Rhinochugger
Retired Oik
Ah, the worm has turned
More heat?
More heat?
Rik, I think your maths are quite correct.I don't think it has anything to do with the condition of the motor. Through various means, I now have three of those motor blocks and they all perform in exactly the same way even though one has a Buhler motor in place of the Bachmann original. The only common factor is the size of the worms.
The formula for calculating rotational inertia indicates that the force is proportional to the distance from the axis of rotation squared! So even in our scale, increasing the diameter of the worm has an exponential effect on the force needed to turn it. Doubling it, requires four times the force, tripling it requires nine times the amount of effort and so on. The larger old worm is roughly three times the diameter of the new worm and so, I reckon it will only require a ninth of the effort needed to turn the new worm.
If anyone wants to check my maths then please feel free to do so.
This could explain why Bachmann redesigned the Lyn mechanism - it now has a single small diameter worm gear.
Rik
The problem is that the motor on the new block has had it. One of the brushes has disintegrated and as it's a can motor, I can't get inside to replace it. I do, however, have identical motors from the old motor blocks but I can't get the worm and flywheel off the motor on the new block. I've bent one gear puller and even a new heavier duty puller just won't budge it. I've tried heating up the worm and flywheel but they still won't budge.
Does anyone have any suggestions?
Rik
While your calculations for rotational inertia may be exact, it's meaningless unless you are changing the speed radically on and off and expect the loco to react that way, from 0 to 100 speed in milliseconds.I don't think it has anything to do with the condition of the motor. Through various means, I now have three of those motor blocks and they all perform in exactly the same way even though one has a Buhler motor in place of the Bachmann original. The only common factor is the size of the worms.
The formula for calculating rotational inertia indicates that the force is proportional to the distance from the axis of rotation squared! So even in our scale, increasing the diameter of the worm has an exponential effect on the force needed to turn it. Doubling it, requires four times the force, tripling it requires nine times the amount of effort and so on. The larger old worm is roughly three times the diameter of the new worm and so, I reckon it will only require a ninth of the effort needed to turn the new worm.
If anyone wants to check my maths then please feel free to do so.
This could explain why Bachmann redesigned the Lyn mechanism - it now has a single small diameter worm gear.
Rik
I remember there was a formula for selecting the gear ratio on your slot car that related to the length of the longest straight on any circuit ............. long time ago, nowI suppose an analogy for the large worm gears are the sizeable chainwheels used on track racing bicycles. They require quite prodigious "torque" inputs from the rider to get them moving, or even to change speed (where the track's bankings steep inclines are used to aid) However, they provide the long gear ratios needed to allow prodigious levels of speed to be maintained while still allowing the rider to optimize the use of their power out put, in the near perfect "speed bowl" environment of the track. With a road racing bicycle they are equipped with a wide range of gear ratios (including smaller chainwheels and gear clusters) so the rider can optimise the use of their power output to meet the prevailing conditions rather than applying energy sapping levels of torque to overcome inclines and changes in speed..
Which begs the question - Why is the configuration, as manufactured, so dismal at delivering a usable performance envelope expected in a typical garden railway ? Max
I think it's significant that Bachmann have redesigned the mechanism completely. The motor now has a small worm driving an idler which transfers power to the axle. They have put a flywheel on the other end of the motor shaft. The motor used in the new mechanism is identical to the old motor - so it's clearly the large worms which are at fault.Ignoring all the maths and engineering, I suppose the simple way to look at the successfulness of the big worms is to consider why that particular method hasn't really been used on many other models? On paper it looks like a very neat way to get a good sized flywheel and the worm into a compact space. If there really isn't a mechanical downside to having the larger worms in our models, why don't we see it more?
I hope you do manage to find a solution after all this Rik, you've made a fine looking locomotive I look forward to seeing it in useful service on your line.
That's a much better analogy than my skater - thanks.I suppose an analogy for the large worm gears are the sizeable chainwheels used on track racing bicycles. They require quite prodigious "torque" inputs from the rider to get them moving, or even to change speed (where the track's bankings steep inclines are used to aid) However, they provide the long gear ratios needed to allow prodigious levels of speed to be maintained while still allowing the rider to optimize the use of their power out put, in the near perfect "speed bowl" environment of the track. With a road racing bicycle they are equipped with a wide range of gear ratios (including smaller chainwheels and gear clusters) so the rider can optimise the use of their power output to meet the prevailing conditions rather than applying energy sapping levels of torque to overcome inclines and changes in speed..
Which begs the question - Why is the configuration, as manufactured, so dismal at delivering a usable performance envelope expected in a typical garden railway ? Max
There's probably a few things that have driven this - 'scuse the pun.I think it's significant that Bachmann have redesigned the mechanism completely. The motor now has a small worm driving an idler which transfers power to the axle. They have put a flywheel on the other end of the motor shaft. The motor used in the new mechanism is identical to the old motor - so it's clearly the large worms which are at fault.
I'm not certain about the maths but intuitively to me it's self evident. The further away from the axis of rotation the force is delivered, the more effort (ie torque) is required.
Rik
I'm wondering if the idler might be to allow for clearance between the motor and the worm wheel. The problem I've encountered with trying to fit a smaller worm is that the can of the motor prevents me from putting the centre of the worm over the centre of the worm wheel - I'll either need to extend the shaft or place an idler between the worm and worm wheel. My engineering capabilities don't extend as far as adding an idler so I might have a go at extending the shaft. I'm having to use copper tube as a reducer on the worm so that is possible.There's probably a few things that have driven this - 'scuse the pun.
A two-stage gearbox reduces the strain on the gears, thus reducing the chances of stripping the gears, plus a flywheel also helps to reduce the strain on the gearbox when a track-powered loco stutters.
The lack of flywheels in our large scale locos has long surprised me - it's simple enough to do and is entirely beneficial. Bachmann woke up to this solution pretty late, but other manufacturers still persistently ignore it, despite it being used extensively in the smaller scales.
Yeah, the theory of the two-stage gearbox is to deal with greater loads - putting one together is an art form.I'm wondering if the idler might be to allow for clearance between the motor and the worm wheel. The problem I've encountered with trying to fit a smaller worm is that the can of the motor prevents me from putting the centre of the worm over the centre of the worm wheel - I'll either need to extend the shaft or place an idler between the worm and worm wheel. My engineering capabilities don't extend as far as adding an idler so I might have a go at extending the shaft. I'm having to use copper tube as a reducer on the worm so that is possible.
The modulus of the new gears are 0.5 which means the teeth are smaller than those on the original gears. This makes meshing them a lot trickier - less wiggle room. I've redesigned the casing to bring them a tiny bit closer (0.2mm) but I'm not sure of they are up to the job. I've sent off for another set which are 0.8 Mod so I'm hoping they will make meshing easier.
Rik
OK GregAgain, while takes more (you choose, torque, energy, horsepower, ergs, etc.) to turn a larger mass, the extra power needed to turn it at constant or slowly changing speeds is minimal between these 2 worms... back to inertia again, only makes a difference if you try to change speeds rapidly, which we do not.
The laws of physics won't be bent to suit an analogy.
So, while you disagree with me, you note that a flywheel has been added to the newer design, again, more rotational mass.
But I'm asking what was wrong with the first solution, and it seems that the current solution is no better. What was the source of the effort to make the change?
But, this may be flogging a dead horse, I asked several times... really all I am curious about is what happened, I have a degree in physics, I don't need a refresher on the laws of kinematics, this stuff I do indeed comprehend.
So I give up my curiosity...
Greg