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nuckolls.bob(at)aeroelect Guest
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Posted: Sat Oct 29, 2011 7:28 am Post subject: RG Batteries: I learned something last night |
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That bench test battery I featured in a posting
a few days ago had not be cap-checked in several years.
The thing is over ten years old and has yielded a
great return on investment.
I did a load test on this battery about a week ago.
It dumped about 300A for 15 seconds at the 70F mark
on the load meter. A value that is less than 1/2 the
as-new capability.
Just for grins, I pulled out the CBAII battery tester.
The bench battery had been on a maintainer for a couple days.
I did a 6A discharge test. The value I use as exemplary
of most of my instrumentation experiments. The battery
delivered 24+ a.h. of useful energy! Going to the
factory data on this battery we see:
http://www.aeroelectric.com/Pictures/Curves/33AH_12V_Capacity_vs_Load.gif
The factory says a 6.6A load will deplete this battery
in about 4 hours . . . or 24+ a.h.
In years past, my teachers modeled the battery as a large
array of cells connected in a series-parallel configuration
with EACH cell offering some finite energy value combined
with it's own source impedance. If you loose 1/2 the cell
in the full-up array, energy drops by 1/2 but source impedance
doubles.
This experiment last night showed that while the source
impedance for the battery had doubled (1/2 the cranking
snort), the total energy available was still almost as-new!
This means that the gazillion itty-bitty cell analogy is not
quite accurate. Those cells can experience a rise in
source impedance while still offering their original
energy capability.
This battery as-new will deliver 9V at over 800A for
15 seconds. This suggests a source impedance of
(12-9)/800 = .004 ohms. It now produces about 300A
so the new source impedance is (12-9)/300 = .010
ohms.
So while the impedance has doubled, the available
energy at 6A loading has been barely affected . . . if
at all. A rise from .004 to .010 ohms source impedance
has little influence on a test load of (12/6)= 2 Ohms.
This argues with any analogy that suggests a "dead"
micro-cell in a battery becomes totally disconnected
from the array. It suggests that individual cells
can demonstrate an ability to store and regurgitate
energy while experiencing an independent and unrelated
rise in source impedance.
This discovery suggests that it is possible for a
battery to meet battery-only-ops requirements while
demonstrating reduced cranking performance. This ol'
dog is still learning . . . and my grey haired bench
test battery is still in service.
Bob . . .
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klehman(at)albedo.net Guest
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Posted: Sun Oct 30, 2011 7:21 am Post subject: RG Batteries: I learned something last night |
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I can report results that seem similar. For a new 9AH dekka vrla battery
discharged at 6 amps (2 ohm resistance) I measure 56 minutes to 11.00
volts or 5.6 AH.
For a 6+ year old but 5 years in service identical battery (420 flight
hours) that has never been deep discharged or been on a maintainer, I
measure 52 minutes to 11.00 volts or 5.2 AH again at 6 amps discharge
rate. All tests were done with the battery stabilized at a 66*F basement
room temperature for several days after top up with a Schumaker 1162.
I don't have an easy way to compare the cranking capabilities other than
last winter the two paralleled batts in my Z-14 system seemed to crank a
bit slower than normal. It cranked fine all summer but I have just
replaced the oldest battery anyway. Hasn't been much colder than
freezing yet to compare this winter. I too am surprised that the old
battery delivered 93% of the capacity of the newer one at a 6 amp
discharge rate.
I'll attempt to compare the current flow from each battery while
cranking (clamp on dc ammeter) the next time I fly. (I have the
automatic parallel option during cranking). Should give an indication of
how another 4 year in service batt compares to the new one for cranking.
Ken
On 29/10/2011 11:25 AM, Robert L. Nuckolls, III wrote:
Quote: |
<nuckolls.bob(at)aeroelectric.com>
That bench test battery I featured in a posting
a few days ago had not be cap-checked in several years.
The thing is over ten years old and has yielded a
great return on investment.
I did a load test on this battery about a week ago.
It dumped about 300A for 15 seconds at the 70F mark
on the load meter. A value that is less than 1/2 the
as-new capability.
Just for grins, I pulled out the CBAII battery tester.
The bench battery had been on a maintainer for a couple days.
I did a 6A discharge test. The value I use as exemplary
of most of my instrumentation experiments. The battery
delivered 24+ a.h. of useful energy! Going to the
factory data on this battery we see:
http://www.aeroelectric.com/Pictures/Curves/33AH_12V_Capacity_vs_Load.gif
The factory says a 6.6A load will deplete this battery
in about 4 hours . . . or 24+ a.h.
In years past, my teachers modeled the battery as a large
array of cells connected in a series-parallel configuration
with EACH cell offering some finite energy value combined
with it's own source impedance. If you loose 1/2 the cell
in the full-up array, energy drops by 1/2 but source impedance
doubles.
This experiment last night showed that while the source
impedance for the battery had doubled (1/2 the cranking
snort), the total energy available was still almost as-new!
This means that the gazillion itty-bitty cell analogy is not
quite accurate. Those cells can experience a rise in
source impedance while still offering their original
energy capability.
This battery as-new will deliver 9V at over 800A for
15 seconds. This suggests a source impedance of
(12-9)/800 = .004 ohms. It now produces about 300A
so the new source impedance is (12-9)/300 = .010
ohms.
So while the impedance has doubled, the available
energy at 6A loading has been barely affected . . . if
at all. A rise from .004 to .010 ohms source impedance
has little influence on a test load of (12/6)= 2 Ohms.
This argues with any analogy that suggests a "dead"
micro-cell in a battery becomes totally disconnected
from the array. It suggests that individual cells
can demonstrate an ability to store and regurgitate
energy while experiencing an independent and unrelated
rise in source impedance.
This discovery suggests that it is possible for a
battery to meet battery-only-ops requirements while
demonstrating reduced cranking performance. This ol'
dog is still learning . . . and my grey haired bench
test battery is still in service.
|
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bicyclop(at)pacbell.net Guest
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Posted: Sun Oct 30, 2011 9:05 pm Post subject: RG Batteries: I learned something last night |
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A few years back, we had a dead short on the battery cable before the contactor that drained the battery dead, dead, dead. I arrived and removed the short after about 2 hours. The battery read ~ 5v at that time. Charged it overnight and put it back in service. Several weeks later I replaced it when it failed to start the engine, charged it and did a CBA II capacity test on it at 4 amps. It delivered just under 24 ah - not bad for a severely abused 24 ah battery. I'm still using it as a shop battery.
Pax,
Ed Holyoke
On 10/29/2011 8:25 AM, Robert L. Nuckolls, III wrote: [quote]--> AeroElectric-List message posted by: "Robert L. Nuckolls, III" <nuckolls.bob(at)aeroelectric.com> (nuckolls.bob(at)aeroelectric.com)
That bench test battery I featured in a posting
a few days ago had not be cap-checked in several years.
The thing is over ten years old and has yielded a
great return on investment.
I did a load test on this battery about a week ago.
It dumped about 300A for 15 seconds at the 70F mark
on the load meter. A value that is less than 1/2 the
as-new capability.
Just for grins, I pulled out the CBAII battery tester.
The bench battery had been on a maintainer for a couple days.
I did a 6A discharge test. The value I use as exemplary
of most of my instrumentation experiments. The battery
delivered 24+ a.h. of useful energy! Going to the
factory data on this battery we see:
http://www.aeroelectric.com/Pictures/Curves/33AH_12V_Capacity_vs_Load.gif
The factory says a 6.6A load will deplete this battery
in about 4 hours . . . or 24+ a.h.
In years past, my teachers modeled the battery as a large
array of cells connected in a series-parallel configuration
with EACH cell offering some finite energy value combined
with it's own source impedance. If you loose 1/2 the cell
in the full-up array, energy drops by 1/2 but source impedance
doubles.
This experiment last night showed that while the source
impedance for the battery had doubled (1/2 the cranking
snort), the total energy available was still almost as-new!
This means that the gazillion itty-bitty cell analogy is not
quite accurate. Those cells can experience a rise in
source impedance while still offering their original
energy capability.
This battery as-new will deliver 9V at over 800A for
15 seconds. This suggests a source impedance of
(12-9)/800 = .004 ohms. It now produces about 300A
so the new source impedance is (12-9)/300 = .010
ohms.
So while the impedance has doubled, the available
energy at 6A loading has been barely affected . . . if
at all. A rise from .004 to .010 ohms source impedance
has little influence on a test load of (12/6)= 2 Ohms.
This argues with any analogy that suggests a "dead"
micro-cell in a battery becomes totally disconnected
from the array. It suggests that individual cells
can demonstrate an ability to store and regurgitate
energy while experiencing an independent and unrelated
rise in source impedance.
This discovery suggests that it is possible for a
battery to meet battery-only-ops requirements while
demonstrating reduced cranking performance. This ol'
dog is still learning . . . and my grey haired bench
test battery is still in service.
Bob . . .
[b]
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