TWI255585B - Light and super broadband microwave absorbent material - Google Patents

Light and super broadband microwave absorbent material Download PDF

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Publication number
TWI255585B
TWI255585B TW94131941A TW94131941A TWI255585B TW I255585 B TWI255585 B TW I255585B TW 94131941 A TW94131941 A TW 94131941A TW 94131941 A TW94131941 A TW 94131941A TW I255585 B TWI255585 B TW I255585B
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layer
resistivity
materials
incident
electromagnetic wave
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TW94131941A
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TW200713698A (en
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Jian-Sheng Sheen
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Chung Shan Inst Of Science
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Abstract

Disclosed is a light and super broadband microwave absorbent material, which comprises the homogeneous electric material and the metal material with two different ratios of resistivity, or the electromagnetic wave high reflection material. The resistivity of the electric homogeneous consuming material of the first layer is 1500 to 3000 Omega/□ and the thickness ranges from 2.5 to 3.5 mm, while the resistivity of the electric homogeneous consuming material of the second layer is 100 to 400 Omega/□ and the thickness is 3.5 to 4.5 mm. The third layer is made of metal material or electromagnetic wave high reflection material. The three kinds of materials are in turn jointed tightly with one anther. The light and super broadband microwave absorbent material features with the vertical reflectance less than -10 dB of the broadband over 5.2 to 18 GHz and the total thickness within 7 mm while the weight of every square meter less than 1.5 kilograms.

Description

1255585 五、發明說明(1) 【發明所屬之技術領域】 全世界無線通訊產業在近數 衛星轉播站及大哥大站台林立 口附近的居民或衛星轉播站機 受電磁波輻射照射,直接、間 制大哥大站台或衛星轉播站輻 微波吸收材以降低微波輻射, 全為大家所共識。 資訊、通訊科技日新月異 •功能化方向發展,此類產品之 重,應用輕、薄及高吸收效益 代電子、資訊、通訊等電器產 (EMC)問題顯得極為迫切。 年來已蓬勃發展,雷達站、 ;居住在雷達站、大 房内的工作人員,因;=站 接影響身體健康;兔二J接 射威脅,應在適當位置$ = 防護居民及工作人員人身= 相關產品多朝小型化與多 電磁干擾(EMI)問題益形^ 之電磁波吸收材以解決新一 品之電磁干擾及電磁相容 以上不論是雷達站、衛星轉播站或大哥大站a 射防護問題’或解決電子、資訊、通訊等電哭產'之、幸田 E:!。、EMC問題均可利用電磁波吸收材將威脅降至最低的程 ^iHdi^DeteCtiQn And ⑽心,簡獅DAR)意為 =線電採測與測距;自從194〇年代發明 = 替代目視的工具;其優點乃^波=氣 2過私中被大氣衰減程度較可見光、近紅外光及紅外光 率偵測距離較遠,1近代科學技術已可將雷達發射功 革及偵測靈敏度有效提高,直接提昇雷達可偵搜距離;故1255585 V. INSTRUCTIONS (1) [Technical field to which the invention belongs] The wireless communication industry in the world is in the vicinity of several satellite relay stations and the residents or satellite relay stations near the Tailin station of the Big Brother station are exposed to electromagnetic radiation. Radiation microwave absorbers at large stations or satellite relay stations to reduce microwave radiation are all agreed by everyone. Information and communication technologies are changing with each passing day. • The development of functionalization, the weight of such products, the application of light, thin and high absorption benefits. The generation of electronic products, information, communication and other electrical products (EMC) problems are extremely urgent. Years have flourished, radar stations, staff living in radar stations, large rooms, because; = station connection affects health; rabbit II J radiation threat, should be in place $ = protection of residents and staff personal = Related products are mostly toward miniaturization and multi-electromagnetic interference (EMI) problems. The electromagnetic wave absorbers are used to solve the electromagnetic interference and electromagnetic compatibility of the new product. Whether it is a radar station, a satellite relay station or a large station Or solve the electronic, information, communication and other power crying ', Koda E:! EMC problems can use electromagnetic wave absorbing materials to minimize the threat ^iHdi^DeteCtiQn And (10) heart, Jane DAR) means = line electric measurement and ranging; since the invention of the 194s = alternative visual tools; The advantage is that the wave is too far away from the visible light, near-infrared light and infrared light. The modern science and technology can effectively improve the radar emission and the detection sensitivity. Raising the radar can detect the distance; therefore

第5頁 1255585 五、發明說明(2) 在軍事應用上 前軍事上最重 武器載具之雷 RCS)是表示武 载具之雷達截 對較弱,因其 知,容易接近 可充分發揮隱 對新型武器之 .之作戰性能, 標。降低武器 載具的雷達波 武器載具之雷 達波反射亮點 量減降回波訊 法0 搜、制導工具,為目 雷達已廣泛被作為偵 要的裝備之一。 ,截面積(Radar Cross Sectl〇n,簡寫為 為載具被雷達照射後散射之回波強度大小, 面積愈小其對雷達波之反射回波訊號強度相 回波訊號弱,載具須較靠近雷達方可被偵 =方,T被發現,因此低雷達截面積載具當 始、及奇襲之功效。現今世界各武器先進國家 研舍無不要求降低其雷達截面積以提昇武器 低RCS將為現今及未來武器設計之重要指 ,具雷達截面積的方法除以造型方式將射抵 散射至異於入射的方向,使雷達無法接收到 達回波訊號以降低載具之RCS外,在載具雷 部位施以雷達波吸波材,吸收入射雷達波能 號強度,以降低載具RCS值為另一可行之方 【先前技術】 ’電磁波吸收材,依材料从所此& 攸柯料材質特性可區分為電性吸收材、 磁性吸收材與綜合型夂麵 机 ^ ~ ^ 口 i芩頬,一般以誘電係數 (permittivity, ε = 〇 ι , · 〇 · 厂 所壯从 ,^ ^ ε1 + ] ,广/-1)描述電性吸收材材 貝4寸性’ £ 1為誘雷你叙每 u ·电係數只部,£ 2為誘電係數虛部。以導磁 係數(permeabi 1 i tv," ,,. y ^ = // 1 +j // 2) 描述磁性吸收材材質特 第6頁 1255585Page 5 1255585 V. Description of the invention (2) In military applications, the former military's heaviest weapon carrier, the RCS), indicates that the radar interception of the military vehicle is weak, and because of its knowledge, it is easy to approach and can fully play its role. The combat performance of a new type of weapon. Reducing the radar wave of the weapon Vehicle The radar wave reflection point of the weapon carrier The amount of the radar wave detection method is one of the equipments that have been widely used as a radar. , the cross-sectional area (Radar Cross Sectl〇n, abbreviated as the echo intensity of the scattering after the radar is irradiated by the radar, the smaller the area, the reflected echo signal strength of the radar wave is weaker, the vehicle must be closer The radar can be detected by the party, T is discovered, so the low radar cross-sectional area vehicle has the effect of the beginning and the surprise attack. Nowadays, all the advanced weapons research institutes in the world are required to reduce the radar cross-sectional area to enhance the weapon low RCS will be nowadays. And the important means of future weapon design, the method of radar cross-sectional area divided by the modeling method will scatter the radiation to a direction different from the incident, so that the radar can not receive the echo signal to reduce the RCS of the vehicle, and the lightning part of the vehicle Applying a radar wave absorbing material to absorb the intensity of the incident radar wave energy to reduce the RCS value of the vehicle is another feasible method. [Prior Art] 'Electromagnetic wave absorbing material, according to the material characteristics of the material It is divided into electric absorbing materials, magnetic absorbing materials and integrated kneading machines ^ ^ ^ mouth i 芩頬, generally with the electric conductivity (permittivity, ε = 〇ι, · 〇 · factory strong, ^ ^ ε1 + ], /-1) Describe the electric absorption material shell 4 inch ' £ 1 for the lure you say each u · electric coefficient only part, £ 2 is the imaginary part of the electric induction coefficient. With magnetic permeability (permeabi 1 i tv, " ,,. y ^ = // 1 +j // 2) Description Magnetic Absorber Material Page 6255585

性 電 射 ’ V 1為導磁係數實部 或導磁係數其虛部稱為 電磁波之電能或磁能。 “ 2為導磁係數虛部 耗損項(loss term) 吸波材之誘 能吸收入 電磁波吸收材依吸收頻寬範圍大小可區分# ,,窄頻吸波材其吸波頻域較 定頁窄、見 :電磁能吸:;固定發射頻率之雷達站、衛星轉m :大站台多抓用它以作為電磁輻射防護、《雷達天 消除等之所需。寬頻吸波材其可吸收電磁波較j瓣 它可應用作為武器載具雷達波回波減降材及電磁波=、由 丨暗室吸波材等。 反…、回波 中華民國專利第42 1 9 88號,井上正之等發明人,以、曾 電材所形成角錐形,利用角錐外型控制入射波之反射 達吸波效果。中華民國專利第42880 1號專利,村瀨琢$ 明人以不燃性與可撓性導電材所形成角錐形吸波材,美二 專利US#5381 1 49,發明人Th〇mas κ.等人以5層採漸進式: 電質所以形成吸波材,以上諸專利均採用電性材質以^ ^ 吸波材。電性吸波材其製作方法通常以碳粉或其他金屬粉 摻合適當填充劑、膠合劑形成一定密度及厚度之塊材或^ 片,此種電性吸波材之吸波特性除與使用原料之材質(/、, _其導磁係數//= 1 )相關外與材料厚度亦關係密切,除特殊造 塑:如以角錐型吸收材外’欲以薄片材達成寬頻吸收之效 果須透過材質檢測、吸波材設計、製作及吸波性質驗證等 技術,開發難度甚高。The electric radiation ' V 1 is the real part of the magnetic permeability or the magnetic part of the magnetic permeability is called the electric energy or magnetic energy of the electromagnetic wave. "2 is the loss term of the imaginary part of the magnetic permeability coefficient. The absorption energy of the absorbing material into the electromagnetic wave absorbing material can be distinguished according to the size of the absorption frequency range. The narrow frequency absorbing material has a narrower frequency domain than the fixed wave. See: electromagnetic energy absorption:; fixed transmission frequency radar station, satellite to m: large station to use it as electromagnetic radiation protection, "radar day elimination, etc.. Broadband absorbers can absorb electromagnetic waves. The valve can be applied as a weapon carrier radar wave echo reduction material and electromagnetic wave =, from the dark room absorbing material, etc.. ..., echoes the Republic of China patent No. 42 1 9 88, Inoue Masahiro and other inventors, The pyramidal shape formed by the former electric material uses the shape of the pyramid to control the reflection of the incident wave to achieve the absorbing effect. The patent of the Republic of China Patent No. 42880 No. 1 is a pyramidal suction formed by the non-combustible and flexible conductive materials. Wave material, US 2 patent US #5381 1 49, the inventor Th〇mas κ. et al. adopts 5 layers of progressive type: electricity to form absorbing materials, all of the above patents use electrical materials to ^ ^ absorbing materials Electrical absorbing materials are usually made of toner or other gold. The powder is suitably mixed with a filler or a binder to form a block or a piece of a certain density and thickness. The absorbing property of the electric absorbing material is different from the material of the raw material (/, _ its magnetic permeability// = 1) The relevant external and material thickness are also closely related, except for special plasticization: if the pyramidal absorption material is used, the effect of wide-band absorption by thin sheet material must be verified by material detection, absorbing material design, fabrication and absorbing properties. Such technology is very difficult to develop.

五、發明說明(4) 美國專 Zn) ^ Mn-Zn 作方法通常 粉接合適當 此種材料之 材料厚度亦 吸波材難度 吸收效果較 候性差、易 【發明内 本發明 寬頻域之 論模擬設 本發明 層,電磁 波穿透第 層,係以 吸波 >電磁波傳 質材料而 利US#323160 Kyung Y等發明人,利用 專F e r r i t e製作磁性吸波材。磁性吸波材其製 以鐵、鈷等金屬微粉或鐵氧磁體(ferri te)微 填充劑、膠合劑形成一定厚度之塊材或薄片, 吸波特性除與使用之原料材質(//)相關外,與 關係密切。現有技術中欲以此種方式製作寬頻 甚高,且磁性吸波材其高頻導磁係數值甚小, 差,又單位體積重量重,·且作為戶外使用其耐 於老化鏽儀等為其主要缺點。 容】 寬頻微波吸波材顧名思義,此種吸波材能對一定 入射電磁波達成吸收效果,本發明專利乃透過理 計’依特定厚度與適當阻抗匹配所完成。 之吸波材受電磁波首先射抵之層稱為第一入射 波穿透第一入射層所射抵之層稱為第二層,電磁 二入射層所射抵之層稱為第三層,第三層為反射 高導電率之金屬等為本層之材料。 材料首先接觸入射波之面稱為入射面,入射面對 f會產生一阻抗,稱為輸入阻抗(7/ ),對一般均 言,輸入阻抗可定義為:V. INSTRUCTIONS (4) Zn-Zn in the United States Mn-Zn is usually used to join the powder. The thickness of the material is also poor. The absorption of the absorbing material is less than that of the absorbing material. In the layer of the present invention, the electromagnetic wave penetrates the first layer, and the inventor of the US #323160 Kyung Y, which uses the absorbing wave > electromagnetic wave mass transfer material, uses a special Ferrer to make a magnetic absorbing material. The magnetic absorbing material is made of a metal micropowder such as iron or cobalt or a ferrite micro-filler or a binder to form a block or a sheet of a certain thickness, and the absorbing property is different from the raw material used (//). Related, and closely related. In the prior art, it is desired to produce a wide frequency band in such a manner, and the magnetic wave absorbing material has a small high frequency magnetic permeability coefficient value, a small difference in weight per unit volume, and is used as an outdoor aging resistance meter. The main drawback. As a name suggests, broadband microwave absorbing materials can absorb absorption of certain incident electromagnetic waves. The invention patent is achieved by matching the appropriate thickness with appropriate impedance. The layer of the absorbing material that is firstly irradiated by the electromagnetic wave is called the layer in which the first incident wave penetrates the first incident layer, and the layer that the electromagnetic two incident layer hits is called the third layer. The three layers are materials that reflect high conductivity and the like. The surface where the material first contacts the incident wave is called the incident surface, and the incident surface f produces an impedance called the input impedance (7/). In general, the input impedance can be defined as:

V ( βτ/ ε r ) t an h ( - i k 0 d • · · · · · (1) ^55585V ( βτ / ε r ) t an h ( - i k 0 d • · · · · · · (1) ^55585

i相對導材料之相對介電常數,π為均質材料 場波波向量=2吸波材純屬介電材,…1),k〇為電 ,d為均質吸收材二/λ 〇,λ 0為電磁波在自由空間之波長 sPaCe)之阻於士 ”、子度。電磁波在自由空間(free 空間之阻抗大4 i為20,Ζ〇 = 377 Ω / □。為方便處理將自由 示如下式: 知一化(Ζ0 = 1),材料對入射波之反射大小i relative conductor material relative dielectric constant, π is homogeneous material field wave wave vector = 2 absorbing material is pure dielectric material, ... 1), k 〇 is electricity, d is homogeneous absorption material 2 / λ 〇, λ 0 The electromagnetic wave is in the free space sPaCe). The electromagnetic wave is in free space (the impedance of the free space is 4 i is 20, Ζ〇 = 377 Ω / □. For convenience, the freedom is shown as follows: Knowing the difference (Ζ0 = 1), the reflection of the material on the incident wave

r"〇- V)/(Ur"〇- V)/(U

V (2) 反射率R定義如 下: R=r.r*=【(1- α)/(1+以分貝值dB為單位之反射率為 R(dB) = 20· iog( |r丨)..... (3) (4) 由以上理論分析得知,吸波材料之吸收效率直接受材料之 輸入阻抗所衫響,介電吸波材之輸入阻抗與材料之材質 ε r關係可由式(1)中得出’介電吸波材之材質與材料之電 阻率(P )具有一定之關係,材料之面電阻值(R □,Ω / □)與V (2) The reflectance R is defined as follows: R = rr * = [(1 - α) / (1 + the reflectivity in decibels dB is R (dB) = 20 · iog ( | r丨).. (3) (4) According to the above theoretical analysis, the absorption efficiency of the absorbing material is directly affected by the input impedance of the material, and the relationship between the input impedance of the dielectric absorbing material and the material ε r of the material can be 1) It is concluded that the material of the dielectric absorbing material has a certain relationship with the resistivity (P) of the material, and the surface resistance value (R □, Ω / □) of the material

12555851255585

• . · (5) 五、發明說明(6) 電卩且率間關係如下• (5) V. Description of invention (6) Electricity and the relationship between rates is as follows

R p L/A 式(5)中(L)為介電吸波材之長度,(A)為其 電磁波在材料兩界面間(波進、 貝 若匹配(match ing)良好,反射率較 二二二)輪入阻抗 入材料内層被吸波材料所吸收, &才有可爿b進 吸收特性多好,將因兩界面間輪入、卿内層的吸波材料 丨波剛剛射抵材料界面處即被反射 抗I匹配,以致電磁 被材料吸收,故高效率之吸波材庫;^ ^入材料内層 好匹配。 +頁應重視輸入阻抗之良 本發明係利用不同材質特性之三種材料 二(= 及材質特徵“)設計製作完成吸波材二:二 八反射率(R)小於-l〇dB之頻率範圍從5 2GHzi18gHz以 ^,—l〇dB之吸波頻寬大於12GHz以上,示如第2圖, :::之寬頻吸波材僅為4GHz之頻寬。本吸 =二於7mm,每平方公尺總重量小於i 5公斤重量輕,並適 〔戶、内外長期使用,耐候性能佳,充分達 溥(厚度)、寬(吸波頻寬)、大(吸收率)之特# (重里) 【實施方式】R p L/A In formula (5), (L) is the length of the dielectric absorber, and (A) is the electromagnetic wave between the two interfaces of the material (wave in, match ing is good, reflectivity is better) 22) The in-line impedance into the inner layer of the material is absorbed by the absorbing material, and the absorption characteristics of the absorbing material are better, and the absorbing material of the absorbing material in the inner layer of the inner layer is just injected against the material interface. The position is reflected by the anti-I, so that the electromagnetic is absorbed by the material, so the high efficiency of the absorbing material library; ^ ^ into the inner layer of the material is well matched. +Page should pay attention to the input impedance. The invention uses three materials of different material properties (= and material characteristics) to design and manufacture the absorbing material. The second eight-eighth reflectance (R) is less than -l〇dB. 5 2GHzi18gHz with ^, -l〇dB absorption bandwidth is greater than 12GHz, as shown in Figure 2, ::: broadband absorbing material is only 4GHz bandwidth. This suction = two at 7mm, per square meter The total weight is less than i 5 kg light weight, and suitable for long-term use, household, internal and external, weather resistance, sufficient to reach the thickness (thickness), width (absorption bandwidth), large (absorption rate) special # (重里) the way】

PU 兩種不同均質電阻率之材料其製作 、HABS、橡膠等基材::方句ί煉 可 或 以在ΡΕ、 均勻浸泡形PU Two kinds of materials with different uniform resistivity, such as HABS, rubber, etc.:: Square smelting can be used in ΡΕ, uniform immersion

第10頁 1255585Page 10 1255585

第11頁 1255585 圖式簡單說明 【圖式簡單說明】 第1圖本輕質特寬頻微波吸收材構造示意圖。 第2圖本輕質特寬頻微波吸收材吸收率與頻率關係圖(橫 軸為頻率(G Η z ),縱軸為吸收率(d B ))。 【主要元件符號說明】 1 :本輕質特寬頻微波吸收材構造示意圖 2 :入射電磁波 丨§ 3 :第一層電性均質耗損材 4 :第二層電性均質耗損材 5 :金屬(或電磁波高反射)材Page 11 1255585 Brief description of the diagram [Simple description of the diagram] Figure 1 shows the structure of the lightweight ultra-wideband microwave absorber. Fig. 2 is a graph showing the relationship between the absorption rate and the frequency of the lightweight ultra-wideband microwave absorbing material (the horizontal axis is the frequency (G Η z ), and the vertical axis is the absorption rate (d B )). [Description of main component symbols] 1 : Schematic diagram of the structure of the lightweight ultra-wideband microwave absorber 2: Incident electromagnetic wave 丨 § 3: The first layer of electrically homogeneous depletion material 4: The second layer of electrically homogeneous depletion material 5: Metal (or electromagnetic wave) High reflection

第12頁Page 12

Claims (1)

1255585 六、申請專利範圍 1. 一種輕質特寬頻微波吸收材,係以兩層不同電阻率之電 性均質耗損材及金屬材或電磁波高反射材所組成;其第 一層電性均質耗損材之電阻率為1 0 0 0〜3 Ο Ο Ο Ω / □,厚 度為2. 5〜3. 5 mm,第二層電性均質耗損材之電阻率為 100〜400Ω/Ε],厚度為3.5〜4.5 mm,第三層為金屬材 或電磁波高反射材,此三種材料依次相互緊密接合所 組成。 2. 如申請專利範圍第1項所述之微波吸收材,其中第一 層係為入射微波最先射抵之該層,第二層為入射微 丨_ 波穿透第一層後所射抵之該層,第三層為入射微波穿 透第二層後所射抵之該層。 3. 如申請專利範圍第1項所述之第一層與第二層電性均質 耗損材,其製作方法可以利用PE、PU、PS、PP、ABS、 橡膠等基材以均勻混煉或均勻浸泡導電材,以形成特定 電阻率之均質導電片材。1255585 VI. Scope of Application Patent 1. A lightweight ultra-wideband microwave absorbing material consisting of two layers of electrically uniform and lossy materials with different resistivity and metal or electromagnetic wave high-reflection materials; the first layer of electrically homogeneous wear and loss materials The resistivity is 1 0 0 0~3 Ο Ο Ω Ω / □, the thickness is 2. 5~3. 5 mm, the resistivity of the second layer of electrically homogeneous consumables is 100~400Ω/Ε], and the thickness is 3.5. ~4.5 mm, the third layer is made of metal or electromagnetic wave high-reflection material, which are composed of two materials in close contact with each other. 2. The microwave absorbing material according to claim 1, wherein the first layer is the layer to which the incident microwave is firstly incident, and the second layer is the incident micro 丨 波 wave penetrates the first layer and is irradiated The layer, the third layer is the layer that the incident microwave penetrates after the second layer is penetrated. 3. For the first layer and the second layer of electrically homogeneous consumables as described in item 1 of the patent application, the method of making the same may be to uniformly knead or evenly use a substrate such as PE, PU, PS, PP, ABS or rubber. The conductive material is immersed to form a uniform conductive sheet of a specific resistivity. 第13頁Page 13
TW94131941A 2005-09-16 2005-09-16 Light and super broadband microwave absorbent material TWI255585B (en)

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