50
2. THICK-ELECTRODE DEP FOR SINGLE-CELL 3D ROTATION
2.7.2 KEY FACTORS IN ELECTRICAL PROPERTY ANALYSIS
e rotation spectrum is mainly determined by four dielectric parameters (permittivity and con-
ductivity (ε
mem
, σ
mem
) of the cell membrane and permittivity and conductivity (ε
cyto
, σ
cyto
) of the
cytoplasm). e dielectric parameters of dierent cells are usually dierent. Without loss of gener-
ality, the cell diameter is set to 15 µm, the cell membrane thickness is set to 20 nm according the
literature [170], and the rotation spectrum curves related to these four parameters can be plotted
according to the parameter settings in Table 2.2.
Table 2.2: Cell dielectric parameter settings
Conductivity of
Cell Membrane
σ
mem
(μS/m)
Permittivity of
Cell Membrane
ε
mem
Conductivity of
Cell Cytoplasm
σ
cyto
(S/m)
Permittivity of
Cell Cytoplasm
ε
cyto
Figure 2.34(a) 1–10
12ε
0
0.4
100ε
0
Figure 2.34(b)
10
1–20ε
0
0.4
100ε
0
Figure 2.34(c)
10
12ε
0
0.1–1
100ε
0
Figure 2.34(d)
10
12ε
0
0.4
10–100ε
0
At the whole frequency range, the eect of conductivity of cell membrane on the rotation
spectrum is negligible (Figure 2.34(a)). When the frequency is < 100 MHz, the eect of permit-
tivity of cytoplasm on the rotation spectrum is negligible (Figure 2.34(b)). When the frequency is
< 100 MHz, permittivity of cell membrane and conductivity of cytoplasm have a signicant eect
on the rotation spectrum (Figure 2.34(c, d)). is experiment was limited by the signal generator
frequency range and the maximum frequency was 20 MHz. erefore, the method of extracting
the dielectric properties of cells can’t essentially distinguish conductivity of cell membrane and
permittivity of cytoplasm. erefore, in the experiment, the two parameters were set to 100ε
0
and
10
-6
S/m according to the literature [165].
e electrical parameters of the cell solution also have an eect on the cell rotation spectrum.
e permittivity and conductivity of the cell membrane were set to 12ε
0
and 10 µS/m, respectively,
and the permittivity and conductivity of the cytoplasm were set to 60ε
0
and 0.4 S/m, respectively.
Figure 2.35 shows the eect of solution permittivity and conductivity on the rotation spectrum.
It can be seen that the permittivity of the solution has signicant inuence on the rotation
spectrum only when the frequency is greater than 100 MHz, and has almost no eect on the ro-
tation spectrum when the frequency is lower than 100 MHz. e change in conductivity of the
solution has obviously inuence on the rotation spectrum over the whole frequency range, so a
lower conductivity (36.5 mS/m) solution was used in the experiment.