A monatomic gas is adiabatically compressed

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Homework Help Overview

The discussion revolves around the adiabatic compression of a monatomic gas, focusing on the relationships between pressure, volume, temperature, and root mean square velocity (vrms) during the process. Participants explore the implications of the adiabatic condition and the behavior of the gas under compression.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants attempt to apply relevant equations for pressure and vrms but express uncertainty about their calculations. Questions arise regarding the relationship between temperature and vrms, as well as the implications of adiabatic processes on these variables. Some participants also question the constancy of specific heat and the mean free path in relation to volume changes.

Discussion Status

The discussion is ongoing, with various participants sharing their findings and interpretations. Some have provided insights into the relationships between temperature, volume, and vrms, while others seek clarification on specific calculations and concepts. There is a mix of attempts to derive equations and understand the underlying principles without reaching a definitive conclusion.

Contextual Notes

Participants note constraints such as the need for specific formulas and the challenge of interpreting the problem correctly. There is also mention of the impact of homework rules on the discussion, as some participants express frustration over grading based on specific answer formats.

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http://img198.imageshack.us/img198/1122/masteringphysicsscreens.jpg

p = ((1/3)*(N/V))*mv^2

vrms = squareroot ((3p)/(N/v))

i tried substituting .125 into the equation to get some numbers, didn't get anything useful

can someone show me the formulas that i have to use, and how to use them? or explain how to solve this problem

cheers
 
Last edited by a moderator:
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anyone?
 
vorcil said:
http://img198.imageshack.us/img198/1122/masteringphysicsscreens.jpg

p = ((1/3)*(N/V))*mv^2

vrms = squareroot ((3p)/(N/v))

i tried substituting .125 into the equation to get some numbers, didn't get anything useful

can someone show me the formulas that i have to use, and how to use them? or explain how to solve this problem

If the question called for an actual calculation (I am not sure it does), you would use the adiabatic condition :

[tex]PV^{\gamma} = constant[/tex] or:

[tex]TV^{\gamma -1} = constant[/tex]

In other words, these quantities remain unchanged in an adiabatic process.

Since work is done on the gas, what can you say about the temperature after adiabatic compression (apply first law)? How does vrms relate to temperature?

Would the specific heat Cv change? (remember, the gas is ideal).

What does the mean free path mean? How would it change with reduced volume?

AM
 
Last edited by a moderator:
Andrew Mason said:
If the question called for an actual calculation (I am not sure it does), you would use the adiabatic condition :

[tex]PV^{\gamma} = constant[/tex] or:

[tex]TV^{\gamma -1} = constant[/tex]

In other words, these quantities remain unchanged in an adiabatic process.

Since work is done on the gas, what can you say about the temperature after adiabatic compression (apply first law)? How does vrms relate to temperature?

Would the specific heat Cv change? (remember, the gas is ideal).

What does the mean free path mean? How would it change with reduced volume?

AM


since those values were constant and work is done on the gas, i would expect the temperature to decrease as the volume of the gas decreases to keep the thermal energy constant,

if the temperature decreases, i don't think anything happens to the vrms of the gas, because i looked through the book at the vRms of a gas section and the formulas have nothing to do with temperature (though I'm sure they do)

hangon i'll just google it
 
ok i found in my book

P = f/a
= 1/3 * N/V * MVrms squared

n/v = p / boltzmanC * temperature

so the volume is inversely proportional to temperature as was my guess, if volume decreases the temperature increases
 
Andrew Mason said:
If the question called for an actual calculation (I am not
Would the specific heat Cv change? (remember, the gas is ideal).

AM

they are constant?
 
vorcil said:
ok i found in my book

P = f/a
= 1/3 * N/V * MVrms squared

n/v = p / boltzmanC * temperature

so the volume is inversely proportional to temperature as was my guess, if volume decreases the temperature increases

oh that was the volume not vrms

i found the equation 1/2m * vrms^2 = 3/2 kb t

which means the average root mean square velocity is directly proportional to temperature

3/2 T with kb being boltz's constant, if it decreases, the velocity decreases aswell
 
bah i failed this question and only got two of the awnsers right

i knew that the heat specific ratio was constant so it was 1,

i got for the first question 2.07 instead of 2.00 and because it's mastering physics i failed that question
i got that from ln(1/.125) for an adiabatic process

the other two awnser for B and C
were lavender = .125 (not sure why the mean free path was the same as the volume percentage it was reduced too
and C was 4,

no idea how the first three awnsers came around for
part a b and c

could someone please show the maths behind it, and the way to those awnsers? I've already finished the question so i just need someone to explain it without asking a question ^ ^
 
vorcil said:
bah i failed this question and only got two of the awnsers right

i knew that the heat specific ratio was constant so it was 1,

i got for the first question 2.07 instead of 2.00 and because it's mastering physics i failed that question
i got that from ln(1/.125) for an adiabatic process

the other two awnser for B and C
were lavender = .125 (not sure why the mean free path was the same as the volume percentage it was reduced too
and C was 4,

no idea how the first three awnsers came around for
part a b and c

could someone please show the maths behind it, and the way to those awnsers? I've already finished the question so i just need someone to explain it without asking a question ^ ^

Since [itex]TV^{\gamma - 1}[/itex] does not change:

[tex]T_fV_f^{\gamma-1} = T_iV_i^{\gamma-1}[/tex]

So:

[tex]\frac{T_f}{T_i} = \frac{V_i^{\gamma-1}}{V_f^{\gamma-1}}[/tex]

since Vi/Vf = 8 and [itex]\gamma = 5/3[/itex]:

[tex]\frac{T_f}{T_i} = 8^{2/3} = 4[/tex]

So the internal energy increases by a factor of 4 and since [itex]v_{rms}^2 \propto T[/itex], the vrms increases by a factor of 2.

[tex]v_{rms-f} = 2v_{rms-i}[/tex]

AM
 
  • #10
Andrew Mason said:
Since [itex]TV^{\gamma - 1}[/itex] does not change:

[tex]T_fV_f^{\gamma-1} = T_iV_i^{\gamma-1}[/tex]

So:

[tex]\frac{T_f}{T_i} = \frac{V_i^{\gamma-1}}{V_f^{\gamma-1}}[/tex]

since Vi/Vf = 8 and [itex]\gamma = 5/3[/itex]:

[tex]\frac{T_f}{T_i} = 8^{2/3} = 4[/tex]

So the internal energy increases by a factor of 4 and since [itex]v_{rms}^2 \propto T[/itex], the vrms increases by a factor of 2.

[tex]v_{rms-f} = 2v_{rms-i}[/tex]

AM

Thanks, i actually figured it out in the end by myself :) Almost exactly the same way as you did XD
cheers
 

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