23.11.2014 Views

Ph.D. thesis (pdf) - dirac

Ph.D. thesis (pdf) - dirac

Ph.D. thesis (pdf) - dirac

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!