This application is a 371 U.S. National Phase of International Application No. PCT/JP2020/017375, filed on Apr. 22, 2020. The entire disclosure of the above application is incorporated herein by reference.
The present disclosure relates to an object permittivity measurement apparatus and an object permittivity measurement method for measuring permittivity of an object. Furthermore, the present disclosure relates to an object thickness measurement apparatus and an object thickness measurement method for measuring a thickness of the object.
A method for irradiating an object to be measured with electromagnetic waves having a plurality of frequencies to calculate relative permittivity of the object to be measured has been developed (for example, see PTL 1).
According to this method, the object to be measured is irradiated with the electromagnetic wave, and the relative permittivity of the object to be measured is calculated from a phase change after transmission through the object to be measured and the known thickness of the object to be measured.
In the method of PTL 1, the object to be measured is irradiated with the electromagnetic waves having the plurality of frequencies, and a phase of the electromagnetic waves after the transmission is measured. For this reason, the method described in PTL 1 cannot be applied to an outdoor communication facility opaque to the electromagnetic wave.
A reflection-type measurement using a terahertz wave that is of the electromagnetic wave at frequency 1011 to 1013 has been devised in order to enable the measurement of a foreign material on the surface of the object opaque to such electromagnetic waves. The reflective type can also be applied to the object opaque to the electromagnetic wave.
A measurement target of the present disclosure will be described, by way of example, an opaque object, namely, a metal body as the object that reflects the electromagnetic wave, and the foreign material existing on the surface of the opaque object, namely, a metal corrosion portion as the foreign material that reflects a light wave and through which the electromagnetic wave is transmitted. At this point, the terahertz wave at frequency 1011 to 1013 is illustrated as an example of the electromagnetic wave.
For the corroded metal body, the light wave is reflected on the surface of the corrosion portion. On the other hand, the terahertz wave is transmitted through the corrosion portion and reflected on the surface of the non-corrosion metal body. Generally, in corrosion in a zinc-plated steel material, zinc on the surface is oxidized and corroded in an initial stage. When the corrosion progresses to disappear plating of zinc, inside iron begins to corrode. A composition of the material changes corresponding to the stage of the corrosion, so that the stage of the corrosion can be estimated by measuring a characteristic of the material on the surface of the metal body.
Thus, for the corroded metal body, the light wave is used to measure a distance to the surface of the corrosion portion and the electromagnetic wave is used to measure a rotation amount of the phase to the surface of the corroded metal body. In measuring the rotation amount of the phase to the surface of the metal body, the rotation amount of the phase increases by the distance from the surface of the corrosion portion to the surface of the metal body as compared to the rotation amount of the phase to the surface of the corrosion portion.
For this reason, the rotation amount of the increased phase may be calculated. When the thickness of the corrosion portion is known, the permittivity of the corrosion portion can be calculated from the rotation amount of the increased phase. When the permittivity of the corrosion portion is known, the thickness of the corrosion portion can be calculated.
Specifically, an object permittivity measurement apparatus according to one aspect of the present invention includes:
Specifically, an object permittivity measurement method according to another aspect of the present invention includes:
Specifically, an object thickness measurement apparatus according to still another aspect of the present invention includes:
Specifically, an object thickness measurement method according to yet another aspect of the present invention includes:
According to the object permittivity measurement apparatus and the object permittivity measurement method of the present disclosure, the permittivity of the foreign material on the object surface can be calculated when the thickness of the foreign material on the object surface is known.
According to the object thickness measurement apparatus and the object thickness measurement method of the present disclosure, the thickness of the foreign material on the object surface can be calculated when the permittivity of the foreign material on the object surface is known.
Hereinafter, embodiments of the present disclosure will be described in detail with reference to the drawings. Note that the present disclosure is not limited to the embodiments described below. These embodiments are just illustrative examples, and the present disclosure can be implemented in forms in which various modifications and improvements are added on the basis of knowledge of those skilled in the art. Note that constituent elements with the same reference signs in the specification and the drawings are assumed to be the same constituent elements.
Light wave distance measurement will be described with reference to
From the reciprocating time t and a light speed c, the distance calculation circuit 124 calculates the distance L from the object permittivity measurement apparatus 10 to the surface of the metal corrosion portion 51 based on the following equation (1) (T3).
L=ct/2 (1)
Electromagnetic wave phase measurement will be described with reference to
The permittivity calculation will be described with reference to
φ=4πLf/c+4π(ε)1/2df/c (2)
A first term of the equation (2) represents an amount of the phase that rotates while the electromagnetic wave having the frequency f reciprocates between the object permittivity measurement apparatus 10 and the surface of the metal corrosion portion 51. A second term of the equation (2) represents the amount of phase that rotates while the electromagnetic wave having the frequency f reciprocates between the surface of the metal corrosion portion 51 and the surface of the metal body 52.
The permittivity of the corrosion portion that is of the foreign material on the object surface can be calculated when the thickness of the corrosion portion that is of the foreign material on the object surface is known. In particular, when the frequency f of the electromagnetic wave is 1011 to 1013, the permittivity of the corrosion portion can be accurately calculated because a large portion of the electromagnetic wave is transmitted through the corrosion portion and reflected by the metal body.
The light wave distance measurements are described with reference to
From the reciprocating time t and the light speed c, the distance calculation circuit 124 calculates the distance L from the object permittivity measurement apparatus 10 to the surface of the metal corrosion portion 51 based on the following equation (1) (T3).
L=ct/2 (1)
The electromagnetic wave phase measurements are described with reference to
The thickness calculation will be described with reference to
φ=4πLf/c+4π(ε)1/2df/c (2)
The first term of the equation (2) represents the amount of phase that is rotated while the electromagnetic wave having the frequency f reciprocates between the object thickness measurement apparatus 20 and the surface of the metal corrosion portion 51. The second term of the equation (2) represents the amount of phase that rotates while the electromagnetic wave having the frequency f reciprocates between the surface of the metal corrosion portion 51 and the surface of the metal body 52.
The thickness of the corrosion portion that is of the foreign material on the object surface when the permittivity of the corrosion portion that is of the foreign material on the object surface is known. In particular, when the frequency f of the electromagnetic wave is 1011 to 1013, the thickness of the corrosion portion can be accurately calculated because the large portion of the electromagnetic wave is transmitted through the corrosion portion and reflected by the metal body.
The present disclosure can be applied in the information communication industry.
Filing Document | Filing Date | Country | Kind |
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PCT/JP2020/017375 | 4/22/2020 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2021/214917 | 10/28/2021 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
6005397 | Zoughi et al. | Dec 1999 | A |
20100064820 | David | Mar 2010 | A1 |
Number | Date | Country |
---|---|---|
1804567 | Jul 2006 | CN |
109556503 | Apr 2019 | CN |
H0763705 | Mar 1995 | JP |
200019132 | Jan 2000 | JP |
2007271412 | Oct 2007 | JP |
2017207422 | Nov 2017 | JP |
2018119929 | Aug 2018 | JP |
2018179663 | Nov 2018 | JP |
2019007743 | Jan 2019 | JP |
WO-0231537 | Apr 2002 | WO |
WO-2019172183 | Sep 2019 | WO |
Number | Date | Country | |
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20230236005 A1 | Jul 2023 | US |