MI = (14.7 X 1.5^2)/3=11.025 Newtons
and as there are 3 blades its 11.025 N * 3 = 33.075N of total Moment of inertia on the rotational Axis..
so now the DC motor has to produce more than 33 Newtons per ... ?
so that it rotates the shaft a 0 RPM ,and if i produces any torque less than 33 Newtons per ... then the motor stalls and will never be able to start the rotation by itself..
am i right about this?
Not quite. To start the rotation, the motor torque just has to overcome the dry friction of the motor (i.e. of the rotor in its bearing(s)).
Then any minimum torque τ is enough to accelerate any Moment of Inertia (MI) with an angular acceleration α
τ = MI * α
_______________
PS: mind the units:
MI = (14.7N X 1.5^2m2)/3=11.025 N*m2 (Newtons times square-meters)
... 3 blades is: 11.025 N*m2 * 3 = 33.075 N*m2 of total Moment of inertia on the rotational Axis. <- Right! (+ MI of rotor & axis)
Yes it can. That's the point.Its obvious the motor cant rotate it...
A physical correct attempt of torque calculation must contain an expression for angular acceleration. It's till missing from your posts. Static friction, as mentioned by erikl is a differnt point, but not directly related to the problem. You can (in principle) design a drive with frictionless bearing, e.g. magnetic or air bearing, so there's a realistic method to rotate a shaft with arbitrarily small torque (and respective large acceleration time).How do i find that torque?
If the plate is truly mounted at the center of gravity (i.e. the plate will stay in any position it is manually rotated to), then the only reason the plate won't rotate is if the static (dry) friction is greater than the motor torque..................................
Ill illustate a example to express my question
Ill take a small motor which are used in radios n toy cars and it is powered by 12 v dc ,n now ill connect a metal rectangular plate which weighs 1kg n the motor shaft is connected to the center of gravity of the plate
Its obvious the motor cant rotate it,it reaches its maximum stall current,unable to rotate it ,as it is unable produce enough torque to rotate the plate...
How is this ?? U said any amount of torque can rotate any amount of moi..
So u mean that the 12v dc motor can rotate the 1kg metal plate wen it the shaft is connected to the CG but the angular velocity will be very low ? Did i get that right ??Yes it can. That's the point.
If the plate is truly mounted at the center of gravity (i.e. the plate will stay in any position it is manually rotated to), then the only reason the plate won't rotate is if the static (dry) friction is greater than the motor torque.
That's what we've all been trying to tell you. :wink:...................
Ok so till today i guess i had thought that the torque of motor should be higher than the shaft load or the combined inertia of shaft to make it move,but the real force the motor has to over come by its torque is the dry friction of shaft ,right?
That's what we've all been trying to tell you. :wink:
That's not what was said. Please re-read the posts. The motor's torque (over and above that needed to overcome friction) will determine how fast the rotor accelerates. And, of course, there will be also be air friction to overcome as the rotor speeds up.........................
so i will assume that,there is no friction in the rotor(hypothetically),
and now the shaft has 33 Newtons of Moment of Inertia,that is the 33 Newtons of resistance of shaft to change its motion..
so in order to rotate the shaft,the 33 N of MOI should be overcomed by the motor,but now i know the motor's torque has nothing to with it,
then what characteristic/attribute of a motor comes to play to overcome this MOI?
No. See post 4. The unit of Moment of inertia is N*m² not N.the shaft has 33 Newtons of Moment of Inertia
No. Moment of Inertia is not a force, and it does not have to be "overcomed" before the shaft can rotate.so in order to rotate the shaft,the 33 N of MOI should be overcomed by the motor
That's not what was said. Please re-read the posts. The motor's torque (over and above that needed to overcome friction) will determine how fast the rotor accelerates. And, of course, there will be also be air friction to overcome as the rotor speeds up.
To summarize the motor torque:
1. Overcomes any bearing friction
2. Accelerates the rotor mass (the more torque, the faster the acceleration)
3. Overcomes air friction at speed
Make sense?
1)Overcomes any bearing friction
Torque definitely matters when you want to speed up the rotor in finite time. That's what the angular acceleration formula is talking about. https://en.wikipedia.org/wiki/Angular_acceleration
... i want to know what "power" motor will be able to overcome the friction of the rotor setup in my first post and rotate it rather than stalling...
Any motor should be able to overcome its own dry friction - otherwise it wouldn't be worth to be called a motor.
You've probably already passed by a wind turbine which you thought to be in state of rest because you didn't see it rotate. If you looked again after a few seconds you might have seen that the position of the blades had changed: it actually rotated, but rather slowly, so you couldn't detect the rotation itself, but only its action after some time.
Now let's assume your motor's torque (τ) is enough to overcome the static (dry) friction of its bearings - as any motor will be able to achieve - , however is rather small compared to the mass of inertia (Mi) of the blades, so after the begin of moving it will start to rotate very slowly.
Let's try an example: Say your motor's torque is just 1Nm , and the total load of your blades has an Mi of 33Nm2 - as calculated by you - then you achieve an angular acceleration of
α = τ/Mi = 1/33 m-1 = 0.03 rad/s2 .
One second after start, the blades will have rotated an
angle = (α/2)*t2 = 0.015 rad = 0.87°
- a rotational movement not easily to be detected.
If now the dynamic friction of the blades in the air eats up a part (or all) of the motor's torque, the rotational velocity will increase even slower (or not at all) - its moving action practically invisible - just by the position of the blades after a while.
Without dynamic friction this acceleration would go on, and after 10 seconds the total rotational movement of the blades would reach 100*0.87°, or nearly a right angle difference - easily detected.
In any case the dynamic friction of the blades in the air will match the motor's torque at some rotational velocity, and so prevent further acceleration of its speed.
and this 0.36 rads/sec² of accelration acclerates the shaft until it reaches the same angular acceleration ,after the shaft reaches to the point where the shafts has the accleration equal to or more than 0.36 rads/sec²,the the torque produced by the motor cannot influence the shaft to increase its speed any further,but when by friction/air resistance,the shaft rotating acceleration reduces,the torque by the motor tries to maintian the acceleration to 0.36 rads/sec²..
Right!so by taking the calculations you made and the theorem you said "Any minimum torque τ is enough to accelerate any Moment of Inertia (MI) with an angular acceleration α"
i think i need not worry about how much torque is necessary to just start the rotation of the shaft..
That's correct if you want to operate the "naked" motor alone, i.e. without the load of the blades.rather i need to calculate the Moment of inertia of the shaft and and determine what amount of Troque is necessary to accelerate the shaft to desired RPM in the given finite time..
so even if the Moment of inertia increases ,say 100Nm² with just 1Nm of torque produced by motor,the shaft will rotate but too too too slow,which is virtually like no rotation...
Exactly!so if assume i have 12Nm of torque and MoI of 33Nm²,the the Angular acceleration would be 0.36 rads/sec²..
am i right about this?
Right!
That's correct if you want to operate the "naked" motor alone, i.e. without the load of the blades.
Together with the blades, the total Moment of inertia is the sum of the Mi's of the rotor, the shaft, and the blades. I'd guess, however, the Mi's of the rotor and the shaft are insignificant compared to the blades' Mi.
the weight of the each blade is 1.5 kg/14.7 Newtons
and the length of blade is 1.5 meter
therefore MI = ( (14.7N) X (1.5meter)^2)/3=11.025 Newtons
and as there are 3 blades its 11.025 N * 3 = 33.075N of total Moment of inertia on the rotational Axis..
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