The user must specify the initial and final volume, the number of samples and time interval between them. This last option indirectly defines the speed at which the transformation occurs.
If the experiment is executed with a o long time interval between samples, the transformation is isothermal. That means the air temperature inside the syringe doesn't change, and the Boyle-Mariotte Law is applicable.
The example bellow is such a case, where we can verify that the product pV is, in average, 49,3±0,3l.kPa, close to the theoretical value of nRT (where n=2×10−4mol, equivalent to the full syringe volume when in rest 5ml, PTN).
[fig.2]
If the time between samples is decreased (i.e. the process is faster), the transformation is no longer isothermal and becomes slight adiabatic, because there is not enough time for heat exchange between the inside of the cylinder and the environment. In this way, the compression no longer follows the Boyle-Mariotte, a fact that is clearly demonstrated by the deviation from the power function, which would be 3/5 in the ideal case (γ−1=cvcp).
It is, however, difficult to obtain a fast enough compression to achieve this value, since thermalization occurs quickly (in the order of the speed of sound), but this can be used to study how the speed of the transformation influences the deviation between the experimental data and Boyle-Mariotte Law.