Section 7.8 · Further exercises · 4 of 10
Exercise 7.8.4: Measuring a liquid with a pillbox
About the further exercises of Section 7.8
Ten further exercises in the spirit of Problems 7.8.1–7.8.5 and the home exercises, graded from easy to harder. Exercises 7.8.1–7.8.6 are about cavity resonators, Exercises 7.8.7–7.8.10 about microwave devices and scattering parameters. They use only the results of this section, in particular , of Eq. (7.8.24) with ( for a cube), of Eq. (7.8.33), , , , the response with , and for S-parameters , reciprocity , losslessness , and .
Measuring a liquid with a pillbox
#The copper TM cavity of Problem 7.8.3 (, , , when empty) is filled completely with a nonmagnetic silicone oil. Weakly coupled, the resonance moves to and its becomes . (a) Find of the oil. (b) Find of the walls with the oil inside. (c) Find , and . (d) How much does a error in change ? What would neglecting the walls give?
Filling a cavity completely scales all its frequencies by , so is the square of the frequency ratio. The two losses add as , and . is not measured: it follows from the empty cavity, since with and , so .
.
. Directly: , at and .
so and . The oil takes of the loss.
With , . With , . The error is or less. Neglecting the walls entirely, , too high.
Forward: , . The radius and length do not change, and TM remains the lowest mode because all modes scale together.
Cavity measurements of are accurate because both readings are frequencies: to many digits, and from a bandwidth (here ). The method works best when , so that the uncertainty of the wall loss hardly matters. For very low-loss materials a small sample is used instead of a full filling, and a perturbation formula relates the shifts to .
cf. Problem 7.8.3