Bishopp, Hugh
asks:
CATAGORY: Thermodynamics
QUESTION: Devise an experiment to prove Charles' Law and hence determine
a value for absolute zero. I have considered using a fairly primitive
method of trapping air in a thin tube , putting it in a water bath and
then heating it, measuring the volume of the gas at various temperatures.
This is not very good - any suggestions
Back to catalog.
I remember doing this experiment when I was an undergraduate student.
The use of a tube is good BUT you want to multiply the effect. What
you are trying to do is measure a change in volume for with a change
in length. Your tube has a cross sectional area A so its volume is A
times l where lis the length the change in volume dV is then equal to
A times the change in length.
(1) dV = A dl
V = Al dV = A dl
_____________________________
()_____________________)______) A
|---------------------|------|
l dl
Since T ~ V then
New volume new temp.
---------- = ----------
Old volume old temp
Which translates to
(2) V(T+dT) T + dT
-------- = ------
V(T) T
Substitution of V =Al and dV = Al gives
(3) Al + Adl T + dT
-------- = -------
Al T
Cancelling the Area a gives
(4) l + dl T + dT
-------- = -------
l T
or
dl dT
(5) 1 + --- = 1 + ---
l T
Subtracting 1 from both sides gives
dl dT
(6) --- = ---
l T
So
dT
(6) dl = l ---
T
So if you have a small length bubble then dl will be very small since in
"classroom" conditions it is difficult to get a big change in dT /T
when t is in degrees Kelvin.
Now how about this instead. construct your tube apparatus as before
but attach a air filled container on one end. The volume of the
container is fixed so any gas that comes out as a result of expansion
will fill the tube.
V(box)
______
|\ \ V(tube) = Al dV = A dl
| \ \ ___________________________
| \ \____________________)______) A
\ \ \-------------------|------|
\ \_____\ l dl
\ | |
\| |
|_____|
Thus if Charles law works then again
New volume new temp.
---------- = ----------
Old volume old temp.
but this time we have
V(box) + V(tube) + Adl T + dT
(7) ---------------------- = -------
V(box) + V(tube) T
or
Adl dT
(8) 1 + ---------------- = 1 + ---
V(box) + V(tube) T
Subtracting 1 from both sides.
Adl dT
(9) --------------- = ---
V(box) + V(tube) T
Solving for dl
V(box) + V(tube) dT
(10) dl = ---------------- ---
A T
Now lets compare the difference between dl from (6) with no box to dl
from (10) with a box. Take the tube diameter to be 2mm so it has a
1mm (inner) radius then A = pi r^2 = 3.14 mm^2. Also suppose that the
length of your bubble l is 10mm. If the temperature change is say 50K
and room temperature is say 293K then dl from (6) is
50K
(11) dl = 10mm ----- = 1.7mm
293K
Which may be difficult to measure.
On the other hand suppose that we now use a box that is 2cm x 2cm x
2cm on a side to give V(box) = 8 x 10^3 mm^3. Then (10 ) gives us
8 x 10^3 mm^3 + 3.14mm^2 x 10mm 50K
(12) dl = -------------------------------- ----
3.14 mm^2 293K
= 436mm ~ .44 m (this is 256 times larger than with (6)!)
Thus a relatively small temp difference is greatly magnified so that
the data you take will be more accurate and you can do a better
extrapolation of the V vs T graph as T -> 0.
Back to catalog.