This application is a U.S. national stage application of the PCT international application No. PCT/JP2017/034612 filed on Sep. 26, 2017, which claims the benefit of foreign priority of Japanese patent application No. 2016-196910 filed on Oct. 5, 2016, the contents all of which are incorporated herein by reference.
The present invention relates to a common mode noise filter for use in various electronic equipment, such as digital devices, audiovisual (AV) devices, and information communication terminals.
As a digital data transmission standard for connecting a main IC to a display or a camera in a mobile computing device, a mipi (Mobile Industry Processor Interface) D-PHY standard has been adopted. In this standard, a system that transmits differential signals by using two transmission lines is used. In recent years, the resolution of cameras has been dramatically increased, and accordingly a higher-speed transmission system, that is, a system in which different voltages are transmitted to respective transmission lines from a transmitter by using three transmission lines, and the differences between the lines are obtained by a receiver to perform differential output has been put in practical use as a mipi C-PHY standard.
A conventional common mode noise filter similar to conventional common mode noise filter 501 is disclosed in, for example, PTL 1.
PTL 1: Japanese Patent Laid-Open Publication No. 2003-77727
A common mode noise filter includes a non-magnetic body and first to third coil conductors provided inside the non-magnetic body. The second coil conductor is provided in a downward direction from the first coil conductor. The third coil conductor is provided in the downward direction from the second coil conductor. The first and third coil conductors are arranged deviate in a direction perpendicular to the downward direction with respect to the second coil conductor. At least one of the first and third coil conductor overlaps the second coil conductor viewing in the direction perpendicular to the downward direction.
In another common mode noise filter, the first, second, and third coil conductors do not overlap each other viewing in the direction perpendicular to the downward direction. An upper surface of the second coil conductor is flush with a lower surface of the first coil conductor. A lower surface of the second coil conductor is flush with an upper surface of the third coil conductor.
These common mode noise filters allow these coil conductors to be magnetically coupled to each other with a good balance, thereby preventing degradation of differential signals.
Common mode noise filter 1001 includes non-magnetic body 14 and coil conductors 11a, 11b, 12a, 12b, 13a, and 13b provided inside non-magnetic body 14. Coil conductors 11a and 11b are electrically connected to each other to constitute coil 11. Coil conductors 12a and 12b are electrically connected to each other to constitute coil 12. Coil conductors 13a and 13b are electrically connected to each other to constitute coil 13. In accordance with Embodiment 1, coil conductors 11a and 11b are electrically connected in series to each other through via-conductor 16a to constitute coil 11. Coil conductors 12a and 12b are electrically connected in series to each other through via-conductor 16b to constitute coil 12. Coil conductors 13a and 13b are electrically connected in series to each other through via-conductor 16c to constitute coil 13. Coils 11, 12, and 13 are independent from each other.
Non-magnetic body 14 includes plural non-magnetic layers staked on one another. Coil conductors 11a to 13a and 11b to 13b are provided by spirally plating or printing the respective non-magnetic layers with conductive material, such as silver.
As illustrated in
Coil conductor 11a constituting coil 11, coil conductor 12a constituting coil 12, coil conductor 13a constituting coil 13, coil conductor 11b constituting coil 11, coil conductor 12b constituting coil 12, and coil conductor 13b constituting coil 13 are disposed in this order from above to constitute laminated body 15. In other words, coil conductor 12a is provided in downward direction D10 from coil conductor 11a. Coil conductor 13a is provided in downward direction D10 from coil conductor 12a. Coil conductor 11b is provided in downward direction D10 from coil conductor 13a. Coil conductor 12b is provided in downward direction D10 from coil conductor 11b. Coil conductor 13b is provided in downward direction D10 from coil conductor 12b.
In downward direction D10, between two coil conductors constituting one of the three coils, one of two coil conductors constituting one of the other two coils and one of two coil conductors constituting another of the other two coils are located. In other words, in downward direction D10, coil conductor 12a constituting coil 12 and coil conductor 13a constituting coil 13 are located between coil conductors 11a and 11b constituting coil 11. In downward direction D10, coil conductor 11b constituting coil 11 and coil conductor 13b constituting coil 13 are located between coil conductors 12a and 12b constituting coil 12. In downward direction D10, coil conductor 11b constituting coil 11 and coil conductor 12b constituting coil 12 are located between coil conductors 13a and 13b constituting coil 13.
Coil 11 is magnetically coupled to coil 12. Coil 12 is magnetically coupled to coil 13. Coil 11 is magnetically coupled to coil 13.
In common mode noise filter 1001, coil conductors 11a and 13a and coil conductors 11b and 13b deviate in direction D11 perpendicular to downward direction D10 with respect to coil conductors 12a and 12b viewing from above. In other words, coil conductors 11a and 13a constituting coils 11 and 13 deviate in direction D11 with respect to coil conductor 12a constituting coil 12 viewing from above. Coil conductors 11b and 13b constituting coils 11 and 13 deviate in direction D11 with respect to coil conductor 12b constituting coil 12 viewing from above.
Coil conductors 11a to 13a and 11b to 13b have spiral shapes wound about coil axis C11. The state in which spirally wound coil conductors 11a, 13a, 11b, and 13b deviate in direction D11 with respect to coil conductors 12a and 12b means that, in any cross-section of laminated body 15 parallel with downward direction D10, portions of coil conductors 11a, 13a, 11b, and 13b at a certain number of turn counted from respective inner circumferences 111a, 113a, 111b, and 113b toward respective outer circumferences 211a, 213a, 211b, and 213b deviate in downward direction D11 with respect to portions of coil conductors 12a and 12b at the certain number of turn counted from respective inner circumferences 112a and 112b toward respective outer circumferences 212a and 212b viewing from above. Specifically, in any cross-section of laminated body 15 parallel with downward direction D10, a portion of coil conductor 12a at a certain number of turn counted from inner circumference 112a toward outer circumference 212a deviates toward coil axis C11 in direction D11 with respect to a cross-section at portions of coil conductors 11a and 13a at the certain number of turn counted from respective inner circumferences 111a and 113a toward respective outer circumferences 211a and 213a viewing from above. In any cross-section of laminated body 15 parallel with downward direction D10, portions of coil conductor 11b and 13b at a certain number of turn counted from respective inner circumferences 111b and 113b toward respective outer circumferences 211b and 213b deviate toward coil axis C11 in direction D11 with respect to a portion of coil conductor 12b at the certain number of turn counted from inner circumference 112b toward outer circumference 212b viewing from above.
Coil conductors 11a and 13a are disposed substantially at the same position viewing from above to face each other in downward direction D10. Coil conductors 11b and 13b are disposed substantially at the same position viewing from above to face each other. A portion of coil conductor 11a having the spiral shape constituting coil 11 overlaps a portion of coil conductor 13a having the spiral shape constituting coil 13 viewing from above. A portion of coil conductor 11b having the spiral shape constituting coil 11 overlaps a portion of coil conductor 13b having the spiral shape constituting coil 13 viewing from above.
In common mode noise filter 1001 illustrated in
In common mode noise filter 1001, the same number of coil conductors are located at the same position viewing from above. This configuration allows stresses applied at the time of lamination to be preferably uniform. The locations of coil conductors 11b and 13b viewing from above may be replaced with the location of coil conductor 12b viewing from above.
A part of coil conductor 11a constituting coil 11 and a part of coil conductor 13a constituting coil 13 overlap coil conductor 12a constituting coil 12 viewing from direction D11. Apart of coil conductor 11b constituting coil 11 and a part of coil conductor 13b constituting coil 13 overlap coil conductor 12b constituting coil 12 viewing from direction D11. In other words, coil conductor 11a constituting coil 11 and coil conductor 13a constituting coil 13 partially overlap coil conductor 12a constituting coil 12 viewing from direction D11. In addition, coil conductor 11b constituting coil 11 and coil conductor 13b constituting coil 13 partially overlap coil conductor 12b constituting coil 12 viewing from direction D11.
Non-magnetic body 14 has coil conductors 11a, 11b, 12a, 12b, 13a, and 13b built therein and includes plural non-magnetic layers stacked on one another. These non-magnetic layers are made of non-magnetic material, such as Cu—Zn ferrite or glass ceramics, having sheet shapes.
Coil conductors 11a, 11b, 12a, 12b, 13a, and 13b are formed by, for example, vapor-depositing on, plating, or printing the non-magnetic layers with conductive material, such as metal.
Magnetic bodies 17a and 17b made of magnetic material, such as Ni—Cu—Zn ferrite, are provided above and below non-magnetic body 14, respectively. Common mode noise filter 1001 does not necessarily include magnetic bodies 17a and 17b. Each of magnetic bodies 17a and 17b may include plural non-magnetic layers and plural magnetic layers that are alternately stacked.
Laminated body 18 has the above-described configuration. Six outer electrodes connected to respective ends of coil conductors 11a, 11b, 12a, 12b, 13a, and 13b are provided on both end surfaces of laminated body 18.
As described above, in common mode noise filter 1001 according to Embodiment 1, a part of coil 11 is adjacent to a part of coil 12 viewing from direction D11. Apart of coil 12 is adjacent to a part of coil 13 viewing from direction D11. Coil 11 is adjacent to coil 13 in downward direction D10 (up-and-down direction). Therefore, coils 11, 12, and 13 are magnetically coupled to each other with a preferable balance. In other words, coils 11 and 12 are magnetically coupled to each other, coils 12 and 13 are magnetically coupled to each other at the same level of strength as that of magnetic coupling between coils 11 and 12. Coils 11 and 13 are magnetically coupled to each other at the same level of strength as that of magnetic coupling between coils 11 and 12 and that of magnetic coupling between coils 12 and 13. This configuration prevents degradation of differentials signal input to coils 11 to 13.
A part of coil 11 and a part of coil 13 overlap coil 12 viewing from direction D11. This configuration reduces the height of common mode noise filter 1001.
In common mode noise filter 1001 according to Embodiment 1, each coil includes two coil conductors that are electrically connected to each other. In the common mode noise filter according to Embodiment 1, even in the case where each coil includes three or more coil conductors that are electrically connected to each other, the same effect is achieved. Alternatively, even in the case where each coil includes a single coil conductor, the same effect is achieved.
Distance La between portion 411a of coil conductor 11a and portion 413a of coil conductor 13a, distance Lb between portion 411a of coil conductor 11a and portion 412a of coil conductor 12a, and distance Lc between portion 412a of coil conductor 12a and portion 413a of coil conductor 13a are substantially identical to one another. Each of portions 411a, 412a, and 413a of coil conductors 11a, 12a, and 13a constitutes corresponding one of the apexes of a regular triangle. Each of portions 311a, 312a, and 313a of coil conductors 11a, 12a, and 13a constitutes a corresponding one of the apexes of a regular triangle.
In other words, line PLa that connects coil conductor 11a and coil conductor 13a, line PLb that connects coil conductor 11a and coil conductor 12a, and line PLc that connects coil conductor 12a and coil conductor 13a form a regular triangle.
The distances between any two of coils 11, 12, and 13 are substantially identical to each other. Then, the balance of magnetic coupling can be further improved.
Distance Ld between portion 412a of coil conductor 12a at the N-th turn and portion 311a of coil conductor 11a at the (N−1)-th turn, and distance Le between portion 412a of coil conductor 12a at the N-th turn and portion 313a of coil conductor 13a at the (N−1)-th turn are substantially identical to distances La, Lb, and Lc.
A method for manufacturing coil conductors 11a, 12a, and 13a of common mode noise filter 1001 according to Embodiment 1 will be described below with reference to
First, portion 13a1 of coil conductor 13a is formed on the upper surface of non-magnetic layer 14a.
Next, non-magnetic layer 14b is formed around portion 13a1 of coil conductor 13a on the upper surface of non-magnetic layer 14a.
Next, portion 13a2 of coil conductor 13a is formed on the upper surface of portion 13a1 of coil conductor 13a. Portion 12a1 of coil conductor 12a is formed on the upper surface of non-magnetic layer 14b. Then, non-magnetic layer 14c is formed around portions 12a1 and 13a2 of respective coil conductors 12a and 13a on the upper surface of non-magnetic layer 14b.
Next, portion 12a2 of coil conductor 12a is formed on the upper surface of portion 12a1 of coil conductor 12a. Then, non-magnetic layer 14d is formed around portion 12a2 of coil conductor 12a on the upper surface of non-magnetic layer 14c.
Next, remaining portion 12a3 of coil conductor 12a is formed on the upper surface of portion 12a2 of coil conductor 12a, and portion 11a1 of coil conductor 11a is formed on the upper surface of non-magnetic layer 14d. Then, non-magnetic layer 14e is formed around portions 11a1 and 12a3 of respective coil conductors 11a and 12a on the upper surface of non-magnetic layer 14d.
Next, remaining portion 11a2 of coil conductor 11a is formed on the upper surface of portion 11a1 of coil conductor 11a. Then, non-magnetic layer 14f is formed around portion 11a2 of coil conductor 11a on the upper surface of non-magnetic layer 14e.
Coil conductors 11b, 12b, and 13b are formed similarly to coil conductors 11a, 12a, and 13a.
Coil conductors 11a, 11b, 12a, 12b, 13a, and 13b may be formed by any one of sputtering (thin film sputtering), plating (transfer plating), and printing, or a combination thereof.
In conventional common mode noise filter 501 illustrated in
In the case that common mode noise filter 501 is applied to a three-wire differential signal line, when differential data signals are transmitted with the signal line, magnetic fluxes generated in coils 2 and 4 that are not magnetically coupled to each other produces a large residual inductance without canceling each other out. This configuration increases a loss in the differential data signals and significant degradation in differential signal quality
However, in the comparative example of common mode noise filter 502, coils 2 and 4 sandwich coil 3, and are accordingly more distant from each other. Thus, magnetic coupling between coils 2 and 4 is weaker than magnetic coupling between coils 2 and 3 and magnetic coupling between coils 3 and 4. Therefore, coils 2, 3, and 4 are magnetically coupled to each other with a poor balance. When differential signals are input to common mode noise filter 502 illustrated in
As described above, common mode noise filter 1001 according to Embodiment 1 prevents degradation of differential signals input to coils 11 to 13.
Coil axis C12 of coil conductors 11b, 12a, and 13b deviates in longitudinal direction D1 with respect to coil axis C11 of coil conductors 11a, 12b, and 13a, but may not deviate in lateral direction D2 with respect to coil axis C11, providing same effect.
In common mode noise filter 1001 illustrated in
In common mode noise filter 1006 according to Embodiment 2 illustrated in
Similarly to common mode noise filter 1001 according to Embodiment 1, in common mode noise filter 1006, distances La, Lb, and Lc are substantially identical to one another. Each of portions 411a, 412a, and 413a of coil conductors 11a, 12a, and 13a constitutes a corresponding one of the apexes of a regular triangle. Each of portions 311a, 312a, and 313a of coil conductors 11a, 12a, and 13a constitutes a corresponding one of the apexes of a regular triangle.
In common mode noise filter 1006, each coil conductor overlaps only one non-magnetic layer in direction D11, and hence, it is not necessary to form one coil conductor with plural processes. Therefore, common mode noise filter 1006 can be more easily manufactured than common mode noise filter 1001 according to Embodiment 1.
Viewing from direction D11, any other non-magnetic layer is not provided between the upper surface of coil conductor 12a and the lower surface of coil conductor 11a, and any other non-magnetic layer is not provided between the lower surface of coil conductor 12a and the upper surface of coil conductor 13a. This configuration allows coil conductors 11a to 13 to be strongly magnetically coupled to each other.
The size and arrangement of the coil conductors are adjusted so that any two of three coil conductor portions at the same number of turn are magnetically coupled at approximately the same strength level.
In common mode noise filter 1006, coil conductors 11a to 13a may be disposed similarly to common mode noise filter 1004 according to Embodiment 1 illustrated in
The above-described enlarged cross-sectional views shown in
In Embodiments, terms, such as “upper surface”, “lower surface”, “downward”, and “viewing from above”, indicating directions indicate relative directions depending only on the relative positional relationship between components, such as coil conductors, of a common mode noise filter, and do not indicate absolute directions, such as a vertical direction.
Number | Date | Country | Kind |
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JP2016-196910 | Oct 2016 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2017/034612 | 9/26/2017 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2018/066405 | 4/12/2018 | WO | A |
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Number | Date | Country |
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2003-077727 | Mar 2003 | JP |
2016-157917 | Sep 2016 | JP |
Entry |
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International Search Report of PCT application No. PCT/JP2017/034612 dated Jan. 9, 2018. |
English Translation of Chinese Search Report dated Sep. 30, 2020 for the related Chinese Patent Application No. 201780004371.9. |
Number | Date | Country | |
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20180336987 A1 | Nov 2018 | US |