CN102798766A - Method for testing microwave dielectric property of high-loss dielectric substance - Google Patents

Method for testing microwave dielectric property of high-loss dielectric substance Download PDF

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CN102798766A
CN102798766A CN2012102750535A CN201210275053A CN102798766A CN 102798766 A CN102798766 A CN 102798766A CN 2012102750535 A CN2012102750535 A CN 2012102750535A CN 201210275053 A CN201210275053 A CN 201210275053A CN 102798766 A CN102798766 A CN 102798766A
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resonance frequency
dielectric
loss
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CN102798766B (en
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李雷
陈湘明
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Zhejiang University ZJU
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Abstract

The invention discloses a method for testing microwave dielectric property of a high-loss dielectric substance. According to the method, a small-size sample to be tested is used, and a large-size and low-loss reference sample is introduced, so that the high loss of the sample to be tested is reduced, and the resonance peak is ensured to be observed. According to the changes of the resonance peak of a TE01 delta model when only the reference sample is arranged in a resonant cavity and the reference sample and the sample to be tested are simultaneously arranged in the resonant cavity, and the distribution of an electromagnetic field under the two conditions can be simulated by using finite element analysis, so that the dielectric constant and the dielectric loss of the sample to be tested at the resonance frequency can be obtained. According to the method, the characteristics of high test precision of the microwave resonance method is utilized, and the influence on the distribution of the electromagnetic field caused by the introduction of the sample to be tested, is considered, so that the defects of low precision of other conventional methods can be overcome from the test principle, and the accurate test of the microwave dielectric property of the high-loss substance can be realized. Meanwhile, the resonance frequency is decided by the reference sample with large size, so that the frequency conversion test can be realized by changing the dielectric constant or the size of the reference sample.

Description

A kind of method of testing high loss dielectric substance microwave dielectric property
Technical field
The invention belongs to the microwave testing field, the measuring technology of particularly high loss dielectric substance microwave dielectric property.
Background technology
High loss is (greater than 10 -2) dielectric substance such as ferroelectric material, huge dielectric constant material have important potential application foreground at microwave frequency band, but its microwave dielectric property is difficult to accurate test.The method of testing of high consumable material microwave dielectric property mainly comprises reflectometry, reflective-transmissive method and resonant cavity perturbation method.As far as the above two, the scattering parameter under the single frequency point directly is used for the calculating of dielectric properties, and along with the rising of specific inductive capacity, scattering parameter is more and more insensitive to the variation of specific inductive capacity, so measuring accuracy also sharply descends thereupon; Resonant cavity perturbation rule has been utilized the characteristic of microwave resonance, and precision is high slightly, but owing to consider to introduce the variation that electromagnetic field distributes in the cavity that sample causes, so the measuring accuracy can't guarantee equally that specific inductive capacity is higher the time.
Summary of the invention
The purpose of this invention is to provide a kind of method of testing high loss dielectric substance microwave dielectric property, this method has the precision height, is prone to realize the characteristics of frequency conversion test.
The method of the high loss dielectric substance of test of the present invention microwave dielectric property is used high Q value cylindrical metal resonator cavity test, and concrete testing procedure is following:
(1) cylindrical low-loss reference coupon A is positioned on the single crystal quartz support C in the cylindrical metal resonator cavity,, utilizes finite element analysis to calculate TE according to the size and the specific inductive capacity of reference coupon 01 δThe resonant frequency range that pattern is corresponding, and in this frequency range, find harmonic peak with vector network analyzer, write down resonance frequency f 01And resonance frequency f 01Near scattering parameter S 11,1With the variation of frequency, obtain the no-load quality factor q with curve fitting method U1
(2) according to resonance frequency f 01And the size of reference coupon A, utilize finite element analysis and the accurate DIELECTRIC CONSTANTS of iteration Method reference coupon A R, A, the electromagnetic field that obtains according to finite element analysis distributes, by the no-load quality factor q U1Calculate reference coupon A at resonance frequency f 01The dielectric loss tan δ at place A
(3) sample to be tested B is positioned on the reference coupon A, the size of reference coupon A is utilized vector network analyzer record resonance frequency f greater than the size of sample to be tested B 02And resonance frequency f 02Near scattering parameter S 11,2With the variation of frequency, obtain the no-load quality factor q with curve fitting method U2
(4) according to size, the DIELECTRIC CONSTANTS of reference coupon A and sample to be tested B R, AAnd resonance frequency f 02, utilize the DIELECTRIC CONSTANTS of finite element analysis and iteration Method sample to be tested B R, B, the electromagnetic field that obtains according to finite element analysis distributes, by the no-load quality factor q U2Calculate sample to be tested B at resonance frequency f 02The dielectric loss tan δ at place B
(5) size or the specific inductive capacity of change reference coupon A, the frequency conversion test of sample to be tested B microwave dielectric property is realized in repeating step (1)-(4).
Low-loss described in the present invention refers to that the dielectric loss of dielectric substance is less than 10 -3, high loss refers to that the dielectric loss of dielectric substance is greater than 10 -2
Method of testing provided by the invention has been utilized the high characteristic of microwave resonance method test dielectric properties precision; And the introducing of having considered sample to be tested influence that electromagnetic field is distributed; So can overcome existing reflectometry, reflective-transmissive method and the low defective of resonant cavity perturbation method measuring accuracy from test philosophy, thereby realize the high precision measurement of high consumable material microwave dielectric property.Used the low-loss reference coupon big among the present invention, be for the high loss that reduces sample to be tested contribution, thereby guarantee to observe harmonic peak the resonator system total losses than the sample to be tested size.Simultaneously, because resonance frequency is mainly by larger-size reference coupon decision, so can realize the frequency conversion test easily through specific inductive capacity and the size that changes reference coupon.
The present invention can to specific inductive capacity less than 1000, dielectric loss is greater than 10 -2The dielectric properties of high consumable material in the 1-20GHz frequency range carry out exact evaluation.The relative error of specific inductive capacity and dielectric loss is all in 5%.
Description of drawings
Fig. 1 is the cross sectional representation of cylindrical metal resonator cavity, wherein, only places reference coupon among the figure (a), then puts into reference coupon and sample to be tested simultaneously among the figure (b).
Fig. 2 is that scattering parameter is with the synoptic diagram of change of frequency near the resonance frequency, and wherein solid line is for only placing the situation of reference coupon, and dotted line is for put into the situation of reference coupon and sample to be tested simultaneously.
Embodiment
TE 01 δPattern is the of paramount importance a kind of mode of resonance of cylindrical metal resonator cavity, has been widely used in the accurate test of low-loss material microwave dielectric property.Electric field in this pattern has only the component E along hoop θIn cylindrical coordinate, the E of every bit θAll satisfy:
∂ 2 E θ ∂ r 2 + ∂ 2 E θ ∂ z 2 + 1 r ∂ E θ ∂ r + ( β 2 - 1 r 2 ) E θ = 0 , - - - ( 1 )
β wherein 22μ ε=(2 π f 0) 2μ ε, μ and ε are respectively the magnetic permeability and the specific inductive capacity of filling medium, and ω is an angular frequency, f 0Be resonance frequency, r, z represent radially the coordinate with vertical direction respectively.When the specific inductive capacity of all packing materials in the cavity and size are known, utilize numerical methods such as finite element analysis, and introduce the cavity metallic walls E of place θ=0 boundary condition, but solving equation (1).With resonance frequency f 0For the equation (1) of unknown quantity has unlimited a plurality of separating, its minimum value is TE 01 δThe resonance frequency that pattern is corresponding, and the electromagnetic field that can try to achieve in the cavity distributes.Distribute based on the electromagnetic field in the cavity, can obtain the electric energy fill factor, curve factor of every kind of medium
P e , i = ∫ S i ϵ r , i E θ 2 · rdS i Σ i ∫ S i ϵ r , i E θ 2 · rdS i , - - - ( 2 )
ε wherein R, iSpecific inductive capacity for medium.The no-load quality factor q of resonator system uCan be expressed as:
1 Q u = Σ i P e , i tan δ i + 1 Q c , - - - ( 3 )
Tan δ wherein iBe the dielectric loss of medium, Q cBe the quality factor of metallic walls, can try to achieve by the metallic surface conductivity.
The method of the high loss dielectric substance of test of the present invention microwave dielectric property, step is following:
(1) with diameter D A, thickness H ACylindrical low-loss reference coupon A be positioned on the single crystal quartz support C in the cylindrical metal resonator cavity, shown in Fig. 1 (a).According to the size and the specific inductive capacity of reference coupon, utilize finite element analysis to calculate TE 01 δThe resonant frequency range that pattern is corresponding, and in this frequency range, find harmonic peak with vector network analyzer, write down resonance frequency f 01And resonance frequency f 01Near scattering parameter S 11,1With the variation of frequency, shown in the solid line among Fig. 2, obtain the no-load quality factor q with curve fitting method U1
(2) when only placing reference coupon in the cavity, the resonance frequency f of resonator system 01Can be expressed as:
f 01=g 1r,A,D A,H A),(4)
G wherein 1Function for by formula (1) decision utilizes finite element analysis and the accurate DIELECTRIC CONSTANTS of iteration Method reference coupon A R, AAnd corresponding electromagnetic field distributes.The dielectric loss of single crystal quartz support is very low, can ignore, so up-to-date style (3) can be rewritten as:
P e , A 1 tan δ A = 1 Q u 1 - 1 Q c 1 . - - - ( 5 )
The electromagnetic field that obtains according to finite element analysis distributes, by the no-load quality factor q U1Calculate reference coupon A at resonance frequency f 01The dielectric loss tan δ at place A
(3) with diameter D B, thickness H BSample to be tested B be positioned on the reference coupon A, the size of sample to be tested B is less than reference coupon A, shown in Fig. 1 (b).Utilize vector network analyzer record resonance frequency f 02And resonance frequency f 02Near scattering parameter S 11,2With the variation of frequency, shown in the dotted line among Fig. 2, obtain the no-load quality factor q with curve fitting method U2
When (4) placing reference coupon and sample to be tested simultaneously in the cavity, the resonance frequency f of resonator system 02Can be expressed as:
f 02=g 2r,A,D A,H Ar,B,D B,H B),(6)
G wherein 2Be function by formula (1) decision.Simultaneously, f 02Usually only than f 01Low several MHz can think that reference coupon A is at f 01And f 02The specific inductive capacity at place is identical with dielectric loss, so the DIELECTRIC CONSTANTS of finite element analysis capable of using and iteration Method sample to be tested B R, BAnd corresponding electromagnetic field distributes.This up-to-date style (3) can be rewritten as:
P e , A 2 tan δ A + P e , B 2 tan δ B = 1 Q u 2 - 1 Q c 2 , - - - ( 7 )
The electromagnetic field that obtains according to finite element analysis distributes, by the no-load quality factor q U2Calculate sample to be tested B at resonance frequency f 02The dielectric loss tan δ at place B
(5) size or the specific inductive capacity of change reference coupon A, the frequency conversion test of sample to be tested B microwave dielectric property is realized in repeating step (1)-(4).
Embodiment 1
To having the BaTiO of high dielectric loss 3The microwave dielectric property of ferroelectric ceramics is tested.
Sample to be tested B is the BaTiO of diameter 2mm, thickness 0.2mm 3Pottery; Low-loss reference coupon A is the Ca of diameter 12mm, thickness 1-5mm 1.15Nd 0.85Al 0.85Ti 0.15O 4, Ba 2Ti 9O 20And Ba 1.85Sm 4.1Ti 9O 24Pottery.
Test result is as shown in table 1.
Table 1
Know by table 1: with method test b aTiO provided by the invention 3The pottery microwave dielectric property the time, in the frequency range of 1-20GHz, have good repeatability.
Embodiment 2
To having the CaCu of high dielectric loss 3Ti 4O 12The microwave dielectric property of ferroelectric ceramics is tested.
Sample to be tested B is the CaCu of diameter 3mm, thickness 0.5mm 3Ti 4O 12Pottery; Low-loss reference coupon A is the Ca of diameter 12mm, thickness 1-5mm 1.15Nd 0.85Al 0.85Ti 0.15O 4, Ba 2Ti 9O 20And Ba 1.85Sm 4.1Ti 9O 24Pottery.
Test result is as shown in table 2.
Table 2
Know by table 2: with method test CaCu provided by the invention 3Ti 4O 12The pottery microwave dielectric property the time, in the frequency range of 1-20GHz, have good repeatability.

Claims (1)

  1. One kind the test high loss dielectric substance microwave dielectric property method, it is characterized in that may further comprise the steps:
    (1) cylindrical low-loss reference coupon A is positioned on the single crystal quartz support C in the cylindrical metal resonator cavity,, utilizes finite element analysis to calculate TE according to the size and the specific inductive capacity of reference coupon 01 δThe resonant frequency range that pattern is corresponding, and in this frequency range, find harmonic peak with vector network analyzer, write down resonance frequency f 01And resonance frequency f 01Near scattering parameter S 11,1With the variation of frequency, obtain the no-load quality factor q with curve fitting method U1
    (2) according to resonance frequency f 01And the size of reference coupon A, utilize finite element analysis and the accurate DIELECTRIC CONSTANTS of iteration Method reference coupon A R, A, the electromagnetic field that obtains according to finite element analysis distributes, by the no-load quality factor q U1Calculate reference coupon A at resonance frequency f 01The dielectric loss tan δ at place A
    (3) sample to be tested B is positioned on the reference coupon A, the size of reference coupon A is utilized vector network analyzer record resonance frequency f greater than the size of sample to be tested B 02And resonance frequency f 02Near scattering parameter S 112With the variation of frequency, obtain the no-load quality factor q with curve fitting method U2
    (4) according to size, the DIELECTRIC CONSTANTS of reference coupon A and sample to be tested B R, AAnd resonance frequency f 02, utilize the DIELECTRIC CONSTANTS of finite element analysis and iteration Method sample to be tested B R, B, the electromagnetic field that obtains according to finite element analysis distributes, by the no-load quality factor q U2Calculate sample to be tested B at resonance frequency f 02The dielectric loss tan δ at place B
    (5) size or the specific inductive capacity of change reference coupon A, the frequency conversion test of sample to be tested B microwave dielectric property is realized in repeating step (1)-(4).
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Cited By (14)

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CN103941101A (en) * 2014-04-09 2014-07-23 芜湖航飞科技股份有限公司 High-frequency medium relative dielectric constant measuring circuit and method and discreteness measuring method
CN103983858A (en) * 2014-05-15 2014-08-13 中国电子科技集团公司第四十一研究所 High-precision broadband measurement method for dielectric property of low-loss material
CN104181341A (en) * 2014-08-29 2014-12-03 中国科学技术大学 Multi-functional sample rod for electromagnetism testing and photoelectricity testing
CN108011171A (en) * 2017-11-30 2018-05-08 电子科技大学 A kind of broadband dielectric resonator
CN109521079A (en) * 2018-11-20 2019-03-26 中电科仪器仪表有限公司 A kind of multifrequency point material testing system and method
CN110441614A (en) * 2019-09-03 2019-11-12 浙江大学 The recognition methods of TE011 mode of resonance in the test of low-loss material micro-wave dielectric
CN110441613A (en) * 2019-08-14 2019-11-12 中电科仪器仪表有限公司 Coaxial resonant cavity test method and system based on scalar network analyzer
CN111157802A (en) * 2020-01-03 2020-05-15 西安交通大学 Method for measuring microwave dielectric property of high-loss material by adopting electric field symmetric structure
CN111239498A (en) * 2020-03-18 2020-06-05 山东国瓷功能材料股份有限公司 Device and method for testing dielectric property of material
CN111487470A (en) * 2020-03-18 2020-08-04 山东国瓷功能材料股份有限公司 Device and method for testing dielectric property of material
WO2021031347A1 (en) * 2019-08-16 2021-02-25 广东浪潮大数据研究有限公司 Method and apparatus for testing dielectric constant
CN113156215A (en) * 2021-02-23 2021-07-23 浙江大学 Identifying TE without estimating the dielectric constant of the material011Method of resonant mode
CN113189155A (en) * 2021-05-11 2021-07-30 南京邮电大学 Improved method for measuring dielectric constant based on resonant cavity perturbation method
CN115862726A (en) * 2023-02-27 2023-03-28 西南交通大学 Wave-absorbing material design method based on dielectric constant genome

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CN1453574A (en) * 2003-05-30 2003-11-05 华中科技大学 Complex microwave dielectric constant measuring method for ceramic with high dielectric constant and low loss
US7285963B2 (en) * 2004-04-09 2007-10-23 Solid State Measurements, Inc. Method and system for measurement of dielectric constant of thin films using a near field microwave probe
CN101187683A (en) * 2007-10-30 2008-05-28 电子科技大学 Low consumption dielectric material high temperature complex dielectric constant test device and method

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DE2542813B1 (en) * 1975-09-25 1977-01-27 Siemens Ag Dielectric constant measurement for ceramic substrates - has built in filter and metallised foil each side of specimen
CN1453574A (en) * 2003-05-30 2003-11-05 华中科技大学 Complex microwave dielectric constant measuring method for ceramic with high dielectric constant and low loss
US7285963B2 (en) * 2004-04-09 2007-10-23 Solid State Measurements, Inc. Method and system for measurement of dielectric constant of thin films using a near field microwave probe
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Cited By (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103941101A (en) * 2014-04-09 2014-07-23 芜湖航飞科技股份有限公司 High-frequency medium relative dielectric constant measuring circuit and method and discreteness measuring method
CN103983858A (en) * 2014-05-15 2014-08-13 中国电子科技集团公司第四十一研究所 High-precision broadband measurement method for dielectric property of low-loss material
CN103983858B (en) * 2014-05-15 2017-01-25 中国电子科技集团公司第四十一研究所 High-precision broadband measurement method for dielectric property of low-loss material
CN104181341A (en) * 2014-08-29 2014-12-03 中国科学技术大学 Multi-functional sample rod for electromagnetism testing and photoelectricity testing
CN108011171A (en) * 2017-11-30 2018-05-08 电子科技大学 A kind of broadband dielectric resonator
CN109521079B (en) * 2018-11-20 2021-06-08 中电科思仪科技股份有限公司 Multi-frequency-point material testing system and method
CN109521079A (en) * 2018-11-20 2019-03-26 中电科仪器仪表有限公司 A kind of multifrequency point material testing system and method
CN110441613B (en) * 2019-08-14 2022-04-19 中电科思仪科技股份有限公司 Coaxial resonant cavity testing method and system based on scalar network analyzer
CN110441613A (en) * 2019-08-14 2019-11-12 中电科仪器仪表有限公司 Coaxial resonant cavity test method and system based on scalar network analyzer
WO2021031347A1 (en) * 2019-08-16 2021-02-25 广东浪潮大数据研究有限公司 Method and apparatus for testing dielectric constant
CN110441614A (en) * 2019-09-03 2019-11-12 浙江大学 The recognition methods of TE011 mode of resonance in the test of low-loss material micro-wave dielectric
CN111157802A (en) * 2020-01-03 2020-05-15 西安交通大学 Method for measuring microwave dielectric property of high-loss material by adopting electric field symmetric structure
CN111239498A (en) * 2020-03-18 2020-06-05 山东国瓷功能材料股份有限公司 Device and method for testing dielectric property of material
CN111487470A (en) * 2020-03-18 2020-08-04 山东国瓷功能材料股份有限公司 Device and method for testing dielectric property of material
CN111239498B (en) * 2020-03-18 2022-05-31 山东国瓷功能材料股份有限公司 Device and method for testing dielectric property of material
CN113156215A (en) * 2021-02-23 2021-07-23 浙江大学 Identifying TE without estimating the dielectric constant of the material011Method of resonant mode
CN113156215B (en) * 2021-02-23 2022-05-27 浙江大学 Identifying TE without estimating the dielectric constant of the material011Method of resonant mode
CN113189155A (en) * 2021-05-11 2021-07-30 南京邮电大学 Improved method for measuring dielectric constant based on resonant cavity perturbation method
CN115862726A (en) * 2023-02-27 2023-03-28 西南交通大学 Wave-absorbing material design method based on dielectric constant genome
CN115862726B (en) * 2023-02-27 2023-05-02 西南交通大学 Wave-absorbing material design method based on dielectric constant genome

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