Hi all
I have been following the factory five 'design the car' thread on Pistonheads..
The concept sounds great and the result should be very interesting to see - but did I read somewhere that the guys behind the Murtaya were working on
a similar layout (i.e inline rear mounted with the box converted to 2WD), but using the flat six unit from a Subaru Legacy?
I love the idea of the subaru running gear being used in this way, but the only cars are the Saker (£££) or the SDR storm.. which isnt really my cup
tea in an exo kind of way..
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Originally posted by dickie b
Hi all
I have been following the factory five 'design the car' thread on Pistonheads..
.
The Murtaya is a brilliant design IMO and one which I would love to get my hands on.
http://www.murtayasportscars.co.uk/design.html
Spotted one of those in Basingstoke at the weekend - looked mean.
There was a tatty one at an Autosolo a few years a go too.
Murtaya just seems, essentially, like a light subaru? Still got the lump up front between the wheels, so effectively just a re-body?
I'm not sure I'd like to use the 4wd driveline as a 2WD - I did consider it and there's kits to lock the centre diff for just that
reason (about 250 quid IIRC), but I'm not sure it'd cope with all the torque through half the shafts.
I agree with Mr Coyote as to the torque issues especially as I've heard of a few gearbox issues in Scoobies. (Not sure about that as not had much to do with them, just something I've heard). On the upside, with so much less weight the shafts should have a easier time than they would in a saloon car!
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On the upside, with so much less weight the shafts should have a easier time than they would in a saloon car!
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Originally posted by coyoteboy
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On the upside, with so much less weight the shafts should have a easier time than they would in a saloon car!
Actually no, the peak torque felt in the shafts is the same as in the saloon car and is limited only by the engine output, not the body weight. The only difference is the same torque accelerates the lighter car faster.
Imagine the simplest possible system; ignore the gearbox and diffs/shafts apart from the last half shaft (we're assuming they're all the
same anyway). Now use a 1m spanner to turn one end of the shaft using a 100kg weight at the end of it and lock the wheel to the ground (providing
infinite resistance, such as driving a rangerover wheel might ). What's the peak torque in the shaft? It's 1000Nm (give or take). Change
the wheel size to one with half the diameter but keep the wheel locked. What's your shaft torque now? 1000Nm. The change of wheel size means the
force at the tyre contact patch (and so the force on the locking mechanism) is twice as large, but the torque in the shaft is the same and is limited
by the spanner/weight arrangement. The force at the contact patch (or our locking mechanism) is what accelerates your cars mass, but it doesn't
determine peak shaft torque. If the cars mass is higher the same torque in the shaft will produce a slower acceleration, but it can't produce a
higher torque in the shaft.
If you're breaking shafts due to changing wheel sizes it's because your shaft was under-sized to start with for the gearing and engine
driving it, probably on the basis of probable use (i.e. we know the car will start to accelerate and not reach peak torque so we can lose a little
meat off those shafts to save weight and cost).
As I say, adding a flywheel massively increases the torque that can be seen for a fraction of a second using stored energy, but assuming you're
not stepping off the clutch at peak torque with ultra-grippy tyres that won't break free, you'll not see it in the shaft.
Without wanting to labour the point, if you followed your analogy and peak torque was related to wheel size or vehicle weight, if you had an
infinitely heavy car and a 50cc scooter engine you'd be snapping infinite diameter driveshafts still, rather than stalling the engine....
[Edited on 31/5/11 by coyoteboy]
i'll agree that we are labouring the point somewhat, but i'll keep on for now
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Originally posted by coyoteboy
Imagine the simplest possible system; ignore the gearbox and diffs/shafts apart from the last half shaft (we're assuming they're all the same anyway). Now use a 1m spanner to turn one end of the shaft using a 100kg weight at the end of it and lock the wheel to the ground (providing infinite resistance, such as driving a rangerover wheel might ). What's the peak torque in the shaft? It's 1000Nm (give or take). Change the wheel size to one with half the diameter but keep the wheel locked. What's your shaft torque now? 1000Nm. The change of wheel size means the force at the tyre contact patch (and so the force on the locking mechanism) is twice as large, but the torque in the shaft is the same and is limited by the spanner/weight arrangement. The force at the contact patch (or our locking mechanism) is what accelerates your cars mass, but it doesn't determine peak shaft torque. If the cars mass is higher the same torque in the shaft will produce a slower acceleration, but it can't produce a higher torque in the shaft.
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If you're breaking shafts due to changing wheel sizes it's because your shaft was under-sized to start with for the gearing and engine driving it, probably on the basis of probable use (i.e. we know the car will start to accelerate and not reach peak torque so we can lose a little meat off those shafts to save weight and cost).
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As I say, adding a flywheel massively increases the torque that can be seen for a fraction of a second using stored energy, but assuming you're not stepping off the clutch at peak torque with ultra-grippy tyres that won't break free, you'll not see it in the shaft.
Without wanting to labour the point, if you followed your analogy and peak torque was related to wheel size or vehicle weight, if you had an infinitely heavy car and a 50cc scooter engine you'd be snapping infinite diameter driveshafts still, rather than stalling the engine....
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the flaw here is that you are overlooking what size force is required to hold the wheel still - by definition, for the force at the contact patch to be negated, the forces in either direction must be equal. It harder to hold the small wheel still - hence why screwdrivers have large handles.
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well, its an agreed principle in 4wd forums that large wheels break halfshafts, because it is harder to turn the wheel.
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assuming the car had infinite mass, youd need infinitely low gearing to move it, and unless your halfshafts also had infinite diameter, they would also snap!
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Originally posted by coyoteboy
Sure if you let the shaft slip it's going to see lower torque....
I'm here all day!
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no need for all day, you've just agreed with me.
Slipping reduces the torque.
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Ps, google about big wheels on offroaders, i think you'd find it eye opening just how many people you are arguing with.
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Originally posted by coyoteboy
Feel free to answer the moon/planet/baseball bat analogy? According to your way of looking at it I'd be able to apply more torque to the larger planet and so snap the bat. In reality I'd just accelerate the planet slower with the same torque and the bat would be fine as I'm fairly weak
Cracking debate
Utterly OT, but I'm loving it...
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Its a poor analogy because firstly, you cannot break a bat by hand, and secondly, both masses are ridiculously heavy.
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If we replace the lighter one with say a beach ball, then yes, i can reason you out of it, provided that you are actually strong enough to break the bat when there is a planet on the end of it.
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So, assume you have a long bat with jupiter on it, and you are phenominally strong. You twist hard, the planet barely moves, and you crack the handle off. Now, replace with a beach ball; you turn as hard as you can, and before you manage to break it, the whole ball is turning. So you get your equally strong mate to hold the ball still, and smash it between you.
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And you cannot call that friction in this scenario, as its clearly inertia!
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If we're going back to analogies, how about the one i mentioned, about trying to snap a spanner with a loose nut?
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As an example, imagine you have a wheel being turned by a shaft, and the shaft will break at say 100nm of torque. With a 1m radius wheel, that basically means a resistance to motion at the contact patch of 100 newtons will break it. If the wheel was only 50cms radius, then the force required at the contact patch to break the shaft would be 200 newtons. So, the larger wheel has caused the shaft to break with a lower force, because the extra radius as increased leverage.
One question to ask yourself- if, in the heavier car, there's more torque in the shaft - what's producing the torque that snaps it? If the
wheel is magically producing torque in the opposite direction to the engine at an amount larger than the engine can, the engine would stall and go
backwards. Wheels don't produce torque, they only react what comes from the engine - nothing from the engine, no force at the wheel contact
patch. Max torque from the engine = max force at the contact patch (assuming no slip). All that changing the mass of the car does is adjust the
acceleration rate required to load the shaft with the max torque, if the shaft is designed large enough to withstand the max torque of the engine
there's nothing you can do with that engine/transmission combo to snap the shaft, whether you're accelerating a moon or a mouse. As I said,
max torque from the engine should technically include the anglular momentum of the flywheel and rotating parts which would produce a much larger
torque than that specified as the engine's nominal torque output, but only for a fraction of a second. Same applies though, design for that
torque instead and you'll never break the shaft regardless of car mass.
In an effort to keep this thread at least partly on track I'm going to bow out now, but feel free to continue the discussion over U2U or MSN, I
need practice explaining stuff like this!
[Edited on 31/5/11 by coyoteboy]
this is getting silly, we might have to agree to disagree
Description
on the subject of the offroaders though, i suspect it is the low ratio box that causes the problem - on my jeep, first gear in low is about a 20x
reduction in gearing so 20x more torque, so somewhere about 4000lbft at max throttle. Im guessing they cannot realistically make it take this, and
rely on the user not booting it when the wheels cannot turn. Big wheels are easier to stop turning (in a similar way to how you can stop a cordless
drill by grabbing the chuck, but not by grabbing the driver bit shaft), so make it more likely that the shaft will see the full whack.
Sadly that is also linked to the idea that the shafts see less torque when the wheels are free to turn.
No no, you're on the right lines with that one - the high ratio box attempts to spin the engine (when moving faster than RPM would make you) and as you say puts massive torque through the box (assuming the wheel doesnt slip) when hitting the throttle. Probably much more than you could design the shafts to withstand! That's fine, torque multipliers do pose a danger!