Kinetic energy of wheel/tyre when braking

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Discussion Overview

The discussion revolves around the kinetic energy of wheels and tires during braking, specifically addressing the calculations and implications of both linear and rotational kinetic energy in the context of a car's total energy when coming to a stop. Participants explore the contributions of the wheels to the overall kinetic energy and how to properly account for it in calculations.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant calculates the total kinetic energy of a 1000kg car and its wheels, suggesting that the energy from the wheels should be added to the car's kinetic energy for a total energy removal of 678kJ.
  • Another participant challenges the initial calculations, stating that the "rolling mass" of the wheels should be considered as half the actual mass of the wheels.
  • A participant provides a rule of thumb indicating that the rotational effects of wheels, tires, and brakes should add an equivalent of 5% of the total mass of the car.
  • Further calculations are presented regarding the rotational kinetic energy of a single wheel, including the moment of inertia and the radius of gyration.
  • Some participants discuss the complexity of mass distribution in wheels, arguing that it cannot be simplified to a disc model and that the calculations must account for the actual distribution of mass.
  • There is a suggestion that the mass of the wheels is already included in the car's mass, leading to a debate on how to properly calculate the total kinetic energy.

Areas of Agreement / Disagreement

Participants express differing views on how to calculate the kinetic energy contributions of the wheels, with no consensus reached on the correct approach or the validity of the initial calculations. Multiple competing views remain regarding the treatment of the wheels' mass and energy contributions.

Contextual Notes

Participants highlight limitations in assumptions regarding mass distribution and the complexity of calculating rotational inertia, indicating that the calculations may depend on specific definitions and conditions that are not universally agreed upon.

Kozy
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I have been doing some working on braking energies, and have hit a bit of confusion with regards to the kinetic energy of the wheels and tyres.

Obviously, the kinetic energy of the moving car itself follows the old rule of 1/2mv2.

For a 1000kg car at 30ms that's then 450kJ.

I have then calculated the kinetic energy of a 12kg wheel/tyre with a rolling diameter of .575m, assuming the 'centre of mass' to be at 75% of the rolling radius as 57kJ. (30ms = 105 rad/s)

This seems substantial addition to the total kinetic energy over four wheels. Now, assuming I have not made a big mistake (I may well have done), should that 228kJ be added to the 450kJ of the moving vehicle, giving me a total of 678kJ of energy that must be removed from the car to bring it to a standstill? Or is it somehow absorbed into the 450kJ?
 
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Hi Kozy! :smile:

I haven't checked your calculations,

but they must be wrong, since the "rolling mass" of the wheels should be half the actual mass of the wheels.
 
tiny-tim said:
Hi Kozy! :smile:

I haven't checked your calculations,

but they must be wrong, since the "rolling mass" of the wheels should be half the actual mass of the wheels.

Could you expand on this? I am not familiar with that...
 
If you do all the calculations, you find that a rolling object of mass m, moment of inertia I, and rolling radius r, behaves like an object of total mass m + mr,

(eg a force F will give it a linear acceleration of F/(m + mr))

where mr is the rolling mass, or equivalent mass, equal to I/r2 :smile:

(and so mr for a uniform disc = m/2)
 
a hollow disc , yes, but a solid disc, no. I =1/2Mr^2 vs I =MR^2
hollow disc acts like 2x the mass Is sitting in the car,
solid might be as low as 1.3x the mass as if it was sitting in the car, depending on the mass distribution of the disc.
 
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The mass of the wheels is included in the mass of the car, so calculate the linear KE @ ½ * 1000 * 30 ²
Now calculate the rotational KE of 1 wheel at 30 m/s:
Start with the rolling radius (r) : = 0.2875 m
The radius of gyration (k) = 0.75 * 0.2875 = 0.2156 m
The moment of inertia (i) = m * k ² = 0.5579 kg-m ²
The rortation rate (w) at 30 m/s = v/r = 30 / 0.2875 = 104.35 rad/sec
The rotational KE at 30 m/s = ½ * i * w ² = 3,037.5 J
Multiply by 4:
12,150 J
Add to linear KE
 
dean barry said:
The mass of the wheels is included in the mass of the car, so calculate the linear KE @ ½ * 1000 * 30 ²
Now calculate the rotational KE of 1 wheel at 30 m/s:
Start with the rolling radius (r) : = 0.2875 m
The radius of gyration (k) = 0.75 * 0.2875 = 0.2156 m
The moment of inertia (i) = m * k ² = 0.5579 kg-m ²
The rortation rate (w) at 30 m/s = v/r = 30 / 0.2875 = 104.35 rad/sec
The rotational KE at 30 m/s = ½ * i * w ² = 3,037.5 J
Multiply by 4:
12,150 J
Add to linear KE
You have calculated all that weight to be at the tire, not the wheel. if the wheel and it is distributed like a disc, then "I" is 1/2mr^2
if you did it correct, the KE of the weight at the outer diameter vs weight in the car would be equal and additive.
 
It can't be considered a disc. The mass distribution isn't that simple.
But if you have the radius of gyration and mass you can calculate the moment of inertia, with that and the rolling radius you can calculate the rotational KE.
Each wheel has both linear and rotating KE.
 
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dean barry said:
It can't be considered a disc. The mass distribution isn't that simple.
But if you have the radius of gyration and mass you can calculate the moment of inertia, with that and the rolling radius you can calculate the rotational KE.
Each wheel has both linear and rotating KE.
I know ,that's why I said it the inertial of the weight if on the tire, is like a hollow disc, and I would be I=MR^2. that weight would be like if the mass was attached on a mass less radius cord, and its center was close to the OD of the tire. (so its going to be a little off due the width (thickness of the tire... or in other words, all the mass is not at the outer diameter, its down toward the center slightly, thus it is not a 'slippless" calculation vs the linear KE equiv. (so slightly less than the linear KE)
However, the wheel could be considered a Disc, and use I=1/2MR^2, if the mass is evenly distributed . best case even if it was, the rotational KE would be less than 1/2 that of the linear KE. (depending on the wheel diameter vs the overall wheel and tire diameter)
 

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