CN107706507A - Dual-frequency antenna - Google Patents
Dual-frequency antenna Download PDFInfo
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- CN107706507A CN107706507A CN201610454771.7A CN201610454771A CN107706507A CN 107706507 A CN107706507 A CN 107706507A CN 201610454771 A CN201610454771 A CN 201610454771A CN 107706507 A CN107706507 A CN 107706507A
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
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- H01Q1/36—Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith
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- H—ELECTRICITY
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Abstract
Description
技术领域technical field
本发明涉及一种双频天线,且特别涉及一种可改善共振信号的带宽的双频耦极天线。The invention relates to a dual-frequency antenna, and in particular to a dual-frequency dipole antenna capable of improving the bandwidth of a resonance signal.
背景技术Background technique
随着网络技术的快速发展,无线通信已经与大多数人的生活紧密结合。也因此,具有无线通信功能的便携式电子产品也成为市场的主流。为了提供无线通信功能,便携式电子产品需要通过内建或外接的方式设置天线,并藉由天线接收来自外部的射频(radiofrequency)信号。基于轻薄短小的考虑,便携式电子产品必须使用微型化的天线设计,尽可能的缩小天线本体的大小。With the rapid development of network technology, wireless communication has been closely integrated with the lives of most people. Therefore, portable electronic products with wireless communication functions have also become the mainstream of the market. In order to provide the wireless communication function, the portable electronic product needs to install an antenna through a built-in or an external way, and receive radio frequency (radiofrequency) signals from the outside through the antenna. Based on the consideration of thinness and shortness, portable electronic products must use a miniaturized antenna design to reduce the size of the antenna body as much as possible.
由于无线通信相关产品愈来愈强调实用性与技术性,多频段、宽频的需求也映应而生。为此,便携式电子产品需要支持多种无线通信标准。连带地,便携式电子产品所使用的小型天线也必须能够用于接收不同频段的射频信号。As wireless communication-related products are increasingly emphasizing practicality and technology, the demand for multi-band and broadband has also emerged. To this end, portable electronic products need to support multiple wireless communication standards. Incidentally, the small antennas used in portable electronic products must also be able to receive radio frequency signals in different frequency bands.
发明内容Contents of the invention
本发明涉及一种双频天线,且特别涉及一种可改善带宽的双频耦极天线。本发明的双频天线通过耦合结构改善低频段共振信号的带宽,以及通过斜边区段而改善高频段共振信号的带宽。The invention relates to a dual-frequency antenna, and in particular to a dual-frequency dipole antenna capable of improving bandwidth. The dual-frequency antenna of the present invention improves the bandwidth of the resonance signal in the low frequency band through the coupling structure, and improves the bandwidth of the resonance signal in the high frequency band through the hypotenuse section.
根据本发明的一方面,提出一种双频天线,用于馈入第一共振信号与第二共振信号,其中第二共振信号的频率高于第一共振信号的频率。双频天线包含:第一天线部与第二天线部。第一天线部进一步包含:彼此相连接的第一辐射段与第二辐射段,第一辐射段与第二辐射段间形成第一夹角。第一辐射段的长度对应于第二共振信号的波长;以及第二辐射段的长度对应于第一共振信号的波长。第二天线部包含:一第一子辐射体与第二子辐射体。第一子辐射体包含耦合区段以延伸区段。延伸区段与耦合区段间形成第二夹角。第二子辐射体设置于第一天线部与第一子辐射体间,且第二子辐射体的至少一部分平行于耦合区段。According to one aspect of the present invention, a dual-frequency antenna is provided for feeding a first resonant signal and a second resonant signal, wherein the frequency of the second resonant signal is higher than the frequency of the first resonant signal. The dual-frequency antenna includes: a first antenna part and a second antenna part. The first antenna part further includes: a first radiating section and a second radiating section connected to each other, and a first angle is formed between the first radiating section and the second radiating section. The length of the first radiation segment corresponds to the wavelength of the second resonance signal; and the length of the second radiation segment corresponds to the wavelength of the first resonance signal. The second antenna part includes: a first sub-radiator and a second sub-radiator. The first sub-radiator includes a coupling section to extend the section. A second angle is formed between the extension section and the coupling section. The second sub-radiator is disposed between the first antenna part and the first sub-radiator, and at least a part of the second sub-radiator is parallel to the coupling section.
为了对本发明的上述及其他方面有更佳的了解,下文特举优选实施例,并配合附图,作详细说明如下:In order to have a better understanding of the above-mentioned and other aspects of the present invention, the preferred embodiments are specifically cited below, together with the accompanying drawings, and are described in detail as follows:
附图说明Description of drawings
图1,其本发明构想的双频天线的示意图。Fig. 1 is a schematic diagram of a dual-band antenna conceived by the present invention.
图2,其双频天线的第一天线部的长度配置的示意图。Fig. 2 is a schematic diagram of the length configuration of the first antenna part of the dual-frequency antenna.
图3A、3B,其是不同态样的第一辐射段的示意图。3A and 3B are schematic diagrams of different aspects of the first radiation section.
图4A、4B、4C、4D,其是不同态样的第二辐射段的示意图。4A, 4B, 4C, and 4D are schematic diagrams of different aspects of the second radiation section.
图5,其是双频天线的第二天线部的长度配置的示意图。Fig. 5 is a schematic diagram of the length configuration of the second antenna part of the dual-frequency antenna.
图6A、6B,其是不同态样的第一子辐射体的示意图。6A and 6B are schematic diagrams of different forms of the first sub-radiator.
图7A、7B,其是不同态样的第二子辐射体的示意图。7A and 7B are schematic diagrams of second sub-radiators in different forms.
图8,其是根据本发明构想的双频天线的实施例的示意图。Fig. 8 is a schematic diagram of an embodiment of a dual-band antenna conceived according to the present invention.
图9A、9B、9C,其是对图8所示的双频天线的细部解释的示意图。9A, 9B, and 9C are schematic diagrams illustrating the details of the dual-frequency antenna shown in FIG. 8 .
图10A、10B,其是本发明的双频天线馈入控制信号时的电流路径的示意图。10A and 10B are schematic diagrams of current paths when the dual-frequency antenna of the present invention feeds control signals.
【符号说明】【Symbol Description】
基板10 双频耦极天线1、2Substrate 10 Dual-frequency dipole antenna 1, 2
第一馈入点15a、25a 第二馈入点15b、25bFirst feed point 15a, 25a Second feed point 15b, 25b
第一天线部11、21The first antenna part 11, 21
第一辐射段111、311、312、211The first radiating section 111, 311, 312, 211
第二辐射段112、411、412、413、414、212Second radiating sections 112, 411, 412, 413, 414, 212
第二天线部12、22Second antenna part 12, 22
第一子辐射体121、621、622、221The first sub-radiators 121, 621, 622, 221
耦合区段121a、6211、6221、221aCoupling section 121a, 6211, 6221, 221a
第二延伸区段121b、221bSecond extension section 121b, 221b
第二子辐射体122、721、722、222Second sub-radiators 122, 721, 722, 222
间距d1、d2、d3、d4、d5 第一天线部的长度L1Distance d1, d2, d3, d4, d5 Length L1 of the first antenna part
第一辐射段的长度L11 第二辐射段的长度L12Length L11 of the first radiating section Length L12 of the second radiating section
夹角α1、α2、α3、α4、β1、β2Angle α1, α2, α3, α4, β1, β2
斜边区段3111、3121、211aHypotenuse sections 3111, 3121, 211a
直边区段3122、211b 第一延伸区段4111、4131Straight section 3122, 211b First extension section 4111, 4131
小区段412a、412b、412c、412c、412d、412e、4141a、4141b、4141c、4141d、4141e、6222a、6222b、6222c、6222dSmall segments 412a, 412b, 412c, 412c, 412d, 412e, 4141a, 4141b, 4141c, 4141d, 4141e, 6222a, 6222b, 6222c, 6222d
垂直区段4132、4142 第二天线部的长度L2Length L2 of the vertical section 4132, 4142 second antenna portion
第一子辐射体的长度L21 平行区段的长度L21aThe length L21 of the first sub-radiator The length L21a of the parallel section
第二延伸区段的长度L21bLength L21b of the second extension section
第二子辐射体的长度L22 长边区段721a、722aThe length L22 of the second sub-radiator Long side sections 721a, 722a
短边区段722b 同轴电缆27Short side section 722b coaxial cable 27
射频收发模块29RF transceiver module 29
宽度w1、w2、w3、w4、w5、w6、w7Width w1, w2, w3, w4, w5, w6, w7
第一第一电流CP11 第一第二电流CP12First first current CP11 First second current CP12
第二第一电流CP21 第二第二电流CP22Second first current CP21 Second second current CP22
具体实施方式detailed description
多频段的应用已经成为设计天线时的必要考虑。若便携式电子产品的无线信号传输模块整合了无线局域网络(Wireless LAN)标准的802.11b和802.11a规格,则其天线结构或电路必须设计成能够应用在2.4GHz和5GHz两种不同运作频率。此种可用于接收不同频段的无线通信信号的天线称为双频天线(Dual Band Antenna)。The application of multiple frequency bands has become a necessary consideration when designing antennas. If the wireless signal transmission module of the portable electronic product integrates the 802.11b and 802.11a specifications of the Wireless Local Area Network (Wireless LAN) standard, its antenna structure or circuit must be designed to be applicable to two different operating frequencies of 2.4GHz and 5GHz. Such an antenna capable of receiving wireless communication signals in different frequency bands is called a dual band antenna (Dual Band Antenna).
在设计双频天线时,双频天线的外观必须满足共振的条件,才能用于馈入共振信号。以下以第一共振信号的频率(第一共振频率f1)为2.4GHz、第二共振信号的频率(第二共振频率f2)为5GHz为例子,说明本发明如何设计与双频天线相关的参数。但是,实际应用时,仍可依据不同的共振信号的频率,换算得出应如何调整与代换设计双频天线的长度、角度等参数。When designing a dual-frequency antenna, the appearance of the dual-frequency antenna must meet the conditions of resonance before it can be used to feed the resonance signal. The frequency of the first resonant signal (first resonant frequency f1) is 2.4 GHz and the frequency of the second resonant signal (second resonant frequency f2) is 5 GHz as an example to illustrate how to design parameters related to the dual-band antenna in the present invention. However, in actual application, according to the frequency of different resonance signals, how to adjust and replace the parameters such as the length and angle of the designed dual-frequency antenna can be obtained through conversion.
当双频天线的辐射体的长度例如为共振信号的1/4波长的整数倍时,可达成共振条件,且共振情况会使辐射体天线和馈入部相互匹配。因此,本申请针对频率为2.4GHz的第一共振信号,与频率为5GHz的第二共振信号的应用,根据第一共振波长λ1的四分之一(1/4*λ1=12.5cm/4=31.25毫米(millimeter,简称为mm)),与第二共振波长λ2的四分之一(1/4*λ2=6cm/4=15mm)而设计与双频天线相关的长度参数。此外,天线长度也可以设计为与1/1*λ1、1/1*λ2、1/2*λ1或1/2*λ2相关。When the length of the radiator of the dual-frequency antenna is, for example, an integer multiple of 1/4 wavelength of the resonance signal, the resonance condition can be achieved, and the resonance condition will make the radiator antenna and the feeding part match each other. Therefore, the present application aims at the application of the first resonant signal with a frequency of 2.4GHz and the second resonant signal with a frequency of 5GHz, according to a quarter of the first resonant wavelength λ1 (1/4*λ1=12.5cm/4= 31.25 mm (millimeter, mm for short), and a quarter of the second resonance wavelength λ2 (1/4*λ2=6cm/4=15mm) to design the length parameters related to the dual-frequency antenna. In addition, the antenna length can also be designed to be related to 1/1*λ1, 1/1*λ2, 1/2*λ1 or 1/2*λ2.
请参见图1,其本发明构想的双频耦极天线的示意图。设置于基板10的双频耦极天线1包含:第一馈入点15a、第二馈入点15b、第一天线部11以及第二天线部12。在以下说明中,以垂直方向的网底代表第一天线部11的辐射体,以格线状的网底代表第二天线部12的辐射体,其中,并以粗黑体的虚线划分不同的区段。须留意的是,由粗黑体虚线划分的各个区段间,仍然彼此相连接。Please refer to FIG. 1 , which is a schematic diagram of a dual-frequency dipole antenna contemplated by the present invention. The dual-band dipole antenna 1 disposed on the substrate 10 includes: a first feeding point 15 a , a second feeding point 15 b , a first antenna part 11 and a second antenna part 12 . In the following description, the radiator of the first antenna part 11 is represented by the bottom of the grid in the vertical direction, and the radiator of the second antenna part 12 is represented by the grid bottom of the grid line, and different regions are divided by bold dotted lines. part. It should be noted that the segments demarcated by bold bold dotted lines are still connected to each other.
为便于说明,此处假设基板10具有矩形外观,其长边平行于x方向(第一方向),短边则平行于y方向(第二方向)。基板10可为玻璃纤维材质的单面印刷电路板、双层或多层印刷电路板等。双频耦极天线1的辐射体使用金属导电材质。若基板10为双层或多层印刷电路板,则在双频耦极天线1的位置相对应的其他侧不能形成、设置任何金属结构,以避免双频耦极天线1在馈入共振信号时,受到他侧的干扰。For the sake of illustration, it is assumed here that the substrate 10 has a rectangular appearance, its long side is parallel to the x direction (the first direction), and its short side is parallel to the y direction (the second direction). The substrate 10 can be a single-sided printed circuit board made of glass fiber, a double-layer or multi-layer printed circuit board, and the like. The radiator of the dual-frequency dipole antenna 1 is made of metal conductive material. If the substrate 10 is a double-layer or multi-layer printed circuit board, no metal structure can be formed or arranged on the other side corresponding to the position of the dual-frequency dipole antenna 1, so as to prevent the dual-frequency dipole antenna 1 from feeding a resonance signal. , interfered by his side.
如图1所示,本发明的辐射体是基于长条形的设计,因此,辐射体的侧边的长度约等于其中心线的长度。基于布线的便利性考虑,辐射体的宽度大致相等,例如宽度可设计为第一共振波长λ1的千分之一倍,12.5cm/1000=0.125mm。As shown in FIG. 1 , the radiator of the present invention is based on a strip-shaped design. Therefore, the length of the sides of the radiator is approximately equal to the length of its centerline. Considering the convenience of wiring, the width of the radiator is roughly equal, for example, the width can be designed to be one-thousandth of the first resonance wavelength λ1, 12.5cm/1000=0.125mm.
根据本发明的实施例,第一天线部11仅包含一个辐射体;第二天线部12包含两个彼此平行相隔一小段距离的第一子辐射体121、第二子辐射体122。其中,第二子辐射体122的位置在第一天线部11与第一子辐射体121间,且第二子辐射体122的长度较第一天线部11与第一子辐射体121短。此外,第二子辐射体122与第一天线部11之间的间距d1须大于或等于1mm。According to an embodiment of the present invention, the first antenna part 11 includes only one radiator; the second antenna part 12 includes two first sub-radiator 121 and second sub-radiator 122 parallel to each other and separated by a small distance. Wherein, the position of the second sub-radiator 122 is between the first antenna part 11 and the first sub-radiator 121 , and the length of the second sub-radiator 122 is shorter than that of the first antenna part 11 and the first sub-radiator 121 . In addition, the distance d1 between the second sub-radiator 122 and the first antenna part 11 must be greater than or equal to 1 mm.
第一天线部11可划分为两个部分,第一辐射段111与第二辐射段112。其中,第二辐射段112与第一辐射段111之间有一夹角α1。在第二天线部12中,第一子辐射体121可进一步划分为耦合区段121a与第二延伸区段121b。其中,耦合区段121a与第二延伸区段121b之间有一夹角β1。根据本发明的构想,耦合区段121a与第二子辐射体122平行设置,且耦合区段121a与第二子辐射体122之间的距离相当接近而能形成耦合效应。The first antenna part 11 can be divided into two parts, the first radiating section 111 and the second radiating section 112 . Wherein, there is an angle α1 between the second radiating section 112 and the first radiating section 111 . In the second antenna part 12, the first sub-radiator 121 can be further divided into a coupling section 121a and a second extending section 121b. Wherein, there is an included angle β1 between the coupling section 121a and the second extension section 121b. According to the idea of the present invention, the coupling section 121a is arranged parallel to the second sub-radiator 122 , and the distance between the coupling section 121a and the second sub-radiator 122 is quite close to form a coupling effect.
如图1所示的双频耦极天线中,各个辐射体的长度、外观、设置的位置等,均可进一步改变与调整。以下分别说明设计第一天线部11与第二天线部12的外观时,可能搭配的几种方式。实际应用时,可因应基板的空间等因素而选择、设计第一天线部与第二天线部的外观。后附各附图的辐射体的各种外观,也可任意搭配、组合使用。In the dual-frequency dipole antenna shown in FIG. 1 , the length, appearance, and location of each radiator can be further changed and adjusted. The following describes several ways of possible matching when designing the appearance of the first antenna part 11 and the second antenna part 12 . In actual application, the appearance of the first antenna part and the second antenna part can be selected and designed according to factors such as the space of the substrate. The various appearances of the radiators in the accompanying drawings can also be used in any combination and combination.
请参见图2,其是双频耦极天线的第一天线部的长度配置的示意图。第一天线部11以第一辐射段111搭配第二共振信号使用。因此,将第一辐射段111的长度L11设计为第二共振波长λ2的四分之一,L11=1/4*λ2。第一天线部11以第二辐射段112搭配第一共振信号使用。因此,将第二辐射段112的长度L12设计为第一共振波长λ1的四分之一,L12=1/4*λ1。Please refer to FIG. 2 , which is a schematic diagram of the length configuration of the first antenna part of the dual-frequency dipole antenna. The first antenna part 11 uses the first radiation section 111 to cooperate with the second resonance signal. Therefore, the length L11 of the first radiation section 111 is designed to be a quarter of the second resonance wavelength λ2, L11=1/4*λ2. The first antenna part 11 uses the second radiation section 112 to cooperate with the first resonance signal. Therefore, the length L12 of the second radiating section 112 is designed to be a quarter of the first resonance wavelength λ1, L12=1/4*λ1.
延续前述说明可以得知,若第一共振频率为2.4GHz、第二共振频率为5GHz时,则第一辐射段的长度L11约为15mm、第二辐射段的长度L12约为31.25mm。第一天线部11的长度L1等于第一辐射段111的长度与第二辐射段112的长度的总和,即,L1=L11+L12=1/4*(λ1+λ2)。例如:15+31.25=46.25mm。此外,因为第二共振频率大于第一共振频率的两倍,使得第一共振信号的波长大于第一共振信号的波长的两倍。也因此,在图2中,1/4*λ2<1/2*1/4*λ1。Continuing the foregoing description, it can be known that if the first resonant frequency is 2.4 GHz and the second resonant frequency is 5 GHz, the length L11 of the first radiating section is about 15 mm, and the length L12 of the second radiating section is about 31.25 mm. The length L1 of the first antenna part 11 is equal to the sum of the lengths of the first radiating section 111 and the second radiating section 112 , ie, L1=L11+L12=1/4*(λ1+λ2). For example: 15+31.25=46.25mm. In addition, because the second resonance frequency is greater than twice the first resonance frequency, the wavelength of the first resonance signal is greater than twice the wavelength of the first resonance signal. Therefore, in Figure 2, 1/4*λ2<1/2*1/4*λ1.
以下,利用图3A、3B说明第一辐射段111可能的外观变化;利用图4A、4B、4C、4D说明第二辐射段111可能的外观变化。其中,第一辐射段111与第二辐射段111的各种外观变化可彼此搭配,并不需要特别限定。Hereinafter, possible appearance changes of the first radiating section 111 will be described by using FIGS. 3A and 3B ; possible appearance changes of the second radiating section 111 will be described by using FIGS. 4A , 4B, 4C and 4D. Wherein, various appearance changes of the first radiating section 111 and the second radiating section 111 can be matched with each other, and no special limitation is required.
第一辐射段111的外观可进一步分为两类,第一类为仅包含斜边区段的情形(如图3A所示);第二类为包含斜边区段与直边区段的情形(如图3B所示)。The appearance of the first radiating section 111 can be further divided into two categories, the first category is the situation including only the hypotenuse section (as shown in Figure 3A); the second category is the situation including the hypotenuse section and the straight section (as shown in Figure 3A). 3B).
请参见图3A,其是第一辐射段仅包含斜边区段的示意图。因图3A的第一辐射段311仅包含斜边区段3111,此处斜边区段3111的长度L11a等于第一辐射段311的长度L11。即,L11a=L11=1/4*λ2。此外,斜边区段3111与垂直方向之间的夹角α2需符合0°<α2<90°的限制。Please refer to FIG. 3A , which is a schematic diagram of the first radiating section including only the hypotenuse section. Since the first radiating section 311 in FIG. 3A only includes the hypotenuse section 3111 , the length L11 a of the hypotenuse section 3111 is equal to the length L11 of the first radiating section 311 . That is, L11a=L11=1/4*λ2. In addition, the angle α2 between the hypotenuse section 3111 and the vertical direction must meet the restriction of 0°<α2<90°.
请参见图3B,其是第一辐射段同时包含斜边区段与直边区段的示意图。若第一辐射段312同时包含斜边区段3121与直边区段3122,则斜边区段3121的长度L11a与直边区段3122的长度L11b的总和等于第一辐射段311的长度L11。即,L11a+L11b=L11=1/4*λ2。其中,斜边区段3121的长度L11a可能小于、等于、大于直边区段3122的长度L11b。Please refer to FIG. 3B , which is a schematic diagram of the first radiating section including both a hypotenuse section and a straight section. If the first radiating section 312 includes both the hypotenuse section 3121 and the straight section 3122 , the sum of the length L11 a of the hypotenuse section 3121 and the length L11 b of the straight section 3122 is equal to the length L11 of the first radiating section 311 . That is, L11a+L11b=L11=1/4*λ2. Wherein, the length L11a of the hypotenuse section 3121 may be less than, equal to, or greater than the length L11b of the straight section 3122 .
斜边区段3121与垂直方向的夹角α4大于0°,斜边区段3121与直边区段312的夹角α3大于或等于90°。斜边区段3121可以上方的端点为中心,朝逆时针方向偏移,进而改变夹角α4的大小。同样的,直边区段3122可以利用与斜边区段3121的连接处为端点,朝逆时针方向或顺时针方向偏移,进而改变夹角α3的大小。夹角α3为180°时,相当在仅包含斜边区段的情形。实际应用时,斜边区段3121与直边区段3122可偏移的幅度,可以直边区段3122不会与第二辐射段碰触为原则。The included angle α4 between the hypotenuse section 3121 and the vertical direction is greater than 0°, and the included angle α3 between the hypotenuse section 3121 and the straight section 312 is greater than or equal to 90°. The hypotenuse section 3121 can be shifted counterclockwise with the upper endpoint as the center, thereby changing the size of the included angle α4. Similarly, the straight side section 3122 can use the connection point with the hypotenuse section 3121 as an end point, and can be shifted counterclockwise or clockwise, thereby changing the size of the included angle α3. When the included angle α3 is 180°, it corresponds to the situation that only includes the hypotenuse section. In actual application, the offset range between the hypotenuse section 3121 and the straight section 3122 can be based on the principle that the straight section 3122 does not touch the second radiation section.
第二辐射段112的外观可进一步分为两类,第一类为仅包含第一延伸区段的情形(如第4A、4B图所示);第二类为同时包含第一延伸区段与垂直区段的情形(如图4C、4D所示)。无论是哪一类情形,第二辐射段112的长度L12均为1/4*λ1(例如:31.25mm)。The appearance of the second radiating section 112 can be further divided into two categories. The first category includes only the first extension section (as shown in Figures 4A and 4B); the second category includes both the first extension section and the first extension section. The situation of the vertical section (as shown in Fig. 4C, 4D). In any case, the length L12 of the second radiating section 112 is 1/4*λ1 (for example: 31.25 mm).
第二辐射段仅包含第一延伸区段的情形,可依据第一延伸段的外观而再进一步分为两类,其一为,第一延伸区段本身为不具任何折角,单纯为一长条形的外观(如图4A所示);其二为,第一延伸区段本身包含多个小区段,且各个小区段间形成折角,且第一延伸段的整体外观呈现凹凸状(如图4B所示)。在第4A、4B图中,第二辐射段的长度等于第一延伸区段的长度L12a。因此,第一延伸区段的长度L12a为第一共振波长λ1的四分之一,L12a=1/4*λ1。In the case where the second radiating section only includes the first extension section, it can be further divided into two types according to the appearance of the first extension section. One is that the first extension section itself does not have any corners and is simply a long strip. Shaped appearance (as shown in Figure 4A); the second is that the first extension section itself contains a plurality of small sections, and the corners are formed between each small section, and the overall appearance of the first extension section is concave-convex (as shown in Figure 4B shown). In Figures 4A and 4B, the length of the second radiating section is equal to the length L12a of the first extending section. Therefore, the length L12a of the first extension section is a quarter of the first resonance wavelength λ1, L12a=1/4*λ1.
请参见图4A,其是第二辐射段仅包含第一延伸区段,且第一延伸区段不具任何折角的示意图。第二辐射段411仅包含第一延伸区段4111,且第一延伸区段4111为水平方向。因此,第一延伸区段4111与垂直方向之间的夹角α5例如为直角。即,α5=90°。Please refer to FIG. 4A , which is a schematic diagram of the second radiating section only including the first extension section, and the first extension section does not have any corners. The second radiating section 411 only includes the first extension section 4111 , and the first extension section 4111 is in a horizontal direction. Therefore, the included angle α5 between the first extension section 4111 and the vertical direction is, for example, a right angle. That is, α5=90°.
请参见图4B,其是假设第二辐射段仅包含第一延伸区段,且第一延伸区段包含折角的示意图。第二辐射段412包含第一延伸区段,且第一延伸区段可进一步区分为多个长度较短的小区段4121a、4121b、4121c、4121d、4121e。这些小区段4121a、4121b、4121c、4121d、4121e彼此间形成约90°的折角。Please refer to FIG. 4B , which is a schematic diagram assuming that the second radiating section only includes the first extension section, and the first extension section includes a knuckle. The second radiating section 412 includes a first extending section, and the first extending section can be further divided into a plurality of small sections 4121a, 4121b, 4121c, 4121d, 4121e with shorter lengths. These small segments 4121a, 4121b, 4121c, 4121d, 4121e form a knuckle with each other of about 90°.
将第一延伸区段加以曲折(meander)形成折角的作法,可以缩小双频天线在基板上占用的面积。实际应用时,第一延伸区段是否具有折角、由折角所区隔的各个小区段的长度,以及折角数量等,并不需要受到限制。The method of meandering the first extension section to form a knuckle can reduce the area occupied by the dual-band antenna on the substrate. In actual application, whether the first extension section has a knuckle, the length of each small section separated by the knuckle, and the number of knuckles do not need to be limited.
为避免第一辐射段与第二辐射段过于接近,除第一延伸区段外,第二辐射段另可使用垂直区段。其中,第一延伸区段的长度较垂直区段长。图4C、4D为第二辐射段同时包含第一延伸区段与垂直区段的情形,其中图4C对应于第一延伸区段不具折角的情形,图4D对应于第一延伸区段具折角的情形。In order to prevent the first radiating section from being too close to the second radiating section, in addition to the first extending section, the second radiating section can also use a vertical section. Wherein, the length of the first extension section is longer than that of the vertical section. Figures 4C and 4D show the situation where the second radiating section includes both the first extension section and the vertical section, wherein Figure 4C corresponds to the situation where the first extension section does not have a knuckle, and Figure 4D corresponds to the situation where the first extension section has a knuckle situation.
请参见图4C,其是第二辐射段同时包含第一延伸区段与垂直区段,且第一延伸区段不具折角的示意图。第二辐射段413包含第一延伸区段4131与垂直区段4132。第一延伸区段4131的长度L12a,以及垂直区段4132的长度L12b的总和(L12a+L12b)相当在第二辐射段的长度L12。即,L12a+L12b=L12=1/4*λ1。Please refer to FIG. 4C , which is a schematic diagram showing that the second radiating section includes both the first extending section and the vertical section, and the first extending section has no corner. The second radiating section 413 includes a first extending section 4131 and a vertical section 4132 . The sum (L12a+L12b) of the length L12a of the first extension section 4131 and the length L12b of the vertical section 4132 is equivalent to the length L12 of the second radiating section. That is, L12a+L12b=L12=1/4*λ1.
请参见图4D,其是假设第二辐射段同时包含第一延伸区段与垂直区段,且第一延伸区段具有折角的示意图。第二辐射段414同时包含第一延伸区段与垂直区段4142,其中第一第一延伸区段由多个长度较短的小区段4141a、4141b、4141c、4141d、4141e组成。尽管图4D绘出五个小区段,但是第一延伸区段实际包含的折角数量、小区段的长度等,并不需要限制。Please refer to FIG. 4D , which is a schematic diagram assuming that the second radiating section includes both the first extending section and the vertical section, and the first extending section has a knuckle. The second radiating section 414 includes both a first extending section and a vertical section 4142 , wherein the first extending section is composed of a plurality of shorter small sections 4141a, 4141b, 4141c, 4141d, 4141e. Although FIG. 4D depicts five small segments, the number of knuckles actually included in the first extension segment, the length of the small segments, etc., are not limited.
请参见图5,其是双频耦极天线的第二天线部的长度配置的示意图。第二天线部12包含第一子辐射体121与第二子辐射体122。第二子辐射体122的长度L22短于第一子辐射体121的长度L21。由于第一子辐射体121的耦合区段121a与第二子辐射体122之间形成耦合的缘故,可以使得第二天线部12的总长度短于1/4*λ1。即,L21+L22=L2<1/4*λ1。Please refer to FIG. 5 , which is a schematic diagram of the length configuration of the second antenna part of the dual-frequency dipole antenna. The second antenna part 12 includes a first sub-radiator 121 and a second sub-radiator 122 . The length L22 of the second sub-radiator 122 is shorter than the length L21 of the first sub-radiator 121 . Due to the coupling formed between the coupling section 121 a of the first sub-radiator 121 and the second sub-radiator 122 , the total length of the second antenna part 12 can be made shorter than 1/4*λ1. That is, L21+L22=L2<1/4*λ1.
第一子辐射体121可进一步包含耦合区段121a与第二延伸区段121b。因此,第一子辐射体121的长度21相当在耦合区段121a的长度L21a与第二延伸区段121b的长度L21b的总和,即,L21=(L21a+L21b)。The first sub-radiator 121 may further include a coupling section 121a and a second extension section 121b. Therefore, the length 21 of the first sub-radiator 121 is equal to the sum of the length L21a of the coupling section 121a and the length L21b of the second extension section 121b, ie, L21=(L21a+L21b).
以下说明第一子辐射体121与第二子辐射体122的外观可能的变化。其中,关于第一子辐射体121的外观变化,将于图6A、6B说明。关于第二子辐射体122的外观变化,将于图7A、7B说明。The following describes possible changes in the appearance of the first sub-radiator 121 and the second sub-radiator 122 . Wherein, the appearance change of the first sub-radiator 121 will be described in FIGS. 6A and 6B . The appearance change of the second sub-radiator 122 will be described in FIGS. 7A and 7B .
依据第二延伸区段的外观不同,第一子辐射体121的外观可进一步分为两类。其一为,第二延伸区段为一长条形的外观,不具任何折角;其二为,第二延伸区段具有至少一个折角处,其整体外观呈现凹凸状。图6A、6B分为第一子辐射体的第二延伸区段不具折角、具有折角的情形。According to the appearance of the second extension section, the appearance of the first sub-radiator 121 can be further divided into two types. One is that the second extension section has an elongated appearance without any corners; the other is that the second extension section has at least one corner, and its overall appearance is concave-convex. 6A and 6B are divided into cases where the second extension section of the first sub-radiator does not have a corner and has a corner.
请参见图6A,其是第二延伸区段不具折角的示意图。第一子辐射体621包含耦合区段6211与第二延伸区段6212。其中耦合区段6211平行于垂直方向。耦合区段6211的长度为L21a,第二延伸区段6212的长度为L21b。由于第一子辐射体121的长度L21须满足:1/4*λ2<L21<1/4*λ1,耦合区段6211与第二延伸区段6212的长度总和必须符合1/4*λ2<L21a+L21b=L21<1/4*λ1的限制。此外,耦合区段6211与第二延伸区段6212之间的夹角β1介于90°与180°间。即,(90≦β1≦180)。Please refer to FIG. 6A , which is a schematic diagram of the second extension section without a corner. The first sub-radiator 621 includes a coupling section 6211 and a second extension section 6212 . Wherein the coupling section 6211 is parallel to the vertical direction. The length of the coupling section 6211 is L21a, and the length of the second extension section 6212 is L21b. Since the length L21 of the first sub-radiator 121 must satisfy: 1/4*λ2<L21<1/4*λ1, the sum of the lengths of the coupling section 6211 and the second extension section 6212 must meet 1/4*λ2<L21a +L21b=Limitation of L21<1/4*λ1. In addition, the angle β1 between the coupling section 6211 and the second extension section 6212 is between 90° and 180°. That is, (90≦β1≦180).
请参见图6B,其是第二延伸区段具有折角的示意图。第一子辐射体621包含耦合区段6221与第二延伸区段。在此图式中,第二延伸区段包含多个长度较短的小区段6221a、6221b、6221c、6221d、6221e。第二延伸区段是否包含折角、各个小区段的长度,以及其折角数量并不需要受到限制。Please refer to FIG. 6B , which is a schematic diagram of the second extension section having a knuckle. The first sub-radiator 621 includes a coupling section 6221 and a second extension section. In this figure, the second extension section includes a plurality of small sections 6221a, 6221b, 6221c, 6221d, 6221e of shorter length. Whether the second extension section includes a knuckle, the length of each small section, and the number of knuckles do not need to be limited.
如图3B、4B、6B中所述,当第一延伸区段和/或第二延伸区段具有折角时,其折角数量并不需要限定,且各个小区段的长度并不需要限定需要等长。在第一延伸区段和/或第二延伸区段所包含的一个或以上的小区段中,若是以与其他辐射体(例如图3B、4B的第一辐射段,以及图6的耦合区段)相连接者开始编号,则其中属于奇数编号的小区段彼此平行,且属于奇数编号的小区段垂直于属于偶数编号的小区段。As shown in Figures 3B, 4B, and 6B, when the first extension section and/or the second extension section have knuckles, the number of knuckles does not need to be limited, and the length of each small section does not need to be limited and needs to be equal. . In one or more small segments included in the first extension section and/or the second extension section, if it is combined with other radiators (such as the first radiation section in Figure 3B, 4B, and the coupling section in Figure 6 ) start numbering, then the small segments belonging to the odd numbers are parallel to each other, and the small segments belonging to the odd numbers are perpendicular to the small segments belonging to the even numbers.
第二子辐射体的外观可进一步分为两类,第一类为仅包含长边区段的情形(如图7A所示,I型形状);第二类为包含长边区段与短边区段的情形(如图7B所示,倒L型形状)。The appearance of the second sub-radiator can be further divided into two categories, the first category is the situation that only includes the long side section (as shown in Figure 7A, I-shaped); the second category is the situation that includes the long side section and the short side section Situation (as shown in Figure 7B, inverted L shape).
请参见图7A,其是第二子辐射体仅包含长边区段的示意图。当第二子辐射体721仅包含长边区段721a时,第二馈入点(未绘式)将设置在长边区段721a的顶端。在图7A中,第二子辐射体721与第一天线部(未绘式)之间的最短距离相当在长边区段721a的右侧边至第一天线部L1间的距离。Please refer to FIG. 7A , which is a schematic diagram of the second sub-radiator only including the long side section. When the second sub-radiator 721 only includes the long side section 721a, the second feeding point (not shown) will be set at the top of the long side section 721a. In FIG. 7A , the shortest distance between the second sub-radiator 721 and the first antenna part (not shown) corresponds to the distance from the right side of the long side section 721 a to the first antenna part L1 .
请参见图7B,其是第二子辐射体同时包含长边区段与短边区段的示意图。如图7所示,第二子辐射体同时包含长边区段722a与短边区段722b。其中长边区段722a的长度L22a较短边区段722b的长度L22b,且两者之间的夹角β2为直角(β2=90°)。当第二子辐射体722为L型形状时,将第二馈入点(未绘式)设置于短边区段722b的最右侧。此时,第二子辐射体722与第一天线部(未绘式)之间的最短距离,相当在短边区段722b的最右侧边缘至第一天线部L1间的距离。Please refer to FIG. 7B , which is a schematic diagram of the second sub-radiator including both the long-side section and the short-side section. As shown in FIG. 7 , the second sub-radiator includes both a long side section 722 a and a short side section 722 b. The length L22a of the long side section 722a is shorter than the length L22b of the short side section 722b, and the angle β2 between them is a right angle (β2=90°). When the second sub-radiator 722 is L-shaped, the second feeding point (not shown) is disposed at the far right of the short side section 722b. At this time, the shortest distance between the second sub-radiator 722 and the first antenna part (not shown) corresponds to the distance from the rightmost edge of the short side section 722b to the first antenna part L1.
请参见图8,其是根据本发明构想的双频耦极天线的实施例的示意图。双频耦极天线2设置于基板20,依据射频收发模块(transceiver)29的控制,同轴电缆27与双频耦极天线20经由馈入点馈入第一共振信号与第二共振信号。第一馈入点25a用于馈入接地信号,且第二馈入点25b用于馈入电磁信号。Please refer to FIG. 8 , which is a schematic diagram of an embodiment of a dual-frequency dipole antenna conceived according to the present invention. The dual-frequency dipole antenna 2 is disposed on the substrate 20. According to the control of the radio frequency transceiver module (transceiver) 29, the coaxial cable 27 and the dual-frequency dipole antenna 20 are fed into the first resonance signal and the second resonance signal through the feeding point. The first feeding point 25a is used for feeding ground signals, and the second feeding point 25b is used for feeding electromagnetic signals.
当共振信号通过第一馈入点25a与第二馈入点25b传送时,电流经传输线产生波导(waveguide)而形成电磁波辐射出去,达成电磁信号的传送;当共振信号通过第一馈入点25a与第二馈入点25b接收时,电磁能的辐射经由天线接收形成无线电频率的电能,从而达成电磁信号的传输。When the resonance signal is transmitted through the first feeding point 25a and the second feeding point 25b, the current generates a waveguide (waveguide) through the transmission line to form an electromagnetic wave to radiate out, thereby achieving the transmission of the electromagnetic signal; when the resonance signal passes through the first feeding point 25a When receiving with the second feeding point 25b, the radiation of electromagnetic energy is received through the antenna to form electric energy of radio frequency, thereby achieving the transmission of electromagnetic signals.
第二子辐射体222与第一子辐射体221的耦合区段221a共同形成耦合结构,且第二子辐射体222的长度L22与第一子辐射体221的耦合区段221a的长度相当接近。当第二子辐射体222为I型形状时,第二子辐射体222的长度小于或等于第一子辐射体的耦合区段的长度。当第二子辐射体222为倒L型形状时,长边区段的长度小于或等于第一子辐射体221的耦合区段221a的长度。此时,短边区段的长度会影响第二子辐射体222与第一子辐射体221的耦合区段221a的长度之间的比较结果。The second sub-radiator 222 and the coupling section 221a of the first sub-radiator 221 jointly form a coupling structure, and the length L22 of the second sub-radiator 222 is quite close to the length of the coupling section 221a of the first sub-radiator 221 . When the second sub-radiator 222 has an I-shaped shape, the length of the second sub-radiator 222 is less than or equal to the length of the coupling section of the first sub-radiator. When the second sub-radiator 222 is in an inverted L shape, the length of the long side section is less than or equal to the length of the coupling section 221 a of the first sub-radiator 221 . At this time, the length of the short side section will affect the comparison result between the length of the second sub-radiator 222 and the length of the coupling section 221 a of the first sub-radiator 221 .
请参见图9A,其是双频耦极天线中的第一天线部的示意图。通过斜边区段211a的使用,双频耦极天线在馈入高频段的共振信号时,可具有较大的带宽范围。经模拟确认后,针对第二共振频率为5GHz的应用,高频段的共振信号的带宽由1150MHz增加至1870MHz。即,本申请的双频耦极天线可改善高频段的共振信号的带宽幅度达62.6%。因馈入点设置于斜边区段211a的缘故,为了避免在焊接馈入点时产生短路,斜边区段211a的宽度w2较直边区段211b的宽度w1宽(w2>w1)。Please refer to FIG. 9A , which is a schematic diagram of the first antenna part in the dual-frequency dipole antenna. Through the use of the hypotenuse section 211a, the dual-frequency dipole antenna can have a larger bandwidth range when feeding a high-frequency resonance signal. After confirmation by simulation, for the application of the second resonance frequency of 5 GHz, the bandwidth of the resonance signal in the high frequency band is increased from 1150 MHz to 1870 MHz. That is, the dual-frequency dipole antenna of the present application can improve the bandwidth of the resonant signal in the high frequency band by 62.6%. Since the feed-in point is disposed on the beveled section 211a, in order to avoid short circuit when soldering the feed-in point, the width w2 of the beveled section 211a is wider than the width w1 of the straight section 211b (w2>w1).
请参见图9B,其双频耦极天线中的第二天线部。本发明的双频耦极天线在第二天线部使用耦合结构,此种做法可以改善馈入低频段的共振信号的带宽。模拟结果显示,针对第一共振频率为2.4GHz的应用,第一共振信号的带宽可由100MHz增加至120MHz,增幅达20%。Please refer to FIG. 9B , the second antenna part of the dual-frequency dipole antenna. The dual-frequency dipole antenna of the present invention uses a coupling structure in the second antenna part, which can improve the bandwidth of the resonance signal fed into the low frequency band. Simulation results show that for the application of the first resonance frequency of 2.4GHz, the bandwidth of the first resonance signal can be increased from 100MHz to 120MHz, an increase of 20%.
在此附图中,第二子辐射体222与耦合区段221b的间距d2小于0.8mm(0<d2<0.8)。第二子辐射体222的短边区段222b的长度介于0~3.2mm、长边区段222a长度介于7.25mm与8.25mm间。据此,此实施例中的长边区段222a的长度与短边区段222b的长度范围间的比值介于2.578125与无限大(∞)间。In this figure, the distance d2 between the second sub-radiator 222 and the coupling section 221b is less than 0.8mm (0<d2<0.8). The length of the short side section 222b of the second sub-radiator 222 is between 0-3.2mm, and the length of the long side section 222a is between 7.25mm and 8.25mm. Accordingly, the ratio of the length of the long side section 222 a to the length of the short side section 222 b in this embodiment is between 2.578125 and infinity (∞).
基于布线时的便利性考虑,在第9A、9B图中,除了斜边区段211a的宽度w2外,直边区段212b的宽度w1、第一延伸区段的宽度w3;短边区段222b的宽度w6;以及长边区段222a的宽度w5、第二延伸区段221b的宽度w7可能彼此相等。Considering the convenience of wiring, in Figures 9A and 9B, in addition to the width w2 of the hypotenuse section 211a, the width w1 of the straight section 212b, the width w3 of the first extension section; the width w6 of the short section 222b ; and the width w5 of the long side section 222a and the width w7 of the second extension section 221b may be equal to each other.
或者,长边区段222a的宽度w5仅次于斜边区段211a的宽度w2,但较短边区段222b的宽度w6、第一天线部中的直边区段212b的宽度w1、第一延伸区段的宽度w3,以及较第一子辐射体221的耦合区段221a的宽度w4、第二延伸区段221b的宽度w7更宽。Alternatively, the width w5 of the long-side section 222a is second only to the width w2 of the hypotenuse section 211a, but the width w6 of the short-side section 222b, the width w1 of the straight-side section 212b in the first antenna part, the width w1 of the first extension section The width w3 is wider than the width w4 of the coupling section 221 a of the first sub-radiator 221 and the width w7 of the second extension section 221 b.
请参见图9C,其是进一步说明本发明实施例的双频耦极天线的相对位置的示意图。间距d3为长边区段与斜边区段之间的最短距离。间距d4为垂直区段中,较靠近第二天线部13的一侧,与短边区段的侧边之间的最段距离。间距d5为斜边区段与第一延伸区段间的最短距离。基于设置馈入点的考虑,在图9C中,间距d3与间距d4至少为1mm。此外,间距d5必须大于0mm。实际应用时,无论第二子辐射体222具有倒L型形状或是I型形状,第二子辐射体222与第一辐射段211间的最小距离,主要取决于馈入点所需的焊接空间。即,用于避免馈入点25a与馈入点25b间短路。Please refer to FIG. 9C , which is a schematic diagram further illustrating the relative positions of the dual-frequency dipole antennas according to the embodiment of the present invention. The distance d3 is the shortest distance between the long side section and the hypotenuse section. The distance d4 is the longest distance between the side closer to the second antenna portion 13 and the side of the short side section in the vertical section. The distance d5 is the shortest distance between the hypotenuse section and the first extension section. Based on the consideration of setting the feeding point, in FIG. 9C , the spacing d3 and the spacing d4 are at least 1 mm. Furthermore, the distance d5 must be greater than 0 mm. In actual application, regardless of whether the second sub-radiator 222 has an inverted L shape or an I-shape, the minimum distance between the second sub-radiator 222 and the first radiating section 211 mainly depends on the welding space required for the feeding point . That is, it is used to avoid a short circuit between the feeding point 25a and the feeding point 25b.
随着所使用的频段不同,双频耦极天线中的电流路径也随着改变。图10A、10B分别代双频耦极天线应用在低频段、高频段的共振信号时的电流路径。With the different frequency bands used, the current path in the dual-frequency dipole antenna also changes. FIGS. 10A and 10B respectively represent the current paths when the dual-frequency dipole antenna is applied to resonance signals in the low frequency band and high frequency band.
请参见图10A,其是双频耦极天线用于馈入第一共振信号的示意图。第一第一电流CP11流经第一天线部21的第二辐射段,第一第二电流CP12流经第二天线部22的第一子辐射体221与第二子辐射体222。随着射频收发模块29设定为传送用途或接收用途的不同,第一第一电流CP11与第一第二电流CP12的流向将随着改变。无论电流的流向为何,电流强度会与馈入点间的距离远近成反比。因此第一第一电流CP11在靠近第一馈入点25a处的电流强度较强;以及,第一第二电流CP12在靠近第二馈入点25b处的电流强度较强。Please refer to FIG. 10A , which is a schematic diagram of a dual-frequency dipole antenna used to feed the first resonance signal. The first first current CP11 flows through the second radiation section of the first antenna part 21 , and the first second current CP12 flows through the first sub-radiator 221 and the second sub-radiator 222 of the second antenna part 22 . Depending on whether the RF transceiver module 29 is set for transmission or reception, the flow directions of the first first current CP11 and the first second current CP12 will change accordingly. Regardless of the direction in which the current flows, the intensity of the current will be inversely proportional to the distance between the feed points. Therefore, the first first current CP11 has a stronger current intensity near the first feeding point 25 a; and, the first second current CP12 has a stronger current intensity near the second feeding point 25 b.
请参见图10B,其是双频耦极天线用于馈入第二共振信号的示意图。第二第一电流CP21流经第一天线部21的第一辐射段。在此同时,第二第二电流CP22流经第一子辐射体221的一部分、第二子辐射体222。随着射频收发模块29设定为传送用途或接收用途的不同,第二第一电流CP21与第二第二电流CP22的流向将随着改变。无论电流的流向为何,电流强度会与馈入点间的距离远近成反比。因此第二第一电流CP21在靠近第一馈入点25a处的电流强度较强,且第二第二电流CP22在靠近第二馈入点25b处的电流强度较强。Please refer to FIG. 10B , which is a schematic diagram of a dual-frequency dipole antenna used to feed the second resonance signal. The second first current CP21 flows through the first radiation section of the first antenna part 21 . At the same time, the second second current CP22 flows through a part of the first sub-radiator 221 , the second sub-radiator 222 . As the radio frequency transceiver module 29 is set to transmit or receive, the flow directions of the second first current CP21 and the second second current CP22 will change accordingly. Regardless of the direction in which the current flows, the intensity of the current will be inversely proportional to the distance between the feed points. Therefore, the current intensity of the second first current CP21 near the first feeding point 25 a is relatively strong, and the current intensity of the second second current CP22 near the second feeding point 25 b is relatively strong.
进一步比较图10A、10B可以看出,频率较低的第一共振信号对应的电流路径(第一第一电流CP11、第一第二电流CP12的流动路径),较频率较高的第二共振信号对应的电流路径(第二第一电流CP21、第二第二电流CP22的流动路径)长。10A and 10B, it can be seen that the current path corresponding to the first resonance signal with a lower frequency (the flow path of the first first current CP11 and the first second current CP12) is smaller than that of the second resonance signal with a higher frequency. The corresponding current paths (the flow paths of the second first current CP21 and the second second current CP22 ) are long.
根据本发明的构想,第二共振频率约为第一共振频率的两倍或以上。举例而言,本发明的双频耦极天线可应用于第一共振频率为800/900MHz,而第二共振频率为1800MHz的情形。或者,本发明的双频耦极天线可应用于第一共振频率为2400~2500MHz,而第二共振频率为5150~5850MHz的情形。According to the idea of the present invention, the second resonance frequency is about twice or more than the first resonance frequency. For example, the dual-frequency dipole antenna of the present invention can be applied to the situation where the first resonant frequency is 800/900 MHz and the second resonant frequency is 1800 MHz. Alternatively, the dual-frequency dipole antenna of the present invention can be applied to the situation where the first resonant frequency is 2400-2500 MHz, and the second resonant frequency is 5150-5850 MHz.
为了因应便携式电子装置的轻薄短小的特性,双频耦极天线可内建于便携式电子装置的系统电路板的一角。或者,用于设置天线的基板可为另一个尺寸相对较小的印刷式电路板,并独立地设置在电子装置的壳体内璧,并搭配同轴电缆或是钮扣式的RF连接器使用。本发明的双频耦极天线可依产品的需求轻易的调整与修正达到系统所需求的操作频段,并可适用于诸多无线通信装置。In order to cope with the thin, light and small features of the portable electronic device, the dual-band dipole antenna can be built into a corner of the system circuit board of the portable electronic device. Alternatively, the substrate used for disposing the antenna can be another printed circuit board with a relatively small size, which is independently disposed on the inner wall of the housing of the electronic device, and used together with a coaxial cable or a button-type RF connector. The dual-frequency dipole antenna of the present invention can be easily adjusted and corrected to meet the operating frequency band required by the system according to product requirements, and is applicable to many wireless communication devices.
综上所述,虽然本发明已以优选实施例公开如上,然其并非用以限定本发明。本发明所属领域技术人员,在不脱离本发明的精神和范围内,当可作各种的更动与润饰。因此,本发明的保护范围当视所附权利要求书界定范围为准。In summary, although the present invention has been disclosed as above with preferred embodiments, it is not intended to limit the present invention. Those skilled in the art to which the present invention belongs may make various changes and modifications without departing from the spirit and scope of the present invention. Therefore, the scope of protection of the present invention should be determined by the appended claims.
Claims (13)
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