Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
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48 Experimental techniques and observables<br />
viscous liquids. Particularly the studies of relaxation time as a function of pressure,<br />
which have lead to the scaling law presented in section 3.2 are to a very high degree<br />
obtained by dielectric spectroscopy. The drawback of dielectric spectroscopy, is that<br />
the exact relation between the macroscopic measured quantity and the microscopic<br />
dynamics is not totally understood. Also the relation between dielectric relaxation<br />
and other more fundamental macroscopic properties, such as the frequency dependent<br />
shear response remains unresolved.<br />
In this section we present the basic principle of the dielectric spectroscopy as well as<br />
give a brief discussion of the physical interpretation. The details of our experimental<br />
setup are given in section 5.1.1.<br />
4.2.1 Basic principle<br />
The basic principle of dielectric spectroscopy is the measurement of a frequency dependent<br />
capacitance of a capacitor filled by the sample. The measuring capacitance<br />
is usually made up of two equally sized parallel plates. This gives the following<br />
capacitance of the empty capacitor,<br />
C 0 = ǫ 0A<br />
d , (4.2.1)<br />
where ǫ 0 is the vacuum permittivity, A is the area of the electrodes and d is the<br />
distance between the plates. The capacitance of the capacitor filled sample with<br />
sample is given by<br />
C(ω) = ǫ(ω) ǫA d = ǫ(ω)C 0 (4.2.2)<br />
where ǫ(ω) is the frequency dependent dielectric constant of the sample. Hence,<br />
ǫ(ω) is determined by dividing the frequency dependent capacitance of the filled<br />
capacitor by the capacitance of the empty capacitor.<br />
The dielectric constant, ǫ, of a sample is defined from the ratio between the applied<br />
electric field, E, and the displacement field, D,<br />
P = ǫ 0 χE m , D = P + ǫ 0 E m = ǫ 0 (χ + 1)E m = ǫ 0 ǫE m , (4.2.3)<br />
where P is the polarization per unit volume. Thus, ǫ(ω) is the response function (see<br />
section 4.1.1), when the applied macroscopic field is the input and the displacement<br />
field is the output.<br />
The experiments reported and discussed in this study are all performed with low