Charles' Law II - Pressure vs. Temperature (This is the Guy Lussac Law).
By
Choong Teow
Introduction:
Guy-Lussac's Law, which describes a pressure-temperature relationship, states that the

pressure of a gas at constant volume is directly proportional to the absolute temperature. The

following equation express the Guy-Lussac's Law, where "P" is the pressure and "T" is the

temperature:

The following experiment shows that the dependence of pressure on temperature of dilute

gases with a constant volume is linear for all gases (Gay-Lussac's law). When the pressure vs.

temperature curve is extrapolated to very low  temperature, one finds that the pressure is zero

when the temperature is -273.15°C. This significant temperature is used as the basis for the

Kelvin (or absolute) temperature scale, which sets -273.15°C as its zero point (0 K or absolute

zero). The size of a Kelvin unit (called a kelvin) is the same as the size of a degree on the

celsius scale. Thus, the relationship of conversion between the temperatures is simply  Tc =

Tk  - 273.15. The meaning of absolute zero becomes clear from the kinetic molecular theory

of the ideal gas. Since the pressure of an ideal gas is proportional to the average kinetic energy

of the molecules, when the pressure goes to zero there is no motion of the gas molecules, and

the temperature is at absolute zero.

Procedure:
The Erlenmeyer flask was assembled, and it was connected to the electronic pressure

transducer - no syringe.  This keeps the volume constant.  The pressure sensor and the

temperature sensor was connected to the computer. The computer was set up to record

temperature and pressure in event mode. While the measurement was being taken,at least 30

minutes of data acquisition was allowed. The horizontal axis of the graph was set to

temperature and vertical axis to pressure (one volt = one atmosphere). The calibration file that

matches the probe was loaded. The flask was immerged in a large jar of hot (100 deg C) water

and data was begun to be recorded. The apparatus was set up as shown in the diagram below:

 In event mode the data was not recorded until the the "keep" button was pressed. Ice was

added gradually to the jar of water to cool the system to 0 deg C. while the acquisition system

is running. The pressure at liquid Nitrogen temperature was obtained.  During this step, the

electronic temperature probe should not be immersed in the liquid nitrogen.  The pressure of

liquid Nitrogen was used to determine the temperature. The pressure vs.temperature graph was

plot, and the absolute zero was determined. This value was compared to the standard value of

absolute zero. The pressure at liquid Nitrogen temperature was obtained, and this value was

used to determine the temperature of liquid Nitrogen. Precaution step were taken whereby the

electronic temperature probe was not immerse in the liquid nitrogen.
 

Results:
The plot of pressure vs. temperature is as shown below:

Data:
Time (minute) Temperature (degree) Potential (volt)
6.07 0.114 0.876
5.99 0.185 0.876
10.80 9.027 0.904
12.00 12.093 0.914
14.80 21.861 0.946
17.80 32.414 0.979
21.40 43.894 1.010
25.30 55.445 1.050
28.60 63.716 1.080
33.00 74.412 1.110
37.40 83.752 1.140
43.00 91.738 1.170

This experiment has proven TheGay-Lussac’s Law which says that when the volume is kept

constant, the absolute pressure of a given amount of any gas varies directly with the

thermodynamic temperature. Therefore, as the temperature increases, the pressure also

increases. From the graph, the absolute zero is around –295 degree C when the pressure is

zero. Therefore the absolute zero is rather close to the standard value of absolute zero. The

temperature of liquid nitrogen is around 200 degree C when the pressure is around 0.25V .

Conclusion:
This experiment was considered successful because the result has proven Charles' Law II

(Guy Lussac Law) which state that the pressure of a gas at constant volume is directly

proportional to the absolute temperature. At constant volume, when the temperature of a gas

increases, the pressure of the gas also increases proportionally.
 


Acknowledgement:
Dr. Don Collins for the guidance and teaching.
Mika Tanioka for working on the experiment together.
All physics II coursemates.
Ronald Sebilo-Tibbits.