Patent Application
20200303117
The present invention relates to a multilayer coil component.
Known multilayer coil components include an element body and a plurality of coil conductors (see, for example, Japanese Unexamined Patent Publication No. 2017-076700). The element body includes a plurality of metal magnetic particles and resin existing between the plurality of metal magnetic particles. The plurality of coil conductors is disposed in the element body, the plurality of coil conductors being separated from each other in a predetermined direction and electrically connected to each other.
An object of one aspect of the present invention is to provide a multilayer coil component that controls a decrease in inductance and a decrease in insulation between coil conductors.
A multilayer coil component according to one aspect of the present invention includes an element body and a plurality of coil conductors. The element body includes a plurality of metal magnetic particles and resin existing between the plurality of metal magnetic particles. The plurality of coil conductors is disposed in the element body, the plurality of coil conductors being separated from each other in a predetermined direction and electrically connected to each other. The plurality of metal magnetic particles included in the element body includes a plurality of metal magnetic particles having a particle size equal to or greater than one third of a distance between the coil conductors adjacent to each other in the predetermined direction and equal to or less than a half of the distance. Between the coil conductors adjacent to each other in the predetermined direction, the metal magnetic particles having the particle size are distributed along the predetermined direction.
Metal magnetic particles having a particle size equal to or greater than one third of a distance between coil conductors adjacent to each other in a predetermined direction are higher in magnetic permeability than metal magnetic particles having a particle size less than one third of the distance between the coil conductors adjacent to each other in the predetermined direction. Hereinafter, the distance between the coil conductors adjacent to each other in the predetermined direction is referred to as “coil conductor-to-coil conductor distance”. In the one aspect, since the plurality of metal magnetic particles having the particle size equal to or greater than one third of the coil conductor-to-coil conductor distance is distributed along the predetermined direction between the coil conductor, a decrease in magnetic permeability is controlled.
Metal magnetic particles having a particle size greater than a half of the coil conductor-to-coil conductor distance are higher in magnetic permeability than metal magnetic particles having a particle size equal to or less than a half of the coil conductor-to-coil conductor distance. However, when the metal magnetic particles having a particle size greater than a half of the coil conductor-to-coil conductor distance are distributed along the predetermined direction between the coil conductors, in the process of manufacturing the multilayer coil component, lamination misalignment between the coil conductors tends to occur. The occurrence of lamination misalignment between the coil conductors may decrease a cross-sectional area of a magnetic path located inside a coil and in turn decrease inductance. In the one aspect, since a plurality of metal magnetic particles having the particle size equal to or greater than a half of the coil conductor-to-coil conductor distance is distributed along the predetermined direction between the coil conductor, lamination misalignment between the coil conductors tends not to occur.
Consequently, the one aspect controls a decrease in inductance.
In a case in which the number of metal magnetic particles distributed along the predetermined direction between the coil conductors is small, insulation between the coil conductors may decrease. The number of metal magnetic particles that have a particle size equal to or less than a half of the coil conductor-to-coil conductor distance and are distributed between the coil conductors tends to be larger than the number of metal magnetic particles that have a particle size greater than a half the coil conductor-to-coil conductor distance and are distributed between the coil conductors. Therefore, in the one aspect, the insulation between the coil conductors tends not to decrease.
The number of metal magnetic particles that have a particle size less than one third of the coil conductor-to-coil conductor distance and are distributed between the coil conductors tends to be larger than the number of metal magnetic particles that have a particle size equal to or greater than one third of the coil conductor-to-coil conductor distance and are distributed between the coil conductors. However, in a case in which the metal magnetic particles having a particle size less than one third of the coil conductor-to-coil conductor distance are distributed between the coil conductors, gaps formed between the metal magnetic particles are small as compared with in a case in which the metal magnetic particles having a particle size equal to or greater than one third of the coil conductor-to-coil conductor distance are distributed between the coil conductors. Therefore, the resin tends not to exist between the metal magnetic particles, and the insulation between the coil conductors may decrease. In the one aspect, since the plurality of metal magnetic particles having the particle size equal to or greater than one third of the coil conductor-to-coil conductor distance is distributed along the predetermined direction between the coil conductors, the resin tends to exist between the metal magnetic particles, and the insulation between the coil conductors tends not to decrease.
Consequently, the one aspect controls the decrease in the insulation between the coil conductors.
In the one aspect, in a cross-section taken along the predetermined direction, an area of a region where the metal magnetic particles having the particle size are distributed along the predetermined direction may be greater than 50% of an area of a region between the coil conductors adjacent to each other in the predetermined direction. This configuration further controls the decrease in the insulation between the coil conductors.
In the one aspect, the plurality of coil conductors may include a pair of side surfaces opposing each other in the predetermined direction. Surface roughness of the pair of side surfaces may be less than 40% of an average particle size of the plurality of metal magnetic particles included in the element body.
Q characteristics of the multilayer coil component depend on a resistance of the coil conductors. In a high-frequency range, a current (signal) tends to flow near surfaces of the coil conductors due to the skin effect. Therefore, as the resistance at and near the surfaces of the coil conductors increases, the Q characteristics of the multilayer coil component decreases. Hereinafter, the resistance component at and near the surfaces of the coil conductors is referred to as “surface resistance”. A configuration in which the surfaces of the coil conductors have irregularities substantially increases a length of current flow, and thus increases the surface resistance, as compared with a configuration in which the surfaces of the coil conductors have no irregularities.
A configuration in which the surface roughness of the pair of side surfaces opposing each other in the predetermined direction is less than 40% of the average particle size of the plurality of metal magnetic particles controls an increase in surface resistance and controls a decrease in Q characteristics in a high-frequency range, as compared with a configuration in which the surface roughness of the pair of side surfaces is equal to or larger than 40% of the average particle size of the plurality of metal magnetic particles. Therefore, the configuration in which the surface roughness of the pair of side surfaces is less than 40% of the average particle size of the plurality of metal magnetic particles controls the increase in the surface resistance and controls the decrease in the Q characteristics in the high-frequency range.
In the one aspect, the plurality of coil conductors may be plating conductors.
In a case in which the coil conductors are sintered metal conductors, the coil conductors are each formed by sintering a metal component (metal powder) contained in a conductive paste. In this case, the metal magnetic particles bite into the conductive paste before the metal component is sintered. Irregularities due to the shape of the metal magnetic particles are formed on a surface of the conductive paste. The formed coil conductors are deformed so that the metal magnetic particles bite into the coil conductors. Therefore, a configuration in which the coil conductors are the sintered metal conductors significantly increases the surface roughness of the coil conductors.
In a case in which the coil conductors are the plating conductors, the metal magnetic particles tend not to bite into the coil conductors. In this case, deformation of the coil conductors is reduced. Therefore, the configuration in which the coil conductors are the plating conductors controls an increase in the surface roughness of the coil conductors and controls an increase in the surface resistance.
The present invention will become more fully understood from the detailed description given hereinafter and the accompanying drawings which are given by way of illustration only, and thus are not to be considered as limiting the present invention.
Further scope of applicability of the present invention will become apparent from the detailed description given hereinafter. However, it should be understood that the detailed description and specific examples, while indicating embodiments of the invention, are given by way of illustration only, since various changes and modifications within the spirit and scope of the invention will become apparent to those skilled in the art from this detailed description.
Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings. In the following description, the same elements or elements having the same functions are denoted with the same reference numerals and overlapped explanation is omitted.
A configuration of a multilayer coil component 1 according to an embodiment will be described with reference to
As illustrated in
The element body 2 has a rectangular parallelepiped shape. The rectangular parallelepiped shape includes a rectangular parallelepiped shape in which corners and ridges are chamfered, and a rectangular parallelepiped shape in which the corners and ridges are rounded. The element body 2 includes a pair of end surfaces 2a, 2b opposing each other and includes four side surfaces 2c, 2d, 2e, 2f. The four side surfaces 2c, 2d, 2e, 2f extend in a direction in which the pair of end surfaces 2a, 2b opposes each other to connect to the pair of end surfaces 2a, 2b.
The end surfaces 2a and the end surface 2b oppose each other in a first direction D1. The side surface 2c and the side surface 2d oppose each other in a second direction D2. The side surface 2e and the side surface 2f oppose each other in a third direction D3. The first direction D1, the second direction D2, and the third direction D3 are approximately orthogonal to each other. The side surface 2d includes a surface that opposes an electronic device (not illustrated) when the multilayer coil component 1 is mounted on the electronic device, for example. Examples of the electronic device include a circuit board and an electronic component. In the present embodiment, the side surface 2d is arranged to constitute a mounting surface. The side surface 2d includes the mounting surface.
The element body 2 is configured by laminating a plurality of magnetic layers 7. The magnetic layers 7 are laminated in the third direction D3. The element body 2 includes the plurality of laminated magnetic layers 7. In an actual element body 2, the plurality of magnetic layers 7 is integrated in such a way that boundaries between the magnetic layers cannot be visually recognized.
Each of the magnetic layers 7 includes a plurality of metal magnetic particles. The metal magnetic particles are made of, for example, a soft magnetic alloy. The soft magnetic alloy is, for example, an Fe—Si alloy. In a case in which the soft magnetic alloy is an Fe—Si alloy, the soft magnetic alloy may contain P. The soft magnetic alloy may be, for example, an Fe—Ni—Si-M alloy. “M” includes at least one element selected from Co, Cr, Mn, P, Ti, Zr, Hf, Nb, Ta, Mo, Mg, Ca, Sr, Ba, Zn, B, Al, and rare earth elements. In the magnetic layers 7, the metal magnetic particles are bonded to each other. The metal magnetic particles are bonded to each other through, for example, bonding of oxide films formed on surfaces of the metal magnetic particles. The element body 2 includes resin. The resin exists between the plurality of metal magnetic particles. The resin is a resin having an electrical insulation, that is, insulating resin. Examples of the insulating resin include a silicone resin, a phenol resin, an acrylic resin, and an epoxy resin.
An average particle size of the metal magnetic particles is in a range of from 0.5 μm to 15 μm. In the present embodiment, the average particle size of the metal magnetic particles is 5 μm. In the present embodiment, the “average particle size” corresponds to a particle size at an integrated value of 50% in a particle size distribution obtained by a laser diffraction/scattering method.
The external electrode 4 is disposed on the end surface 2a of the element body 2, and the external electrode 5 is disposed on the end surface 2b of the element body 2. The external electrode 4 and the external electrode 5 are separated from each other in the first direction D1. The external electrodes 4, 5 have an approximately rectangular shape in plan view, and corners of the external electrodes 4, 5 are rounded. The external electrodes 4, 5 include an electrically-conductive material. The electrically-conductive material is, for example, Ag or Pd. The external electrodes 4, 5 are each configured as a sintered body of a conductive paste. The conductive paste contains a conductive metal powder and glass frit. The conductive metal powder is, for example, an Ag powder or a Pd powder. On surfaces of the external electrodes 4, 5, plating layers are formed. The plating layers are formed by, for example, electroplating. The electroplating is, for example, Ni electroplating or Sn electroplating.
The external electrode 4 includes five electrode portions. The external electrode 4 includes an electrode portion 4a located on the end surface 2a, an electrode portion 4b located on the side surface 2d, an electrode portion 4c located on the side surface 2c, an electrode portion 4d located on the side surface 2e, and an electrode portion 4e located on the side surface 2f. The electrode portion 4a covers a whole of the end surface 2a. The electrode portion 4b covers a part of the side surface 2d. The electrode portion 4c covers a part of the side surface 2c. The electrode portion 4d covers a part of the side surface 2e. The electrode portion 4e covers a part of the side surface 2f. The five electrode portions 4a, 4b, 4c, 4d, 4e are formed integrally.
The external electrode 5 includes five electrode portions. The external electrode 5 includes an electrode portion 5a located on the end surface 2b, an electrode portion 5b located on the side surface 2d, an electrode portion 5c located on the side surface 2c, an electrode portion 5d located on the side surface 2e, and an electrode portion 5e located on the side surface 2f. The electrode portion 5a covers a whole of the end surface 2b. The electrode portion 5b covers a part of the side surface 2d. The electrode portion 5c covers a part of the side surface 2c. The electrode portion 5d covers a part of the side surface 2e. The electrode portion 5e covers a part of the side surface 2f. The five electrode portions 5a, 5b, 5c, 5d, 5e are integrally formed.
The multilayer coil component 1 includes a coil 20 and a pair of connection conductors 13, 14. The coil 20 is disposed in the element body 2. The coil 20 includes a plurality of coil conductors CC. In the present embodiment, the plurality of coil conductors CC includes six coil conductors 21 to 26. The coil 20 includes a through-hole conductor 17. The pair of connection conductors 13, 14 is also disposed in the element body 2.
The coil conductors CC (coil conductors 21 to 26) are disposed in the element body 2. The coil conductors 21 to 26 are separated from each other in the third direction D3. Distances Dc between the coil conductors 21 to 26 adjacent to each other in the third direction D3 are equivalent to each other. The distances Dc may be different from each other. A coil axis of the coil 20 extends along the third direction D3. A thickness of the coil conductors 21 to 26 is, for example, about 40 μm. A width of the coil conductors 21 to 26 is, for example, about 150 μm.
The distances Dc are, for example, in a range of from 5 μm to 30 μm. In the present embodiment, the distances Dc are 15 μm. A surface of each of the coil conductors CC (each of the coil conductors 21 to 26) has roughness as described later, and thus, the distances Dc vary in response to a surface shape of each of the coil conductors CC. Therefore, the distances Dc are obtained, for example, as follows.
A cross-sectional photograph of the multilayer coil component 1 including each of the coil conductors CC (each of the coil conductors 21 to 26) is acquired. The cross-sectional photograph is obtained, for example, by capturing a cross-section of the multilayer coil component 1 when cut along a plane that is parallel to the pair of end surfaces 2a, 2b and is separated from the end surface 2a by a predetermined distance. The plane may be located equidistant from the pair of end surfaces 2a, 2b. The cross-sectional photograph may be obtained by capturing a cross-section of the multilayer coil component 1 when cut along a plane that is parallel to the pair of side surfaces 2e, 2f and is separated from the side surface 2e by a predetermined distance.
A distance between the coil conductors CC adjacent to each other in the third direction D3 on the acquired cross-sectional photograph is measured at a plurality of given positions. The number of measurement positions is, for example, “50”. An average of the measured distances is calculated. The calculated average value is the distance Dc.
One end and another end of each of the coil conductors 21, 23, 25, 26 are separated from each other in the third direction D3. One end and another end of each of the coil conductors 22, 24 are separated from each other in the second direction D2. Each of the coil conductors 21 to 26 adjacent to each other in the third direction D3 includes a first conductor portion and a second conductor portion. The first conductor portions overlap each other when viewed from the third direction D3. The second conductor portions do not overlap each other when viewed from the third direction D3.
The through-hole conductor 17 is located between ends of the coil conductors 21 to 26 adjacent to each other in the third direction D3. The through-hole conductor 17 connects the ends of the coil conductors 21 to 26 adjacent to each other in the third direction D3. The plurality of coil conductors 21 to 26 is electrically connected to each other through the through-hole conductor 17. An end of the coil conductor 21 constitutes one end of the coil 20. An end of the coil conductor 26 constitutes another end of the coil 20. An axis direction of the coil 20 extends along the third direction D3.
The connection conductor 13 is connected to the coil conductor 21. The connection conductor 13 is contiguous with the coil conductor 21. The connection conductor 13 is formed integrally with the coil conductor 21. The connection conductor 13 couples an end 21a of the coil conductor 21 and the external electrode 4 and is exposed at the end surface 2a of the element body 2. The connection conductor 13 is connected to the electrode portion 4a of the external electrode 4. The connection conductor 13 electrically connects the one end of the coil 20 and the external electrode 4.
The connection conductor 14 is connected to the coil conductor 26. The connection conductor 14 is contiguous with the coil conductor 26. The connection conductor 14 is formed integrally with the coil conductor 26. The connection conductor 14 couples an end 26b of the coil conductor 26 and the external electrode 5 and is exposed at the end surface 2b of the element body 2. The connection conductor 14 is connected to the electrode portion 5a of the external electrode 5. The connection conductor 14 electrically connects the other end of the coil 20 and the external electrode 5.
The coil conductors CC (coil conductors 21 to 26) and the connection conductors 13, 14 are plating conductors. The coil conductors CC and the connection conductors 13, 14 include an electrically-conductive material. The electrically-conductive material is, for example, Ag, Pd, Cu, Al, or Ni. The through-hole conductor 17 includes an electrically-conductive material. The an electrically-conductive material is, for example, Ag, Pd, Cu, Al, or Ni. The through-hole conductor 17 is constituted as a sintered body of a conductive paste. The conductive paste contains a conductive metal powder. The conductive metal powder is, for example, an Ag powder, a Pd powder, a Cu powder, an Al powder, or an Ni powder. The through-hole conductor 17 may be a plating conductor.
The plurality of metal magnetic particles included in the element body 2 includes a plurality of metal magnetic particles MM. The plurality of metal magnetic particles MM has a particle size equal to or greater than one third of the distance Dc and equal to or less a half of the distance Dc. In the present embodiment, the particle size of the metal magnetic particles MM is in a range of from 5.0 to 7.5 μm. As illustrated in
The state where the metal magnetic particles MM are distributed along the third direction D3 includes not only a state where the metal magnetic particles MM entirely overlap each other when viewed from the third direction D3, but also a state where the metal magnetic particles MM partially overlap each other when viewed from the third direction D3. The plurality of metal magnetic particles included in the element body 2 includes metal magnetic particles that are larger in particle size than the metal magnetic particles MM, and metal magnetic particles that are smaller in particle size than the metal magnetic particles MM. In the present embodiment, the particle size is defined by an equivalent circular diameter.
The equivalent circular diameter of the metal magnetic particles is obtained, for example, as follows.
A cross-sectional photograph of the multilayer coil component 1 including each of the coil conductors CC (each of the coil conductors 21 to 26) and the metal magnetic particles is acquired. As described above, the cross-sectional photograph is obtained, for example, by capturing the cross-section of the multilayer coil component 1 when cut along the plane that is parallel to the pair of end surfaces 2a, 2b and is separated from the end surface 2a by the predetermined distance. In this case, the plane may be located equidistant from the pair of end surfaces 2a, 2b. As described above, the cross-sectional photograph may be obtained by capturing the cross-section of the multilayer coil component 1 when cut along the plane that is parallel to the pair of side surfaces 2e, 2f and is separated from the side surface 2e by the predetermined distance. The cross-sectional photograph may be the cross-sectional photograph captured to obtain the distance Dc.
The acquired cross-sectional photograph is subjected to image processing by software. In this image processing, boundaries of the metal magnetic particles are determined, and an area of each of the metal magnetic particles is calculated. From the calculated area of each of the metal magnetic particles, the particle size converted to the equivalent circular diameter is calculated.
A region between the coil conductors CC adjacent to each other in the third direction D3 includes a region where the metal magnetic particles MM are distributed along the third direction D3. The region between the coil conductors CC adjacent to each other in the third direction D3 is a region in the element body 2 that is sandwiched between the coil conductors CC adjacent to each other in the third direction D3. For example, a region between the coil conductor 21 and the coil conductor 22 is a region in the element body 2 that is sandwiched between the coil conductor 21 and the coil conductor 22 and is placed to cover the whole of the coil conductor 21 and the whole of the coil conductor 22 when viewed from the third direction D3. In the cross-section taken along the third direction D3, an area of the region where the metal magnetic particles MM are distributed along the third direction D3 is greater than 50% of an area of the region between the coil conductors CC adjacent to each other in the third direction D3. In the region where the metal magnetic particles MM are distributed along the third direction D3, the metal magnetic particles MM may be in contact with each other, or the metal magnetic particles MM may not be in contact with each other. In the region between the coil conductors CC adjacent to each other in the third direction D3, the metal magnetic particles larger in particle size than the metal magnetic particles MM, and the metal magnetic particles smaller in particle size than the metal magnetic particles MM are also located.
The area of the region where the metal magnetic particles MM are distributed along the third direction D3 is obtained, for example, as follows.
A cross-sectional photograph of the multilayer coil component 1 including each of the coil conductors CC (each of the coil conductors 21 to 26) and the metal magnetic particles is acquired. As described above, the cross-sectional photograph is obtained, for example, by capturing the cross-section of the multilayer coil component 1 when cut along the plane that is parallel to the pair of end surfaces 2a, 2b and is separated from the end surface 2a by the predetermined distance. In this case, the plane may be located equidistant from the pair of end surfaces 2a, 2b. As described above, the cross-sectional photograph may be obtained by capturing the cross-section of the multilayer coil component 1 when cut along the plane that is parallel to the pair of side surfaces 2e, 2f and is separated from the side surface 2e by the predetermined distance. The cross-sectional photograph may be the cross-sectional photograph captured to obtain the distance Dc, or the cross-sectional photograph captured to obtain the equivalent circular diameter of the metal magnetic particles.
The acquired cross-sectional photograph is subjected to image processing by software. In this image processing, boundaries of the metal magnetic particles located in the region between the coil conductors CC adjacent to each other in the third direction D3 are determined, and an area of each of the metal magnetic particles is calculated. From the calculated area of each of the metal magnetic particles, the particle size converted to the equivalent circular diameter is calculated. Among the metal magnetic particles located in the region between the coil conductors CC adjacent to each other in the third direction D3, the metal magnetic particles MM are identified. As described above, the metal magnetic particles MM have the particle size equal to or greater than one third of the distance Dc and equal to or less than a half of the distance Dc.
As shown in
The area of the region between the coil conductors CC adjacent to each other in the third direction D3 is obtained, for example, as follows.
The cross-sectional photograph acquired to obtain the area of the region where the metal magnetic particles MM are distributed along the third direction D3 is subjected to image processing by software. In this image processing, boundaries of the coil conductors CC are determined, and an area of a region sandwiched between the pair of coil conductors CC opposing each other in the third direction D3 is calculated.
Each of the coil conductors CC (each of the coil conductors 21 to 26) includes a pair of side surfaces SF1, as illustrated in
Surface roughness of each of the side surfaces SF1 is less than 40% of an average particle size of metal magnetic particles. In the present embodiment, the surface roughness of each of the side surfaces SF1 is less than 2 μm. The surface roughness of each of the side surfaces SF1 is, for example, in a range of from 1.0 μm to 1.8 μm. In this case, the surface roughness of each of the side surfaces SF1 is in a range of from 20% to 36% of the average particle size of the metal magnetic particles. The surface roughness of each of the side surfaces SF1 may be approximately 0 μm. As illustrating in
The surface roughness of each of the side surfaces SF1 of the coil conductors CC is obtained, for example, as follows.
A cross-sectional photograph of the multilayer coil component 1 including each of the coil conductors CC (each of the coil conductors 21 to 26) is acquired. As described above, the cross-sectional photograph is obtained, for example, by capturing the cross-section of the multilayer coil component 1 when cut along the plane that is parallel to the pair of end surfaces 2a, 2b and is separated from the end surface 2a by the predetermined distance. In this case, the plane may be located equidistant from the pair of end surfaces 2a, 2b. As described above, the cross-sectional photograph may be obtained by capturing the cross-section of the multilayer coil component 1 when cut along the plane that is parallel to the pair of side surfaces 2e, 2f and that is separated from the side surface 2e by the predetermined distance. The cross-sectional photograph may be the cross-sectional photograph captured to obtain the distance Dc, the cross-sectional photograph captured to obtain the equivalent circular diameter of the metal magnetic particles, or the cross-sectional photograph captured to obtain the area of the region where the metal magnetic particles MM are distributed along the third direction D3.
A curve corresponding to each of the side surfaces SF1 on the acquired cross-sectional photograph is represented by a roughness profile. A portion of the side surface SF1 (roughness profile) on the cross-sectional photograph is sampled only by a sampling length, and a peak line at the highest peak in the sampled portion is obtained. The sampling length is, for example, 100 μm. The peak line is orthogonal to the third direction D3 and serves as a reference line. The sampled portion is equally divided into a predetermined number of sections. The predetermined number is, for example, “10”. A valley line at the lowest bottom is obtained for each of the equally divided sections. The valley line is also orthogonal to the third direction D3. A distance between the peak line and the valley line in the third direction D3 is measured for each of the equally divided sections. An average of the measured distances is calculated. The calculated average is the surface roughness. The surface roughness is obtained for each of the side surfaces SF1 by the above-described procedure.
A plurality of cross-sectional photographs is acquired at different positions, and the surface roughness may be obtained for each of the cross-sectional photographs. In this case, the average value of the plurality of degrees of obtained surface roughness may be the surface roughness.
The metal magnetic particles MM having the particle size equal to or greater than one third of the distance Dc are higher in magnetic permeability than the metal magnetic particles having a particle size less than one third of the distance Dc. In the multilayer coil component 1, since the plurality of metal magnetic particles MM having the particle size equal to or greater than one third of the distance Dc is distributed along the third direction D3 between the coil conductors CC (coil conductors 21 to 26), a decrease in magnetic permeability is controlled.
The metal magnetic particles having a particle size greater than a half of the distance Dc are higher in magnetic permeability than the metal magnetic particles MM having the particle size equal to or less than a half of the distance Dc. However, when the metal magnetic particles having a particle size greater than a half of the distance Dc are distributed along the third direction D3 between the coil conductors CC, in the process of manufacturing the multilayer coil component 1, lamination misalignment between the coil conductors CC tends to occur. The occurrence of lamination misalignment between the coil conductors CC may decrease a cross-sectional area of a magnetic path located inside the coil 20 and in turn decrease the inductance. In the multilayer coil component 1, since the plurality of metal magnetic particles MM having the particle size equal to or less than a half of the distance Dc is distributed along the third direction D3 between the coil conductors CC, lamination misalignment between the coil conductors CC tends not to occur.
Consequently, the multilayer coil component 1 controls a decrease in inductance.
In a case in which the number of metal magnetic particles distributed along the third direction D3 between the coil conductors CC (coil conductors 21 to 26) is small, insulation between the coil conductors CC may decrease. The number of metal magnetic particles MM that have the particle size equal to or less than a half of the distance Dc and are distributed between the coil conductors CC tends to be larger than the number of metal magnetic particles that have a particle size greater than a half the distance Dc and are distributed between the coil conductors CC. Therefore, in the multilayer coil component 1, the insulation between the coil conductors CC tends not to decrease.
The number of metal magnetic particles that have a particle size less than one third of the distance Dc and are distributed between the coil conductors CC tends to be larger than the number of metal magnetic particles MM that have the particle size equal to or greater than one third of the distance Dc and are distributed between the coil conductors. However, in a case in which the metal magnetic particles having a particle size less than one third of the distance Dc are distributed between the coil conductors CC, gaps formed between the metal magnetic particles (metal magnetic particles MM) are small as compared with in a case in which the metal magnetic particles MM having the particle size equal to or greater than one third of the distance Dc are distributed between the coil conductors CC. Therefore, the resin RE tends not to exist between the metal magnetic particles, and the insulation between the coil conductors CC may decrease. In the multilayer coil component 1, since the plurality of metal magnetic particles MM having the particle size equal to or greater than one third of the distance Dc is distributed along the third direction D3 between the coil conductors CC, the resin RE tends to exist between the metal magnetic particles MM, and the insulation between the coil conductors CC tends not to decrease.
Consequently, the multilayer coil component 1 controls the decrease in the insulation between the coil conductors CC.
Q characteristics of the multilayer coil component 1 depend on a resistance of the coil conductors CC (coil conductors 21 to 26). In a high-frequency range, a current (signal) tends to flow near the surfaces of the coil conductors CC due to the skin effect. Therefore, as the surface resistance of the coil conductors CC increases, the Q characteristics of the multilayer coil component 1 decreases. A configuration in which the surfaces of the coil conductors CC have irregularities substantially increases a length of current flow, and thus increases the surface resistance, as compared with a configuration in which the surfaces of the coil conductors CC have no irregularities.
A configuration in which the surface roughness of each of the side surfaces SF1 is less than 40% of the average particle size of the metal magnetic particles MM controls an increase in surface resistance and controls a decrease in Q characteristics in a high-frequency range, as compared with a configuration in which the surface roughness of each of the side surfaces SF1 is equal to or greater than 40% of the average particle size of the metal magnetic particles MM. Therefore, the multilayer coil component 1 controls the increase in the surface resistance and controls the decrease in the Q characteristics in the high-frequency range.
In the multilayer coil component 1, the surface roughness of the pair of side surfaces SF2 is smaller than the surface roughness of the pair of side surfaces SF1. The multilayer coil component 1 has low surface resistance of the coil conductors CC (coil conductors 21 to 26), as compared with a configuration in which the surface roughness of the pair of side surfaces SF2 is equal to or greater than the surface roughness of the pair of side surfaces SF1. Therefore, the multilayer coil component 1 further controls the increase in the surface resistance and further controls the decrease in the Q characteristics in the high-frequency range.
In the multilayer coil component 1, the coil conductors CC (coil conductors 21 to 26) are plating conductors.
In a case in which the coil conductors are sintered metal conductors, the coil conductors are each formed by sintering a metal component (metal powder) contained in the conductive paste. In this case, the metal magnetic particles bite into the conductive paste before the metal component is sintered. Irregularities due to the shape of the metal magnetic particles are formed on a surface of the conductive paste. In a case in which a coil conductor is a sintered metal conductor, the coil conductor is deformed so that the metal magnetic particles bite into the coil conductor. Therefore, the configuration in which the coil conductor is the sintered metal conductor significantly increases surface roughness of the coil conductor.
In a case in which the coil conductors CC are the plating conductors, as illustrated in
Although the embodiments and modifications of the present invention have been described above, the present invention is not necessarily limited to the embodiments and modifications, and the embodiment can be variously changed without departing from the scope of the invention.
In the cross-section taken along the third direction D3, the area of the region where the metal magnetic particles MM are distributed along the third direction D3 may be equal to or less than 50% of the area of the region between the coil conductors CC adjacent to each other in the third direction D3. The configuration where, in the cross-section taken along the third direction D3, the area of the region where the metal magnetic particles MM are distributed along the third direction D3 is greater than 50% of the area of the region between the coil conductors CC adjacent to each other in the third direction D3 further controls the decrease in the insulation between the coil conductors CC, as described above.
The number of coil conductors CC (coil conductors 21 to 26) is not limited to the above-descried number.
The coil axis of the coil 20 may extend along the first direction D1. In this case, the magnetic layers 7 are laminated in the first direction D1, and the coil conductors CC (coil conductors 21 to 26) are separated from each other in the first direction D1.
The external electrode 4 may include only one of the electrode portions 4a, 4b. The external electrode 5 may also include only one of the electrode portions 5a, 5b.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2019-054732 | Mar 2019 | JP | national |
