Cycling Equipment · Public discussion

Dynamo Lights Brightness PROBLEM

Started by Gordon · · Last activity · 56 posts · 1,459 views

Thread navigation

Jump through the discussion

Go to the original post, the replies on this page, or the latest preserved contribution.

Thread details

What we know about this thread

Original section
Cycling Equipment
Published
9 August 2006
Last activity
11 September 2006
Original author
Gordon
Posts
56
Discussion status
Public discussion
Total views
1,459
Views / 30 days
0

The navigation and discussion metadata provide context. Posts remain in their original chronological order.

Showing posts 41–56 of 56
Posts remain in their original chronological order.

Text size
  1. Don Kelly said:

    Thanks for the info. You did a good job. I have done a few rough
    calculations as below

    The electrical efficiency is about 60% in either case (theoretically the
    same) and any change in overall efficiency is in the mechanical side.

    For the Bottom bracket machine which appears to be the one that the test
    results were for:
    No capacitor: internal impedance at 190Hz =3.8+j8.07 ohms and total
    impedance magnitude is 17.74 ohms so the internal voltage is about 9.5 V
    With capacitor the total impedance drops to about 15.8 ohms and the internal
    voltage generated is still 9.5V. Electrical efficiency in both cases is
    about 76%

    For the Union machine:
    Zinternal =7.9+j7.4 ohms (190Hz)so total circuit impedance is about 21.3
    ohms without the capacitor so, using 0.53A or 6.4V the internal generated
    voltage is about 11.3V
    With capacitor the total impedance drops to 19.9 +j1 ohms or a magnitude of
    19.93 ohms and the internal voltage is about 12V.
    The difference may be some drop in demagnetising effect or a slight change
    in speed. Electrical efficiency about 60%

    I used the higher inductance as this is the one that actually counts (direct
    axis vs quadrature axis inductance).

    Actually, your bike generators are, electrically, rather conventional
    synchronous machines with permanent magnet fields and the internal voltage
    is speed dependent, with the current depending on the load and the internal
    impedance. It is simply a lousy "voltage source " which is identical to a
    lousy "current source".
    However in the case of the bottom bracket machine, the inductance is
    dominant and rises with speed as well so the total circuit impedance rises,
    tending to limit the current somewhat. Note that at twice speed and a 12 ohm
    load the current will be about 0.85A and the power about 8.6 watts. Not
    really constant current. However there may be other factors involved such as
    the demagnetising effect of the current actually reducing the voltage a bit.
    That depends on the actual characteristics of the field magnets.
    If you put a 24 ohm load on, at the original speed, then you'll get about
    7.9V,0.33A and 2.6 watts. Lower current and power. At twice the speed the
    internal voltage will be doubled as will the inductance so the output would
    be 14.2V (probably a bit less) and current 0.6A for 8.4watts (actually less
    current in practice as bulb is hotter). The Union machine will likely have a
    wider current range due to its lower inductance.

    These figures are based on the data given and other factors come into play.
    Some other experiments for you to while away spare time that you could spend
    riding!.

    :-) Oh, I've wasted plenty of riding time on these things!

    Here you go. The article starts on page 4, I think. Some of the
    figures don't print properly in this PDF, but were fine in the printed
    version.

    http://www.ihpva.org/HParchive/PDF/hp49-1999.pdf

    - Frank Krygowski

  2. In message <[email hidden]>, dated Wed,
    6 Sep 2006, David Kerber <ns_dkerber@ns_ids.net> writes

    Quoted message said:

    In article <[email hidden]>, [email hidden]
    says...

    ...

    Quoted message said:
    Quoted message said:

    No, the torque required to turn a generator at a given speed into a
    resistive load is a function of the *power* (Voltage * Current), not the
    current alone. If you short it, your voltage goes to near zero, so the
    power does too.


    That would be true if the generator had zero-impedance windings. It
    doesn't. When you short-circuit the generator, all the power is
    dissipated in the resistance of the winding.

    That's why I said *near* zero. It still doesn't use much true power, so
    the actual mechanical load isn't very high.


    Frank Krygowski reported:

    Union bottle generator: 7.9 Ohms, 5.45 mH (up to 6.2 mH)

    The designed output is 6 V at 0.5 A. We don't know the frequency, so
    we'll neglect the inductance (but at 100 Hz it's about 3.8 ohms), and
    just note that the voltage across the 7.9 ohms is 3.95 V. Compared with
    the 6 V output, that's far from negligible.

    When short-circuited, we have the same 9.75 V generator, but now seeing
    a load of 7.9 ohms (or 8.7 ohms if we include the inductance). That
    gives a current of 1.23 A, and a power of 12 W, **four times** the
    normal output power.
    --
    OOO - Own Opinions Only. Try www.jmwa.demon.co.uk and www.isce.org.uk
    2006 is YMMVI- Your mileage may vary immensely.

    John Woodgate, J M Woodgate and Associates, Rayleigh, Essex UK

  3. In article <[email hidden]>, [email hidden]
    says...

    ....

    Quoted message said:

    Frank Krygowski reported:

    Union bottle generator: 7.9 Ohms, 5.45 mH (up to 6.2 mH)

    The designed output is 6 V at 0.5 A. We don't know the frequency, so
    we'll neglect the inductance (but at 100 Hz it's about 3.8 ohms), and
    just note that the voltage across the 7.9 ohms is 3.95 V. Compared with
    the 6 V output, that's far from negligible.

    When short-circuited, we have the same 9.75 V generator, but now seeing
    a load of 7.9 ohms (or 8.7 ohms if we include the inductance). That
    gives a current of 1.23 A, and a power of 12 W, **four times** the
    normal output power.

    Ok, now that makes sense. I was hugely under-estimating the coil
    impedence of the generator.

    --
    Remove the ns_ from if replying by e-mail (but keep posts in the
    newsgroups if possible).

  4. Thanks- I haven't correlated the graphs with my estimates which do not take
    all into account and appear to be off. The general shape of current vs
    speed curves is flatter than I estimated which implies a higher inductance
    than measured.
    a)Measurement of inductance with an inductance meter may be a bit iffy
    because of the perversity of ferromagnetic devices. Short circuit and open
    circuit tests similar to those used for larger machines may give a
    different result because armature reaction is not negligable and affects
    the apparent inductance.
    To sort this out requires more sophisticated tests which aren't worth while.

    Again- good job- you made your point.

    --

    Don Kelly [email hidden]
    remove the X to answer
    ----------------------------
    <[email hidden]> wrote in message
    news:[email hidden]...

    Quoted message said:


    Don Kelly said:

    Thanks for the info. You did a good job. I have done a few rough
    calculations as below

    The electrical efficiency is about 60% in either case (theoretically the
    same) and any change in overall efficiency is in the mechanical side.

    For the Bottom bracket machine which appears to be the one that the test
    results were for:
    No capacitor: internal impedance at 190Hz =3.8+j8.07 ohms and total
    impedance magnitude is 17.74 ohms so the internal voltage is about 9.5 V
    With capacitor the total impedance drops to about 15.8 ohms and the
    internal
    voltage generated is still 9.5V. Electrical efficiency in both cases is
    about 76%

    For the Union machine:
    Zinternal =7.9+j7.4 ohms (190Hz)so total circuit impedance is about 21.3
    ohms without the capacitor so, using 0.53A or 6.4V the internal generated
    voltage is about 11.3V
    With capacitor the total impedance drops to 19.9 +j1 ohms or a magnitude
    of
    19.93 ohms and the internal voltage is about 12V.
    The difference may be some drop in demagnetising effect or a slight
    change
    in speed. Electrical efficiency about 60%

    I used the higher inductance as this is the one that actually counts
    (direct
    axis vs quadrature axis inductance).

    Actually, your bike generators are, electrically, rather conventional
    synchronous machines with permanent magnet fields and the internal
    voltage
    is speed dependent, with the current depending on the load and the
    internal
    impedance. It is simply a lousy "voltage source " which is identical to
    a
    lousy "current source".
    However in the case of the bottom bracket machine, the inductance is
    dominant and rises with speed as well so the total circuit impedance
    rises,
    tending to limit the current somewhat. Note that at twice speed and a 12
    ohm
    load the current will be about 0.85A and the power about 8.6 watts. Not
    really constant current. However there may be other factors involved such
    as
    the demagnetising effect of the current actually reducing the voltage a
    bit.
    That depends on the actual characteristics of the field magnets.
    If you put a 24 ohm load on, at the original speed, then you'll get about
    7.9V,0.33A and 2.6 watts. Lower current and power. At twice the speed the
    internal voltage will be doubled as will the inductance so the output
    would
    be 14.2V (probably a bit less) and current 0.6A for 8.4watts (actually
    less
    current in practice as bulb is hotter). The Union machine will likely
    have a
    wider current range due to its lower inductance.

    These figures are based on the data given and other factors come into
    play.
    Some other experiments for you to while away spare time that you could
    spend
    riding!.

    :-) Oh, I've wasted plenty of riding time on these things!

    Here you go. The article starts on page 4, I think. Some of the
    figures don't print properly in this PDF, but were fine in the printed
    version.

    http://www.ihpva.org/HParchive/PDF/hp49-1999.pdf

    - Frank Krygowski

  5. In message <sHLLg.512208$Mn5.109648@pd7tw3no>, dated Thu, 7 Sep 2006,
    Don Kelly <[email hidden]> writes

    Quoted message said:

    Measurement of inductance with an inductance meter may be a bit iffy
    because of the perversity of ferromagnetic devices.

    I think that's a valuable contribution. Magnetic devices have been known
    for years to exhibit reluctance, so it's a small step of intention to
    exhibit perversity. This is obviously measured in murphys, but a formal
    definition is required.
    --
    OOO - Own Opinions Only. Try www.jmwa.demon.co.uk and www.isce.org.uk
    2006 is YMMVI- Your mileage may vary immensely.

    John Woodgate, J M Woodgate and Associates, Rayleigh, Essex UK

  6. Quoted message said:
    John Woodgate said:
    Quoted message said:

    What's the ASCII abbreviation for "micro"? I'll go with "mu".)

    Quoted message said:

    'u'. but 'mu' is understood.

    How about: How about: µ

    not ASCII.

    --

    Bye.
    Jasen

  7. John Woodgate said:

    Yes, it's difficult but it can be done. But I doubt that ferrite
    permanent magnets are used in cycle dynamos. They would probably be too
    big.

    I've looked, they are. the magnet was about the size of 1/2 a "D" cell.
    it had 4 poles. (this was in a friction drive dynamo)

    Bye.
    Jasen

  8. John Woodgate said:

    In message <[email hidden]>, dated Thu,
    17 Aug 2006, David Kerber <ns_dkerber@ns_ids.net> writes

    Quoted message said:

    Yes, you are. A filament is a nearly pure resistance load, so the pf
    is already equal to 1.

    The alternator has internal resistance and inductance. To match its
    impedance for maximum power transfer, you need a resistor AND a
    capacitor. The capacitor resonates with the inductance, but the
    resistances apply heavy damping.

    As I indicated a while back, doing this can seriously damage your
    permanent magnet.
    --
    OOO - Own Opinions Only. Try www.jmwa.demon.co.uk and www.isce.org.uk
    2006 is YMMVI- Your mileage may vary immensely.

    John Woodgate, J M Woodgate and Associates, Rayleigh, Essex UK

    How can this seriously damage the permanent magnet? The only possible
    significant damage I can think of is demagnetization, but I don't see
    how the circuit operation would create this. Demagnetizers, at least
    for soft materials, work by cycling the cores magnetically in
    decreasing BH loops, until the remanent magnetization is tolerably
    small. I don't see how this operation would happen in a bike light
    system.

    Ken

  9. Quoted message said:
    Don Kelly said:

    Thanks- that is enough info to determine the inductance but not the
    resistance of the generator.

    We measured the resistances and inductances directly. We had the
    instruments.

    Union bottle generator: 7.9 Ohms, 5.45 mH (up to 6.2 mH)

    Soubitez bottom bracket generator: 3.8 Ohms, 6.76 mH (down to 4.9 mH)

    Briefly, a standard 3 Watt generator bulb (assuming only headlight, no
    taillight) is 12 Ohms. A 2.4 Watt bulb used with a 0.6 Watt taillight
    in parallel has a combined R of 12 Ohms.

    Bike generators are, roughly speaking, constant current devices. Open
    circuit, their output current is zero, and their output voltage is
    roughly proportional to their rpm (up to a certain limit).

    - Frank Krygowski

    If the internal resistance of the dynamo source is about 6 ohms and the
    load resistance applied (the bulb) is 12 ohms or more, the source is
    more akin to a Thevenin source (a voltage source) than a Norton source
    (a current source). NOT a constant current device, but a constant
    voltage device. For a true (zero resistance) Thevenin source with a
    small series resistance in addition to the load (your measured values
    of 3.8 and 7.9 ohms) the voltage will be only about 40 percent higher
    with the load removed, than with the load. But the power will be zero
    because the current into an open circuit is zero.

    For a current source the open-circuit voltage would become much higher
    (theoretically infinite) with the load removed.

    For the generators you cite, the situation is more like a matched load,
    where about teh same power is dissipated in the source internal
    resistance and in the load resistance. In this case the dissipations
    are within about 50%, which practically is pretty well matched.

    Sorry for all the dweeby stuff, but I have fun with this as well as
    with bikes!

    Ken

  10. In message <[email hidden]>,
    dated Sun, 10 Sep 2006, [email hidden] writes

    Quoted message said:

    How can this seriously damage the permanent magnet? The only possible
    significant damage I can think of is demagnetization, but I don't see
    how the circuit operation would create this. Demagnetizers, at least
    for soft materials, work by cycling the cores magnetically in
    decreasing BH loops, until the remanent magnetization is tolerably
    small. I don't see how this operation would happen in a bike light system.

    The output current of the dynamo tries to do exactly that. The 'cycling'
    in decreasing hysteresis loops occurs as you slow down your own
    'cycling', of course. But the root cause of the risk to the magnet is
    the INCREASED load current. We assume that the magnet is designed to
    resist the demagnetizing effect of the 0.5 A (or whatever is the design
    value), but if the load current is increased above that value, the
    magnet wasn't designed with that value of H in mind.
    --
    OOO - Own Opinions Only. Try www.jmwa.demon.co.uk and www.isce.org.uk
    There are benefits from being irrational - just ask the square root of 2.
    John Woodgate, J M Woodgate and Associates, Rayleigh, Essex UK

  11. jasen said:
    Quoted message said:
    John Woodgate said:

    > What's the ASCII abbreviation for "micro"? I'll go with "mu".)

    Quoted message said:

    'u'. but 'mu' is understood.

    How about: How about: µ

    not ASCII.

    --

    Bye.
    Jasen

    What's TRULY (yes, I'm shouting) clear in ASCII (not shouting, it's an
    acronym) is "micro."

  12. In message <[email hidden]>, dated
    Sun, 10 Sep 2006, [email hidden] writes

    Quoted message said:

    If the internal resistance of the dynamo source is about 6 ohms and the
    load resistance applied (the bulb) is 12 ohms or more, the source is
    more akin to a Thevenin source (a voltage source) than a Norton source
    (a current source). NOT a constant current device, but a constant
    voltage device.

    The generators obviously aren't either a constant-voltage OR a
    constant-current source. 'More akin' doesn't help understanding. And you
    haven't taken the inductances into account.
    --
    OOO - Own Opinions Only. Try www.jmwa.demon.co.uk and www.isce.org.uk
    There are benefits from being irrational - just ask the square root of 2.
    John Woodgate, J M Woodgate and Associates, Rayleigh, Essex UK

  13. In article <[email hidden]>

    Quoted message said:
    jasen said:
    Quoted message said:

    John Woodgate writes:

    >> What's the ASCII abbreviation for "micro"? I'll go with "mu".)

    > 'u'. but 'mu' is understood.

    How about: How about: µ

    not ASCII.

    What's TRULY (yes, I'm shouting) clear in ASCII (not shouting, it's an
    acronym) is "micro."


    Why is 'abbreviation' such a long word?

  14. ----------------------------
    <[email hidden]> wrote in message
    news:[email hidden]...

    Quoted message said:


    John Woodgate said:

    In message <[email hidden]>, dated
    Sun, 10 Sep 2006, [email hidden] writes

    Quoted message said:

    If the internal resistance of the dynamo source is about 6 ohms and the
    load resistance applied (the bulb) is 12 ohms or more, the source is
    more akin to a Thevenin source (a voltage source) than a Norton source
    (a current source). NOT a constant current device, but a constant
    voltage device.

    The generators obviously aren't either a constant-voltage OR a
    constant-current source. 'More akin' doesn't help understanding. And you
    haven't taken the inductances into account.

    Strictly speaking, bike generators are neither constant current nor
    constant voltage. Strictly speaking, that's also true of batteries -
    because their internal resistance affects their apparent voltage output
    to varying degrees, depending on current draw. And if we wish to speak
    even more strictly, we could include their lowering voltage over time
    (needing recharge, or perhaps replacement).

    IOW, nothing is perfect. Welcome to the universe!

    But there is definite usefulness in thinking of batteries as constant
    voltage. Almost everyone learns the bulk of their electronics theory
    by assuming that, and for the bulk of practical problems, it's a
    perfectly adequate assumption.

    Similarly, stating that a bike generator is approximately constant
    current does have validity, within limits; and it's certainly more
    valid than saying it's constant voltage! Here's one reason why:

    As I've described, with certain generators, it's possible to drive two
    identical headlamp bulbs connected in _series_. If the generator
    design is such that the drive doesn't slip, and if the bike speed is
    high enough (above 14 mph for mine) the generator will light both lamps
    to normal brightness. The power output of the generator will be
    approximately double it's normal value. Current output will be
    depressed only slightly.

    See http://www.blayleys.com/articles/lights/page2.htm or
    http://www.peterwhitecycles.com/wiringinstructions.asp for some
    details.

    If generators were constant voltage, that setup wouldn't be possible.
    Current would be cut in half, and each bulb would glow only dimly. If
    generators were constant voltage, you'd instead connect two headlights
    in parallel. That absolutely does not work - try it!

    Another minor point: Generator headlamps and taillamps are normally
    connected in parallel. It's fairly well known that, if you blow your
    headlamp bulb, your incandescent taillamp will last only a few seconds.
    Why? All the 0.5 amp is pumped through that low-power (i.e. high
    resistance) bulb. Voltage output rises as the generator
    instantaneously tries to maintain its constant current. The bulb
    blows.

    If the generator were constant voltage, the bulb would feel no
    difference.

    Yes, I realize "constant current" is a simplification, but it's good
    enough to be useful, and points out important differences between bike
    generators and batteries.

    - Frank Krygowski


    Speed---> voltage induced
    Current--->torque
    At a given speed, the internal voltage will be nearly constant. Internal
    impedance exists- you can treat the device as a voltage source with a series
    internal impedance (as it actually is) or as a current source shunted by
    this impedance. There are some demagnetising amp turns under load so that
    the flux density decreases as load increases resulting in a decrease of the
    internal voltage. This can be expressed in terms of an equivalent inductance
    in addition to the leakage inductance that an inductance meter can measure.
    Extra internal impedance or the equivalent tends to limit the current
    variation with load or speed leading to the nearly constant current
    characteristic due to the dominant effect of the internal impedance.

    You simply have a high impedance speed dependent (variable- not constant)
    voltage source. The difference between this and a battery is that the
    battery internal voltage is not speed dependent and its impedance is low so
    it looks more like a constant voltage source .
    If the headlamp burns out, the tail lamp will see more current as the
    terminal voltage will rise. That is true. It is not a case of the generator
    trying to pump 0.5A through the bulb although it may look that way.

    Consider a 10V source with a 10 ohm internal resistance (to simplify by
    ignoring inductance) supplying a 10 ohm load. The load voltage and current
    will be 5V, 0.5A
    Now increase the load to 20 ohms. The load voltage will be 7.5V and current
    0.75A.
    In the case of the generator, the armature reaction will actually reduce the
    internal voltage so the output will be lower- possibly 6V and 0.6A. No more
    than that, excluding speed effects.
    --

    Don Kelly [email hidden]
    remove the X to answer

    Quoted message said:
  15. In article <DZ2Ng.526182$Mn5.110669@pd7tw3no>,

    Don Kelly said:

    At a given speed, the internal voltage will be nearly constant.
    Internal impedance exists- you can treat the device as a voltage
    source with a series internal impedance (as it actually is) or
    as a current source shunted by this impedance. There are some
    demagnetising amp turns under load so that the flux density
    decreases as load increases resulting in a decrease of the
    internal voltage. This can be expressed in terms of an equivalent
    inductance in addition to the leakage inductance that an
    inductance meter can measure. Extra internal impedance or the
    equivalent tends to limit the current variation with load or
    speed leading to the nearly constant current characteristic due
    to the dominant effect of the internal impedance.

    In the case of that bottom bracket generator the OP
    physically measured 3.8 ohms and 6.72mH.

    But he also did a separate experiment, where the output
    was seen to increase from 6.4V to 7.3V when a 100uF
    capacitor was placed in series.

    If it assumed that the internal voltage, the resistance,
    and the inductance remained reasonably constant across the
    experiment, then the inductance works out to about 7mH.

    7mH is not far off the physical measurement of 6.72mH.

    Umm... all sums assume a sinewave output, something that
    is not neccessarily true for small PM alternators.

    [snip]

    Quoted message said:

    Consider a 10V source with a 10 ohm internal resistance (to
    simplify by ignoring inductance) supplying a 10 ohm load. The
    load voltage and current will be 5V, 0.5A Now increase the load
    to 20 ohms. The load voltage will be 7.5V and current 0.75A.

    Small typo there? At a 20-ohm load the load voltage will
    only rise to 10*20/30 and the current will drop to 10/30.

    --
    Tony Williams.

  16. ----------------------------
    "Tony Williams" <[email hidden]> wrote in message
    news:[email hidden]...

    Quoted message said:

    In article <DZ2Ng.526182$Mn5.110669@pd7tw3no>,

    Don Kelly said:

    At a given speed, the internal voltage will be nearly constant.
    Internal impedance exists- you can treat the device as a voltage
    source with a series internal impedance (as it actually is) or
    as a current source shunted by this impedance. There are some
    demagnetising amp turns under load so that the flux density
    decreases as load increases resulting in a decrease of the
    internal voltage. This can be expressed in terms of an equivalent
    inductance in addition to the leakage inductance that an
    inductance meter can measure. Extra internal impedance or the
    equivalent tends to limit the current variation with load or
    speed leading to the nearly constant current characteristic due
    to the dominant effect of the internal impedance.

    In the case of that bottom bracket generator the OP
    physically measured 3.8 ohms and 6.72mH.

    But he also did a separate experiment, where the output
    was seen to increase from 6.4V to 7.3V when a 100uF
    capacitor was placed in series.

    If it assumed that the internal voltage, the resistance,
    and the inductance remained reasonably constant across the
    experiment, then the inductance works out to about 7mH.

    7mH is not far off the physical measurement of 6.72mH.

    Umm... all sums assume a sinewave output, something that
    is not neccessarily true for small PM alternators.

    [snip]

    Quoted message said:

    Consider a 10V source with a 10 ohm internal resistance (to
    simplify by ignoring inductance) supplying a 10 ohm load. The
    load voltage and current will be 5V, 0.5A Now increase the load
    to 20 ohms. The load voltage will be 7.5V and current 0.75A.

    Small typo there? At a 20-ohm load the load voltage will
    only rise to 10*20/30 and the current will drop to 10/30.

    --
    Tony Williams.

    The physically measured inductance using an inductance meter only measures
    the leakage reactance at a negligably low current (varying with position as
    it is salient pole) which is generally much lower than the total direct axis
    reactance of the machine. I did calculations based on the given reactance
    and these estimations indicated a wider variation of current with speed or
    load resistance than his given curves. To me, this indicates that there is
    more going on than what can be represented by a leakage reactance and Dc
    resistance behind a speed dependent voltage-- i.e. demagnetization effect
    (depending on the characteristics of the actual permanent magnet material
    used). is not negigable In models, this is treated by an increase in
    reactance above leakage reactance (in a large machine this will far exceed
    leakage reactance but in this device-who knows). The apparent internal
    voltage based on the data does change when the capacitor is added. Less so
    for the bottom bracket machine than the other (better magnet?). An
    inductance meter is inherently inadequate for measuring the "inductance" of
    a synchronous machine. If the magnet's BH curve is nearly flat topped, one
    could assume no demagnetisation effect- but is it?

    Data for his published curves may have enough information to actually
    construct a model which gives a more realistic "inductance" than what the
    inductance meter gives. However, I have lost his reference and even with
    the curves- it would be still a crude estimation.

    It is true that the behaviour of the generator more closely resembles a
    "constant current source" than a "constant voltage source" because it is a
    "variable voltage "source. The inductive impedance also varies with speed so
    that where this is dominant, the current change with a given load and
    varying speed will be small. This is what is happening. A true constant
    current source would produce the same current (at the same speed) for any
    reasonable load variation. This is not not happening.

    As for sine wave output- you are quite right.

    As for the example that I gave- you are also quite right- and I am
    embarrassingly wrong! Even with the wine I had consumed at the time I should
    have seen that increasing the resistance reduces the current.

    Anyhow it is fun even if it is not particularly useful.
    --

    Don Kelly [email hidden]
    remove the X to answer

Active in the last 60 minutes

Active in this thread

0 users · 0 guests ·0 bots ·0 total

No signed-in users are active right now.

No known search crawlers active right now.