Calculating RPM Required to Simulate Earth Gravity on 100m Space Habitat

  • Thread starter galoshes
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In summary: So the spin rate you need to create a 100m diameter space habitat with Earth-style gravity is 2*pi/60*rad/sec. In summary, you would need to spin the donut-shaped space habitat at 2*pi/60*rad/sec in order to simulate the Earth's gravity on it.
  • #1
galoshes
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So i was presented this question and I would not even like the answer but just the path to walk on. Can you help?

In order to simulate the Earth gravity on a space habitat of 100m diameter, what spin rate of a donut-shape space habitat, in terms of RPM, should be.

conversion of RPM is 2(pi)/60 radians/sec

where do I even begin?
 
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  • #2
I think you should look into the radial acceleration of a rotating body and the "centrifugal force" associated with a body rotating in a circle. Any freshman physics text could help. An extended (large) donut would be difficult to use though...

Good luck!
 
  • #3
There is no centrifugal force. Instead, you want the normal force exerted on the people inside the space colony to match the normal force that a person on Earth would experience.

A "weight" scale is really nothing more than a normal force o'meter. And when a person steps on a weight scale on flat land with no acceleration, then N - mg = 0 (Newton's second law) so that N = mg. (NEVER ASSUME N = MG! USE NEWTON'S SECOND LAW TO PROVE IT.)

So you want N = mg on the space colony as well. Find the spin rate that produces that amount.

If you need more help, let us know. But try to finish the problem off to the best of your ability first.
 
  • #4
galoshes I do not want to spoil your fun, so don't look if you haven't satisfied yourself yet.

JohnDubYa said:
There is no centrifugal force. Instead, you want the normal force exerted on the people inside the space colony to match the normal force that a person on Earth would experience.

...

So you want N = mg on the space colony as well. Find the spin rate that produces that amount.

Are we not saying the same thing? The g produced by the rotation of the donut would be the same as the radial (centripital) acceleration caused by rotation in a circular path. Something else which confuses me: wouldn't the mass of the the donut produce some gravitational force, and thus acceleration? I thought since the dounout is not spherical, then you can't consider it's mass to effectively be located at the geometric center!
 
  • #5
Yes, we are saying pretty much the same thing.

RE: "The g produced by the rotation of the donut would be the same as the radial (centripital) acceleration caused by rotation in a circular path."

But this brings up the problem we are discussing in a separate thread: The person in the colony is radially accelerating, but the person on the Earth is not (to any significant extent). So if you tell them to produce a radial acceleration equal to g, then that is going to confuse the Hell out of them. That is why I prefer to talk in terms of normal force instead of acceleration. And this makes even more sense if you think about what actually happens when you weigh yourself. You are not measuring g, or even m*g. Instead you are measuring the normal force.

Even if you define weight as w = mg, a bathroom scale is not a weight scale. It measures the normal force, which happens to equal mg in some situations.

We can ignore the mass of the donut, since the gravitational attraction of the two bodies is negligible. After all, it takes an object having the mass of the Earth to produce a force of mg on the person.
 

1. How do you calculate the RPM required to simulate Earth gravity on a 100m space habitat?

The formula for calculating RPM (revolutions per minute) required to simulate Earth gravity on a 100m space habitat is: RPM = √(G x M / R) / 2π, where G is the gravitational constant (6.67 x 10^-11 Nm^2/kg^2), M is the mass of the space habitat (in kg), and R is the radius of the space habitat (in meters). This formula is based on the centripetal force required to simulate Earth's gravity, which is provided by the rotation of the habitat.

2. What factors influence the RPM required for Earth gravity simulation on a 100m space habitat?

The RPM required for Earth gravity simulation on a 100m space habitat is influenced by three main factors: the gravitational constant, the mass of the habitat, and the radius of the habitat. As the mass and radius of the habitat increase, the RPM required for Earth gravity simulation also increases. Additionally, the higher the gravitational constant (which varies depending on the units used), the lower the required RPM.

3. Can you calculate the RPM required for other gravity simulations on a 100m space habitat?

Yes, the same formula can be used to calculate the RPM required for other gravity simulations on a 100m space habitat, as long as the desired gravity is known. For example, if you wanted to simulate Mars gravity (0.38g) on a 100m space habitat, you would simply plug in the corresponding gravitational constant for Mars (4.3 x 10^-3 Nm^2/kg^2) into the formula.

4. Are there any limitations to using RPM as a means of simulating gravity on a space habitat?

Yes, there are limitations to using RPM as a means of simulating gravity on a space habitat. One limitation is the potential for motion sickness or disorientation due to the constant rotation of the habitat. Additionally, the required RPM may be difficult to achieve and maintain, especially for larger habitats. Alternative methods, such as using a centrifuge, may be more practical for simulating gravity on a space habitat.

5. How accurate is using RPM to simulate Earth gravity on a 100m space habitat?

The accuracy of using RPM to simulate Earth gravity on a 100m space habitat depends on the precision of the calculations and the stability of the habitat's rotation. Small variations in the RPM can result in noticeable differences in the simulated gravity. Additionally, factors such as air resistance and the distribution of mass within the habitat can also affect the accuracy of the simulation. Therefore, it is important to carefully consider and account for all factors when using RPM to simulate gravity on a space habitat.

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