Leakage of Air in a Spacecraft

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  • #1
flyusx
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Homework Statement
A spacecraft measuring 8 m by 3 m by 3 m is struck by space junk leaving a circular hole of radius 4 mm. About how much time is left to patch the leak? Assume an ideal gas and STP (1 mol of atoms occupies 22.4 L).
Relevant Equations
Leakage: $$\frac{NA\bar{v}}{4V}$$
Boltzmann Distribution: $$\Pr(v)=4\pi\left(\frac{m}{2\pi k_{B}T}\right)^{\frac{3}{2}}v^{2}\exp\left(-\frac{mv^{2}}{2k_{B}T}\right)$$
The leakage equation is pretty straightforward to use once I found the average velocity: N is the number of atoms, A is the area of the hole, v-bar is the average velocity and V is the volume of the container.

To find the average velocity, I used the Boltzmann distribution. I set the temperature be 273.15 K. For mass, I used $$\frac{28.96 g}{1 mol}\frac{1 mol}{N_A atoms}\frac{1 kg}{1000 g}=\frac{4.808921063\cdot10^{-26} kg}{atom}$$I then used the Boltzmann distribution to find the average velocity by taking $$\frac{\int_{0}^{10000}v\Pr(v)\text{d}v}{\int_{0}^{10000}\Pr(v)\text{d}v}=446.8783872 m/s$$From the leakage formula, I just took the area of the hole to be $$A=\pi r^{2}=\pi\left(4\cdot10^{-3}\right)^{2}$$, N to be the number of atoms in a mol and V to be the volume of the container (multiplied by ##10^{-3}## to convert to cubic metres). This returned a leakage rate of ##1.509739807\cdot10^{23}## atoms per second.

To find the number of atoms in the spaceship, I used 1.293 kg/m^3 as the average density of air. $$\frac{1.293 kg}{m^{3}}72m^{3}\frac{28.96 g}{1 mol}\frac{1 mol}{N_A atoms}\frac{1 kg}{1000 g}=1.935902021\cdot10^{27}\text{ atoms}$$Dividing the total number of atoms by the leakage rate returns 213.7 minutes (over 3 hours). The textbook says the correct answer is about 2 hours.

What am I doing wrong?
 
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  • #2
I don't know if it helps, but the leakage rate should decrease as the pressure inside the spacecraft drops due to leakage. I'm not able to tell if you've accounted for that in your work.

Also, if I'm in that spacecraft, I'd want to patch the hole before the air pressure inside dropped to zero. Does the problem statement say what the pressure can drop to in that "time to patch the hole"?
 
  • #3
berkeman said:
I don't know if it helps, but the leakage rate should decrease as the pressure inside the spacecraft drops due to leakage. I'm not able to tell if you've accounted for that in your work.

Also, if I'm in that spacecraft, I'd want to patch the hole before the air pressure inside dropped to zero. Does the problem statement say what the pressure can drop to in that "time to patch the hole"?
I'm sorry, I should've been clearer. We ignore the drop in leakage rate and take the time to patch as until the ship is empty. Physics textbooks and their simplifying assumptions, I suppose.
 
  • #4
Hi @flyusx. A few thoughts....

flyusx said:
Homework Statement: A spacecraft measuring 8 m by 3 m by 3 m is struck by space junk leaving a circular hole of radius 4 mm. About how much time is left to patch the leak? Assume an ideal gas and STP (1 mol of atoms occupies 22.4 L).
A key word here is 'About'. It indicates that you don't need to work to great precision (such as ##446.8783872 m/s##).

flyusx said:
Relevant Equations: Leakage: $$\frac{NA\bar{v}}{4V}$$
Not familiar with that equation – can you give explanation or reference (in particular for the '4')?

flyusx said:
The leakage equation is pretty straightforward to use once I found the average velocity: N is the number of atoms, A is the area of the hole, v-bar is the average velocity and V is the volume of the container.
The average velocity of the particles is zero because velocity is a vector and directions are random in 3D! I guess you mean average speed.

For an approximate calculation of this sort, you would typically use the RMS (root mean square) velocity or the average speed. There are simple, standard formulae for RMS velocity and for average speed which you may be expected to use (rather than using the Boltzmann distribution and integrating!).

flyusx said:
We ignore the drop in leakage rate and take the time to patch as until the ship is empty. Physics textbooks and their simplifying assumptions, I suppose.
Ignoring the drop in leakage rate is (IMO) a terrible (unphysical) thing to do! Also, it wasn't mentioned in the original (Post #1) question, indicating that you didn't post the full/accurate question.
 
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  • #5
Steve4Physics said:
Hi @flyusx. A few thoughts....


A key word here is 'About'. It indicates that you don't need to work to great precision (such as ##446.8783872 m/s##).


Not familiar with that equation – can you give explanation or reference (in particular for the '4')?


The average velocity of the particles is zero because velocity is a vector and directions are random in 3D! I guess you mean average speed.

For an approximate calculation of this sort, you would typically use the RMS (root mean square) velocity or the average speed. There are simple, standard formulae for RMS velocity and for average speed which you may be expected to use (rather than using the Boltzmann distribution and integrating!).


Ignoring the drop in leakage rate is (IMO) a terrible (unphysical) thing to do! Also, it wasn't mentioned in the original (Post #1) question, indicating that you didn't post the full/accurate question.
Thank you very much. I haven't a clue as to where 1/4 comes from. My textbook effectively states that it's 1/4 for 'complicated math reasons we won't discuss here' and that a full derivation can be found in a statistical mechanics textbook. You are correct that I meant average soeed, not velocity (and not rms speed for the textbook explicitly states average speed).

I included all the decimal points because I was working inside Maple and would always just round off the answers at the very end instead of at intermediate steps.

I agree that ignoring the drop in leakage rate doesn't make sense. The problem, which I should have stated, states 'state what simplifying assumptions you make' which in my opinion is very vague.
 
  • #6
flyusx said:
I agree that ignoring the drop in leakage rate doesn't make sense. The problem, which I should have stated, states 'state what simplifying assumptions you make' which in my opinion is very vague.
First note that different ‘reasonable assumptions’ will lead to different answers. In fact 2 hours and 3 hours are pretty close! But your approach is based on incorrect physics so wouldn't gain marks.

The solution should start with a clear statement of any necessary reasonable assumptions. The assumption that the rate of particle loss is constant is (IMO) unreasonable.

My solution would be something like this (hope I’m not giving too much away):

Assumptions:

1) The occupant has no breathing apparatus but can remain conscious and work until the pressure is about 0.5atm.

2) The internal temperature remains constant so the internal pressure is proportional to the remaining number of air particles.

Strategy:

Use the given formula for rate of particle loss: ##\frac {dN}{dt} = - \frac {NA \bar v}{4V}##. This describes a simple exponential decay process. ##N(t)## is easily found by integration.

Average particle speed is given by standard equation ##\bar v = \sqrt {\frac {8RT}{\pi M}}##.

Using the equation for ##N(t)## find the time for the ##N## to halve (which corresponds to pressure falling from 1atm to 0.5atm). If you know how to find half-life from a decay constant, this will save a line or two of working.

If you can, work symbolically and evaluate at the end.

Edited as text and LaTeX got badly corrupted somehow.
 
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  • #7
Steve4Physics said:
The assumption that the rate of particle loss is constant is (IMO) unreasonable.
Agreed; what the question is effectively asking for is the number of molecules divided by the initial rate of loss of molecules.

Here’s how I reasoned:
Let the width of the box in the x direction be ##s_x##, the velocity of molecule ##i## in the x direction have magnitude ##v_{ix}##, and the box volume be ##B##; similarly y, z.
Let the hole be in a wall normal to the x axis. The hole's fraction of that wall is ##\frac{As_x}V##.
(Typo fixed.)
Frequency at which a given molecule hits where the hole will appear is ##\frac{v_{ix}}{2s_x}\frac{As_x}V=\frac{v_{ix}}{2}\frac{A}V##.
Rate of loss of molecules = ##\Sigma_i\frac{v_{ix}}{2}\frac{A}V##.
If the overall speed of a molecule is ##u_i## then, on average, its x direction speed will be ##\frac 12u_i##.
Average (over the molecules) rate of loss = ##\frac{\bar{u_{i}}}{4}\frac{A}V##.
But note that ##\bar{u_i}## is not the RMS speed. Rather, it is calculated by the Boltzmann formula in post #1, which is there evaluated at 447m/s.
Based on this as the constant rate of loss, the time to lose all the molecules is ##4\frac V{A\bar{u_i}}##, or about 3 hours.
 
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  • #8
haruspex said:
what the question is effectively asking for is the number of molecules divided by the initial rate of loss of molecules.
Maybe! The (very badly posed) question simply asks "About how much time is left to patch the leak?" which, in the absence of any further information, is open to widely different interpretations.

haruspex said:
Let the hole be in a wall normal to the x axis. The hole's fraction of that wall is ##\frac{As_i}V##.
Typo'? ##\frac{As_i}V## should be ##\frac{As_x}V##.

haruspex said:
If the overall speed of a molecule is ##u_i## then, on average, its x direction speed will be ##\frac 12u_i##.
Wouldn't the average x-direction speed be ##\frac 1{\sqrt 3}u_i## because ##\vec u_i## has three orthogonal components which are equal on average?
 
  • #9
I don't understand why this is being worked as a statistical mech problem. Wouldn't the air be driven out the hole by the pressure difference between the spacecraft (Po=1 atm) and the vacuum of space?

I tried using choked (sonic) flow (343 m/s at STP) through the 4 mm hole; I get 4.6 hours to empty the spacecraft. Assuming the velocity doesn't drop off. I was surprised that my result is longer than the ~3 hours being calculated above.
 
  • #10
gmax137 said:
I don't understand why this is being worked as a statistical mech problem.
I'd guess it's a teaching-exercise set in the context of the material being taught.

gmax137 said:
Wouldn't the air be driven out the hole by the pressure difference between the spacecraft (Po=1 atm) and the vacuum of space?
Yes - initially. The initial pressure-difference is 1atm but immediately starts to fall.

gmax137 said:
I tried using choked (sonic) flow (343 m/s at STP) through the 4 mm hole; I get 4.6 hours to empty the spacecraft. Assuming the velocity doesn't drop off. I was surprised that my result is longer than the ~3 hours being calculated above.
I'd guess the exit velocity is more or less constant. But since the density of the air inside falls, the mass flow-rate will also fall.
 
  • #11
Steve4Physics said:
But since the density of the air inside falls, the mass flow-rate will also fall.
Yes, but that means that my 4.6 hours is a minimum time required. I am surprised that the time based on molecules bumping around and happening to hit the hole is less. Or have I misunderstood the posts above mine.
 
  • #12
Steve4Physics said:
Maybe! The (very badly posed) question simply asks "About how much time is left to patch the leak?" which, in the absence of any further information, is open to widely different interpretations.
Except that post #3 adds that the leak rate is to be treated as constant.
Steve4Physics said:
Typo'? ##\frac{As_i}V## should be ##\frac{As_x}V##.
Yes, thanks.
Steve4Physics said:
Wouldn't the average x-direction speed be ##\frac 1{\sqrt 3}u_i## because ##\vec u_i## has three orthogonal components which are equal on average?
In two dimensions, the average value of ##\cos(\theta)## between ##0## and ##\pi/2## is ##2/\pi##, not ##1/\sqrt 2##. In 3D, we can use Archimedes' observation that a band on the surface of a sphere between ##x## and ##x+\delta x## has the same area as its projection onto the enclosing cylinder sharing the x axis.
https://mathspace.co/textbooks/syllabuses/Syllabus-451/topics/Topic-8309/subtopics/Subtopic-109173
Edit: In n dimensions, expressing it as a general formula involves gamma functions, just as for volumes and areas of n-dimensional spheres.
Edit 2:
Maybe it can be simplified, but I get that the distance from the origin to the mass centre of an n-dimensional unit hemisphere centred at the origin is
##\frac{n+1}{n\sqrt\pi}\frac{\Gamma(\frac n2+1)}{\Gamma(\frac n2+\frac 32)}##.
That gives n=1: 1, n=2: 2/π, n=3: 1/2, all of which appear to be correct.

Asymptotically that would be ##\sqrt{\frac 2{n\pi}}##.
gmax137 said:
Wouldn't the air be driven out the hole by the pressure difference between the spacecraft (Po=1 atm) and the vacuum of space?
Sure, but that’s just another approach. The molecular view is valid, and arguably more obviously so. Using concepts like pressure and energy is a macroscopic view, and can have limitations. If the answers don’t match, I would trust the reductionist view.
 
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  • #13
haruspex said:
If the answers don’t match, I would trust the reductionist view
My previous answer 4.6 hr is based on my misreading of the hole size as 4mm diameter, where it's really 4mm radius. So I should have gotten 4.6/4 = 1.15 hours. So the most untrustworthy bit is my reading comprehension.
 
  • #14
Steve4Physics said:
Wouldn't the average x-direction speed be ##\frac 1{\sqrt 3}u_i## because ##\vec u_i## has three orthogonal components which are equal on average?
That would give the textbook answer of about 2 hours I believe.
 
  • #15
I've come back and worked with haruspex's method of writing it as a differential equation (which to me makes more sense) which generated an answer that was more realistic and one for which I feel better about. The question seems to be badly posed as Steve4Physics pointed out. Thanks all!
 
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  • #16
flyusx said:
N to be the number of atoms in a mol and V to be the volume of the container
I did not see it mentioned, but this is incorrect. You either need to take N to be the number of atoms in the container and V to be the volume of the container or N to be the Avogadro number and V the molar volume of the gas. The main point being that ##N/V## should be the number density of the molecules - which is what the leak rate will depend on. Otherwise you could have a very very large container and get much lower leakagd even if the conditions around thd leak are the same.

Another reason I do not like this problem is that the problem author clearly has no insight into how breathable air in a spacecraft works. Regular air at STP in a volume of 8x3x3 m^3 would contain about 17 kg of oxygen. An astronaut needs about 1 kg of oxygen per day and the partial pressure needs to be kept around the same. A crew of 4 and those astronauts are dead in 4 days without leaks. (On actual spacecraft oxygen is stored in tanks and released continuously to maintain partial pressure)

See eg https://www.esa.int/Science_Exploration/Human_and_Robotic_Exploration/Orion/Air_and_water
 
  • #17
Orodruin said:
I did not see it mentioned, but this is incorrect. You either need to take N to be the number of atoms in the container and V to be the volume of the container or N to be the Avogadro number and V the molar volume of the gas. The main point being that ##N/V## should be the number density of the molecules - which is what the leak rate will depend on. Otherwise you could have a very very large container and get much lower leakagd even if the conditions around thd leak are the same.
Sorry for the mistype. I'm used to ##N## standing for the total number of atoms but evidently my brain was somewhere else. Thanks!
 
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