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Table 2 The table shows the relative frequency change, by adding 0.5 μm to the liquid film thickness h . Considering the \(\pmb{f_{0}}\) listed in Table  3 , these numbers represent frequency changes of the order 10 \(\pmb{^{2}}\) -10 \(\pmb{^{3}\mbox{ Hz}}\)

From: Reconstruction of annular bi-layered media in cylindrical waveguide section

Mode

Relative tunability h  = 1 mm

Relative tunability h  = 2 mm

TE110

3.701⋅10−6

5.107⋅10−6

TE210

7.452⋅10−6

1.293⋅10−5

Quarter wave

1.520⋅10−5

1.059⋅10−5