Can a Variable Inertia Flywheel Maintain Constant Speed?

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Discussion Overview

The discussion revolves around the energy requirements for changing the inertia of a flywheel to maintain a constant rotational speed while varying its radius. Participants explore the implications of this concept in relation to energy input and output, centrifugal forces, and the mechanics of mass distribution on the flywheel.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions how much energy is needed to change the inertia of a flywheel when the radius is altered, given a specific mass and rotational speed.
  • Another participant provides formulas for calculating the moment of inertia and kinetic energy, suggesting that a radial force must be applied to maintain constant speed when changing the moment of inertia.
  • Some participants discuss the implications of energy storage in the flywheel and the need to adjust mass distribution to maintain speed, raising concerns about energy expenditure when moving mass inward or outward.
  • There is mention of the complexity introduced by non-uniform mass distribution on the flywheel, which could affect calculations related to energy and force.
  • A participant shares a sketch to clarify their concept of using the flywheel as a battery, indicating that energy input and output would dictate changes in radius.
  • Another participant emphasizes the need for details on mass distribution to accurately calculate energy requirements and challenges the feasibility of maintaining speed solely through radius changes.
  • One participant expresses uncertainty about whether all energy stored in the flywheel would need to be expended to change the radius, questioning the practicality of the proposed method.
  • Further discussion includes the need for additional engineering considerations and calculations related to the movement of a linear bearing to regulate flywheel inertia.

Areas of Agreement / Disagreement

Participants express differing views on the feasibility and energy implications of maintaining constant speed while changing the radius of the flywheel. There is no consensus on the exact energy requirements or the practicality of the proposed methods.

Contextual Notes

Participants note that the calculations depend on the mass distribution of the flywheel, which has not been fully disclosed. The discussion also highlights the complexity of energy expenditure related to moving mass and maintaining rotational speed.

miljacev
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Hello,


My question is: how much energy is needed for changing inertia of flywheel?

example: on rotary shaft we have linear actuator which is moving some object (mass). by that movement, radius of flywheel is changing. ...if there is energy input to flywheel, mass is moving away form shaft in order to maintain constant flywheel speed. If flywheel is sending energy to generator we need to move that mass towards the shaft in order to maintain speed.

m=10kg
r=100mm
speed= 3000rpm

at that moment, there is 10kN of centrifugal force on that mass. ...do I need to apply more than 10kN of force on that mass in order to change radius?


Thanks
 
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miljacev said:
Hello, My question is: how much energy is needed for changing inertia of flywheel?

example: on rotary shaft we have linear actuator which is moving some object (mass). by that movement, radius of flywheel is changing. ...if there is energy input to flywheel, mass is moving away form shaft in order to maintain constant flywheel speed. If flywheel is sending energy to generator we need to move that mass towards the shaft in order to maintain speed.

m=10kg
r=100mm
speed= 3000rpm

at that moment, there is 10kN of centrifugal force on that mass. ...do I need to apply more than 10kN of force on that mass in order to change radius?Thanks
Welcome to PF!

Assuming the flywheel is of uniform thickness and density, the moment of inertia is:

I = \frac{1}{2}mr^2

The kinetic energy of the spinning flywheel is:

KE = \frac{1}{2}I\omega^2 where ω is the angular speed in radians / sec.

If you are applying torque to the flywheel changing it rotational speed, the work done is the change in kinetic energy:

W = \frac{1}{2}I({\omega_f^2 - \omega_i^2})

If you are changing the moment of inertia of the flywheel to maintain constant speed, then you will have to apply a radial force to the mass on the wheel. You would have to tell us the mass distribution on the wheel and how you change that. But the change in energy is just:

\Delta KE = \frac{1}{2} \Delta(I\omega^2)

AM
 
Andrew Mason said:
Welcome to PF!

Assuming the flywheel is of uniform thickness and density, the moment of inertia is:

I = \frac{1}{2}mr^2

The kinetic energy of the spinning flywheel is:

KE = \frac{1}{2}I\omega^2 where ω is the angular speed in radians / sec.

If you are applying torque to the flywheel changing it rotational speed, the work done is the change in kinetic energy:

W = \frac{1}{2}I({\omega_f^2 - \omega_i^2})

If you are changing the moment of inertia of the flywheel to maintain constant speed, then you will have to apply a radial force to the mass on the wheel. You would have to tell us the mass distribution on the wheel and how you change that. But the change in energy is just:

\Delta KE = \frac{1}{2} \Delta(I\omega^2)

AM

...thanks for welcome and replay.
To make things more clear, I've made a simplified sketch in paint, and I think that it will be a good idea to explain little bit more that concept in my head.

That flywheel should have function of a battery. energy will be pumped into flywheel in cycles, but generator is hooked up to flywheel and it requires constant rotation speed.

My idea is to maintain constant speed of flywheel with variable radius. More power is pumped into flywheel than it is taken by generator, radius is increasing. Les power is pumped into flywheel than it is taken by generator, radius is decreasing.

My question is: how much energy I need for changing radius?

tnx







http://cdn.imghack.se/images/5af9e9c18fabbd84e5aec5b9a234c9ce.jpg
 
miljacev said:
...thanks for welcome and replay.
To make things more clear, I've made a simplified sketch in paint, and I think that it will be a good idea to explain little bit more that concept in my head.

That flywheel should have function of a battery. energy will be pumped into flywheel in cycles, but generator is hooked up to flywheel and it requires constant rotation speed.

My idea is to maintain constant speed of flywheel with variable radius. More power is pumped into flywheel than it is taken by generator, radius is increasing. Les power is pumped into flywheel than it is taken by generator, radius is decreasing.

My question is: how much energy I need for changing radius?

tnx







http://cdn.imghack.se/images/5af9e9c18fabbd84e5aec5b9a234c9ce.jpg

You can calculate work from

\mathtt{\ W\ =\ \int_{r_2}^{r_1}\ F_{(r)}dr}\ =\mathtt{ \int_{r_2}^{r_1} m\ \omega^{2}rdr}
 
miljacev said:
...thanks for welcome and replay.
To make things more clear, I've made a simplified sketch in paint, and I think that it will be a good idea to explain little bit more that concept in my head.

That flywheel should have function of a battery. energy will be pumped into flywheel in cycles, but generator is hooked up to flywheel and it requires constant rotation speed.

My idea is to maintain constant speed of flywheel with variable radius. More power is pumped into flywheel than it is taken by generator, radius is increasing. Les power is pumped into flywheel than it is taken by generator, radius is decreasing.

My question is: how much energy I need for changing radius?

Just use: ΔKE = \frac{1}{2}\Delta (I\omega^2) = \frac{1}{2}\omega^2 ΔI

As the flywheel gives up energy it will slow down so to maintain rotational speed, mass must be pulled in toward the centre. As you add energy to the wheel, you have to less mass out to maintain speed.

If the mass distribution was always uniform throughout the disc:

ΔKE = \frac{1}{2}\omega^2 ΔI = \frac{m\omega^2}{4} (R_f^2-R_i^2)If the disk is not uniform, which this sounds like, you have to provide the details of the mass distribution in the wheel in order to calculate I and ΔI.

AM
 
let me just comment:

if I have X joules stored in flywheel with max radius, I need to spend all my energy of flywheel in order to move that mass to minimum radius!?

My idea is to maintain constant speed when flywheel is receiving and sending energy by changing inertia (radius). ... if I understood correctly from above formulas, that is not possible without taking a lot more energy from flywheel?

If flywheel loses ΔKE of its energy, his ω will also drop down. If I want to increase ω to the previous value (when energy was bigger, I would like to do it only by changing radius to smaller one.tnx
 
Last edited:
This could be complex. For a start, as stated by AM, if the distribution of mass of the flywheel is not equal then the calculations change.
How much energy is expended pulling the mass in or letting it out (relative to the KE of the system) is a dependent on other (non-disclosed) engineering decisions as to how you do this.
 
mic* said:
This could be complex. For a start, as stated by AM, if the distribution of mass of the flywheel is not equal then the calculations change.
How much energy is expended pulling the mass in or letting it out (relative to the KE of the system) is a dependent on other (non-disclosed) engineering decisions as to how you do this.

...I don't know why I did not simply made this drawing immediately, but now it is here: http://cdn.imghack.se/images/fb100c74f331a9b088e45039b8b775df.jpg

By moving that pink linear bearing (up and down) I would like to regulate flywheel inertia.
Is it possible to calculate how much energy I will need in order to move that bearing along the shaft, and how much force I will need in order to keep it in place?
 
miljacev said:
...I don't know why I did not simply made this drawing immediately, but now it is here: http://cdn.imghack.se/images/fb100c74f331a9b088e45039b8b775df.jpg

By moving that pink linear bearing (up and down) I would like to regulate flywheel inertia.
Is it possible to calculate how much energy I will need in order to move that bearing along the shaft, and how much force I will need in order to keep it in place?
I assume that the wheel will be balanced so that there is an equal mass diametrically opposite that undergoes the same change in radius.

You add energy to the wheel by applying a torque through an angle to the wheel. This causes the mass in the wheel to increase its tangential speed. If you do not change the distance of that mass from the centre of rotation, the rotational speed has to increase. However, if you then increase its moment of inertia by increasing that radius of rotation, you decrease the rotational speed (back to its original rotational speed) but maintain that increased tangential speed.

When you take energy from the wheel, the reverse applies. The wheel applies a torque through an angle which causes the mass to lose tangential speed. If you do not change the distance of that mass from the centre of rotation, the rotational speed has to decrease. If you then decrease the radius, you increase the rotational speed back to the original and maintain that decreased tangential speed.

If you make these changes in radius at the same as the wheel is slowing or speeding up, you don't use any energy in changing the radius. The force you will need for each m is the centripetal force: mω2r where ω=2πf where f = number of rotations per unit of time.

AM
 
  • #10
The description from the op remind me of a centrifugal governor, used to regulate the speed of steam engines.
But perhaps I am missing something?
 

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