrote: >>> > >>> >>> I=C3=A2=82=AC=84=A2m trying to work out why a diode has *any* sig nificant effect on >>> release time compared to a tranzorb or similar, and if it did, why you >>> might care. >>> Also, why should it have any effect on relay life reduction ? >>> My skeptical self needs help to get beyond merely =C3=A2=82=AC=C5=93 more expensive >>> therefore must be better=C3=A2=82=AC . >>> >>> >>> >>> When mechanical contacts are opened, an electric >>> arc forms in the air gap. With low voltages and >>> currents, the fire may be small, but it is never >>> zero. In one of my articles, I mentioned and experiment >>> when a microswitch was biased up with a dry cell >>> and resistor. The contacts were observed >>> through a microscope in the dark (the side was opened >>> up on the switch for the experiment). >>> >>> Even at these very low power levels, a BLUE arc >>> could be observed. The temperature of blue is >>> HOT. This suggests that no matter what the power >>> level, every opening even will transfer molecules >>> of metal between contacts. >>> >>> Again, not a lot of metal but never zero. >>> >>> As energy levels go up and particularly >>> at higher voltages, the intensity and DURATION >>> of the arcing event increases. This is an expected >>> condition. Relays are designed to meet life cycle >>> ratings at specific power levels and circuit >>> characteristics by adjusting contact material, >>> closing forces, opening velocities, opening >>> gaps, etc. Conditions are important . . . switches >>> and relays will have AC, DC and LAMP ratings >>> applied to their service life limits. >>> >>> https://goo.gl/CPtPYJ >>> >>> If you've ever tried to do any stick-welding, you >>> understand the need for (1) making initial cold >>> contact, (2) breaking that contact to form an >>> arc, then maintaining an optimum distance between >>> rod and work-piece to achieve a SUSTAINED fire >>> at a temperature conducive to the TRANSFER >>> of metal from rod to work-piece. >>> >>> If the contacts of a switch or relay do not spread >>> fast enough, wide enough and with sufficient >>> thermal mass in contacts, then the TRANSFER of >>> metal will exceed that which meets design goals >>> for service life. >>> >>> This lays the groundwork for a notion that relay >>> contacts will accelerate open at some rate which is >>> a function of spring, mass and decay of the >>> magnetic field which was originally applied to >>> close the contacts. >>> >>> It's easily demonstrated that rate of decay for >>> this magnetic field is strongly influenced by >>> the choice of suppression for energy stored in >>> the coil at the time it is de-energized. >>> >>> A totally open-circuit coil is the fastest, but >>> transient voltage during field collapse is greatest. >>> You can drive a coil with a current limited source >>> and the throw a dead short across the coil, reducing >>> its excitation current to zero thus initiating >>> the contact opening sequence. In this condition, >>> the field collapse transient voltage will be zero >>> and time to decay will be a whole lot longer. >>> Hence, there is a range of decay rates offered by >>> the array of suppression techniques. >>> >>> I've have yet to discover a paper that describes >>> the behavior of relay magnetic holding force >>> in detail . . . many papers that jump to an >>> 'obvious' conclusion that if decay rate in >>> the coil is extended by factors of 10 or more, >>> then opening velocity of the contacts is similarly >>> depressed. >>> >>> What I observed (in 45 years of herding electrons >>> in airplanes and conducting numerous relay and >>> switch failure studies) is that as a relay closes, >>> the CONTACTS CLOSE before the magnetic armature >>> BOTTOMS OUT. There is a spring rate associated >>> with this extra motion that sets the contact >>> closed holding force. >>> >>> This leads us to the idea that as the magnetic >>> field in the device decays, there is a period >>> of time from first motion the of armature off >>> the bottomed-out position until closing force >>> on the contacts drops to zero and they begin >>> to move. This means that there is a GROWING >>> AIR GAP in the magnetic circuit holding the >>> contacts closed. >>> >>> This air gap has a profound suppressing effect >>> on that magnetic force. It's an effect that >>> grossly over-rides the decay rate of the magnetic >>> from the coil. >>> >>> Magnetic decay rate does indeed affect drop-out >>> time for the relay . . . this was demonstrated in >>> the data collected during my bench-top experiments. >>> Decay rate adds a time delay between de-energizing >>> of the coil and first opening of the contacts. >>> However, by the time the contacts see first motion, >>> the magnetic air gap is established and growing. >>> >>> The air gap has much more control over contact >>> acceleration than does coil current. Hence, the >>> duration of arc between spreading contacts showed >>> only a slight difference between diode-suppressed >>> and non-suppressed contactor. >>> >>> The case for 'supper suppressors' is further >>> weakened by the fact that starter and battery >>> contactors on our airplanes are considered very >>> busy if they get a few operations per week. >>> The average light aircraft flies 50 hours >>> a year. If you install switches and relay rated >>> for tens of thousands of operations, it stands to >>> reason that benefits gained by going-the-extra-mile >>> on coil suppression yields no measurable benefit. >>> >>> Then, there is the study of contact erosion during >>> closure as influenced by the physics of the switched >>> circuit. This is due to arcing that occurs during >>> contact BOUNCE. Many closures and openings per >>> operation . . . much smaller gap during the bounce . . . >>> but exceedingly unfriendly to relay life under >>> some conditions. >>> >>> But that's a totally different story . . . >>> >>> >>> >>> >>> Bob . . . >>> >> > > > <https://www.avast.com/sig-email?utm_medium=email&utm_source=link&utm _campaign=sig-email&utm_content=emailclient&utm_term=icon> Virus-free . > www.avast.com > <https://www.avast.com/sig-email?utm_medium=email&utm_source=link&utm _campaign=sig-email&utm_content=emailclient&utm_term=link> > <#m_-9065681909408129575_DAB4FAD8-2DD7-40BB-A1B8-4E2AA1F9FDF2> >


    Message 9


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    Time: 10:32:03 AM PST US
    From: "Robert L. Nuckolls, III" <nuckolls.bob@aeroelectric.com>
    Subject: Re: diode on starter contactor
    At 10:44 AM 1/19/2018, you wrote: >I'm confused. It seems like you are now saying that because the >relays are rated for far more cycles than they will ever see, there >is no reason to bother with diodes. No . . . . I am saying that 'optimized' coil spike suppression has a perhaps a tiny benefit for contactors in heavy usage applications and no benefit in our airplanes (very low duty). Spike suppression is (and always has been) indicated for enhancing LIFE OF THE DEVICE THAT CONTROLS the contactor. E.g. AD against key-switch. The plain-vanilla diodes have been installed on TC aircraft for decades. See item 29 in screenshot of 1969 C172 service manual. Couldn't put my hands on my copy of the Beechjet manual . . . but the little critters are sprinkled about that airplane as well. Emacs! The diode has (1) no practical effect on service life of contactor and (2) demonstrable benefit on service life of the controlling switch . . . Bob . . .


    Message 10


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    Time: 10:43:33 AM PST US
    From: "Robert L. Nuckolls, III" <nuckolls.bob@aeroelectric.com>
    Subject: Re: diode on starter contactor
    At 10:56 AM 1/19/2018, you wrote: >Does the risk not lie in having contacts that weld together or overheat? Contacts 'weld' on closure. The risk of welding begins with deformation of contact surfaces due to combinations of age and service conditions (extra ordinary inrush current), low energizing current. Contact welding can also be a function of unanticipated behaviors due to aircraft wiring. See this study on 'sticking' roll trim relays on the Beechjet: https://goo.gl/QcfSYo Spike suppression on the at-risk relay/contactor has no effect on conditions that promote contact sticking/welding. 'Overheating' contacts are either too small for the service or so badly worn as to degrade conductivity across the contacts. https://goo.gl/1BJP7y Note that this victim of severe overheat still carries remains of its coil suppression diode. This contactor was used to control power to a 3 horsepower, 28v motor used in the air conditioning system of a King Air. The diode was there . . . but the contactor simply got 'tired'. Bob . . .


    Message 11


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    Time: 10:53:23 AM PST US
    From: "Robert L. Nuckolls, III" <nuckolls.bob@aeroelectric.com>
    Subject: Re: diode on starter contactor
    > >Kilovac and Gigavac both use bidirectional zeners inside their >contactors for coil supression. What does these people know that you don't? Not a thing I can see . . . the bidirectional zener performs as advertised. No reason to avoid it or to change it out in favor of an alternative. By the same token, there's no demonstrable benefit for any extra effort to steer clear of the lowly diode that has also performed as advertised in literally billions of applications for a very long time. My complaint is with publications that make sweeping assertions that are demonstrably short on physical evidence or experimental confirmation. Bob . . .


    Message 12


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    Time: 12:05:28 PM PST US
    From: Alec Myers <alec@alecmyers.com>
    Subject: suppression diodes
    on a similar subject to recent discussion, why dont we use a suppression device across the load of the starter contactor (i.e. the motor) to prevent arcing at the contactor contacts?


    Message 13


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    Time: 07:13:22 PM PST US
    From: Sebastien <cluros@gmail.com>
    Subject: Re: diode on starter contactor
    I was wondering the same thing Bob so I had a look, no fuse or breaker in that line. I guess the builder thought it didn't need one since it connects to ground 8(. I think I should install an inline fuse? Thank you, Sebastien On Fri, Jan 19, 2018 at 8:07 AM, Robert L. Nuckolls, III < nuckolls.bob@aeroelectric.com> wrote: > At 07:09 PM 1/18/2018, you wrote: > > Last year I put a lighter AGM battery in my aircraft and moved it to the > firewall along with the master contactor and made some new diodes for the > contactors (one was broken). Saved about 4 pounds in wiring alone! Only > problem afterwards was that if the battery was even slightly down sometimes > the starter would turn a split second and then nothing. Repeated attempts > usually ended up with the starter eventually running fine until the engine > started. Putting a voltmeter on the starter confirmed that the problem was > a lack of power to the starter, not the starter itself. I had a battery > problem later on and replaced the battery, no change. Thinking I had messed > up the starter contactor while tightening nuts on it I swapped it out, no > change. At this point I started to suspect my diode so I disconnected it: > Problem gone! I suspect I installed it backwards. Going to make the new one > with clear shrinkwrap tubing so it can't happen again. > > > If your diode is installed backwards, it will conduct > HARD while the starter button is depressed. Plastic > diodes generally smoke for a few seconds and split, > some will literally explode. I've seen a few cases > where they simply fused short and tripped the starter > control circuit breaker. > > If removing the diode cured your problem, then it > probably was 'backwards'. Do you have a breaker > or fuse on your starter control line? That shorted condition > should have opened the circuit protection. > > > Bob . . . >




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