Plant water sensor
US-2019187072-A1 · Jun 20, 2019 · US
US11435385B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11435385-B2 |
| Application number | US-202016850054-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 16, 2020 |
| Priority date | Apr 23, 2019 |
| Publication date | Sep 6, 2022 |
| Grant date | Sep 6, 2022 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A specific conductivity measurement method includes: performing first measurement to obtain a resonance frequency f1 that is outputted to a measuring device when the first and second dielectric flat plates each have a thickness t1, and an unloaded Qu1 that corresponds to the resonance frequency f1; performing second measurement to obtain a resonance frequency f2 that is outputted to the measuring device when the first and second dielectric flat plates each have a thickness t2 that is different from the thickness t1, and an unloaded Qu2 that corresponds to the resonance frequency f2; and calculating a specific conductivity σr of the copper foil and the first and second conductor flat plates based on an arithmetic equation that includes the resonance frequency the unloaded Qu1, the resonance frequency f2, and the unloaded Qu2.
Opening claim text (preview).
What is claimed is: 1. A specific conductivity measurement method comprising: obtaining, by a computer, a resonance frequency f 1 that is acquired by a measuring device coupled to a resonator, which includes a circular copper foil, first and second dielectric flat plates that are disposed on both surface sides of the copper foil to sandwich the copper foil, first and second conductor flat plates that each have a hole at a center part and that sandwich the first and second dielectric flat plates from both sides with the centers of the first and second conductor flat plates aligned with the centers of the first and second dielectric flat plates, and excitation wires that are disposed in the respective holes of the first and second conductor flat plates, based on the first and second dielectric flat plates that each has a thickness t 1 , and an unloaded Q u1 that corresponds to the resonance frequency f 1 ; obtaining a resonance frequency f 2 that is acquired by the measuring device based on the first and second dielectric flat plates that each has a thickness t 2 that is different from the thickness t 1 , and an unloaded Q u2 that corresponds to the resonance frequency f 2 ; and calculating a specific conductivity σ r of the copper foil and the first and second conductor flat plates based on an arithmetic equation that includes the resonance frequency f 1 , the unloaded Q u1 , the resonance frequency f 2 , and the unloaded Q u2 . 2. The specific conductivity measurement method according to claim 1 , wherein the calculating includes calculating the specific conductivity σ r based on Equation (1): σ r ( f 0 ) = 1 πμ 0 σ 0 1 f 0 [ t f 2 - t f 1 Q u 1 Q u 2 t f 1 t f 2 Q u 2 - Q u 1
of plate type, i.e. with the sample sandwiched in the middle · CPC title
Measuring-systems or electronic circuits (G01R27/2635, G01R27/2682 take precedence) · CPC title
Cavities, resonators, free space arrangements, reflexion or interference arrangements (G01R27/2647 takes precedence; optical methods G01R27/2682) · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.