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AirNZ wrote:So if the plane is moving forward at all, the belt is not doing it's job. Which according to the question can't happen, because the speed always matches.
That's a problem right there, because we're working off a falsehood.
pidge wrote:
Treat the conveyor belt as one gear, the wheel as the other.
Meshed gears rotate in opposite directions, correct? If the wheel rotates anti-clockwise, the converyor belt will "rotate" clockwise, staying in mesh.
V8MOFO wrote:Yea, I have just had an epiphany. Thinking of the toy car on the tredmill... Think about it, If you believe that pushing the car ( by hand, no power going to the wheels ) along, the only way it would actually move forward relative to the ground would be if the wheels were moving faster than the belt. If you add more thrust ( more push! ) and the car did move, the wheels would slip, do a burnout, do a skid!. Thus failing to match the conditions of the original setup.
RedMist wrote:Lets take dynos as an example. If wheelspeed matches dyno speed the vehicle will never ever climb out of the dynos. Because in order to do so wheelspeed has to be greater than dyno speed. So you accelerate using thrust the wheels attempt to move, the dyno reacts instantaneously and reverse rolls, you instanatly accelerate both wheels and dyno to have enough wheelspeed and friction on said spindles and bearings to counteract the thrust. To climb out of the dynos is to ignore the constraints of the question posed as the wheelspeed is greater than the dyno (conveyor) speed.
RedMist wrote:Beautiful example. If both cogs are turning, in opposing directions at exactly the same speed can one gear rotate around the other? Because thats what you are stating in the plane instance.
RedMist wrote:pidge wrote:You have a set containing the numbers 1 to 9 {1,2,3,4,5,6,7,8,9)}
Which numbers in that set are divisible by 3?
Why?
Simple. All of them. You didn't state you required a whole number.
pidge wrote:Here's another one:
You have a set containing the numbers 1 to 9 {1,2,3,4,5,6,7,8,9)}
Which numbers in that set are divisible by 3?
Why?
RomanV wrote: Mr Mainstream: The king of the Pushrods?!
Mr. Mainstream wrote:my brain hurts from reading that and i wont be able to sleep for day![]()
Adamal wrote:*Skips 9 pages of stuff he can't be bothered reading*
Too many concerning factors if you ask me.
One of the biggest is the size of the leading edge of the wing. The larger the curve of the leading edge effects the amount of 'lift' that can be created by the wing. The down side is that this will reduce the planes top speed, but we're not concerned about this here.
One thing is that in this situation, the runway is only as long as it is wide. If we're assuming that the width of the runway in question is the same as say, Auckland International, then you're probably not going to be able to take off in ANY plane (Except my dad's Zennith Air STOL701 Microlite) unless the rate of acceleration is increadible. (When you consider that a 747-400 is about as long as a runway is wide!)
blitza wrote:Adamal wrote:*Skips 9 pages of stuff he can't be bothered reading*
Too many concerning factors if you ask me.
One of the biggest is the size of the leading edge of the wing. The larger the curve of the leading edge effects the amount of 'lift' that can be created by the wing. The down side is that this will reduce the planes top speed, but we're not concerned about this here.
One thing is that in this situation, the runway is only as long as it is wide. If we're assuming that the width of the runway in question is the same as say, Auckland International, then you're probably not going to be able to take off in ANY plane (Except my dad's Zennith Air STOL701 Microlite) unless the rate of acceleration is increadible. (When you consider that a 747-400 is about as long as a runway is wide!)
WTF??
I always thought lift charistics were dictated by the chord/span/rib ratio, but then I wouldnt know..........
TOOT '06?
RomanV wrote:RedMist wrote:Lets take dynos as an example. If wheelspeed matches dyno speed the vehicle will never ever climb out of the dynos. Because in order to do so wheelspeed has to be greater than dyno speed. So you accelerate using thrust the wheels attempt to move, the dyno reacts instantaneously and reverse rolls, you instanatly accelerate both wheels and dyno to have enough wheelspeed and friction on said spindles and bearings to counteract the thrust. To climb out of the dynos is to ignore the constraints of the question posed as the wheelspeed is greater than the dyno (conveyor) speed.
This is of course, unless the dyno doesnt roll about its centre.... What if it rolls on the tangent of the wheel? (The line on the pic)
It doesnt state that the conveyor rolls around a centre line, like you are implying.
eg... Imagine that the dyno is the 'imaginary' wheel, and both the 'real' and 'imaginary' wheels rotate along the line, as opposed to around their centres.
Foward motion is obtained, both of the wheels travel at exactly the same speed, one in the opposite direction of the other.
The 'line' doesnt move, which would be the equivilent of hard ground, or a conveyor that is stationary.
pidge wrote:You are assuming speed of rotation of the wheel is directly linked to the speed of the wheel. The wheel is able to rotate freely, independant of the speed at which the wheel itself is moving.
pidge wrote:Take a matchbox car and a sheet of paper. Roll the car over the sheet of paper. The speed of the wheels = speed of the car, relative to the ground and to the sheet of paper, and the rotational speed of the wheels is the same speed of the wheels and car.
pidge wrote:Now hold the car car still and pull the sheet of paper. Relative to the ground, the speed of the wheels and the car are still the same (and zero), but the rotational speed of the wheels is the same as the paper.
pidge wrote:Now push the car while pulling the sheet of paper (at the same speed - hey, this sounds familiar...). The speed of the car and wheels, relative to the ground are the same, and opposite to the speed of the sheet of paper. The rotational speed of the wheels is same as relative speed of the
sheet of paper and car, twice either speed.
pidge wrote:The speed of the wheel is determined by the speed of the plane. The speed of rotation of the wheel is determined by the relative speed of the plane and the converyor belt surface.
pidge wrote:Oh, and go look up planetary gears - where one gear rotates about another... found in automatic gearboxes.
RomanV wrote:V8MOFO wrote:Yea, I have just had an epiphany. Thinking of the toy car on the tredmill... Think about it, If you believe that pushing the car ( by hand, no power going to the wheels ) along, the only way it would actually move forward relative to the ground would be if the wheels were moving faster than the belt. If you add more thrust ( more push! ) and the car did move, the wheels would slip, do a burnout, do a skid!. Thus failing to match the conditions of the original setup.
Unless.... The belt doesnt move at all.
eg. The speed of the car, relative to the (not moving) belt, is 10kph to the east.
The speed of the belt, (and the rest of the world for that matter) relative to the car, is 10kph to the west.
In other words, the belt has MATCHED the speed of the wheels, and in the opposite direction.... Criteria satisfied.
The speed of the wheels and the belt are matched.... 10kph relative to each other.
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