POWER INDUCTOR ENCAPSULATED THROUGH INJECTION MOLDING
20180001523 · 2018-01-04
Inventors
Cpc classification
B29C45/00
PERFORMING OPERATIONS; TRANSPORTING
H01F2003/106
ELECTRICITY
H01F2017/048
ELECTRICITY
H01F27/29
ELECTRICITY
International classification
Abstract
The present invention discloses a power inductor encapsulated through injection molding. The power inductor comprises a coil winding, a soft magnetic ferrite middle column inserted in a middle of the coil winding, and a magnetic powder glue for encapsulating the coil winding and the soft magnetic ferrite middle column through injection molding. The power inductor is square and meets L≧W and 2rc>0.4×2W, wherein a section width of the soft magnetic ferrite middle column perpendicular to a height direction of the inductor is 2rc, a length of the power inductor is 2L, and a width of the power inductor is 2W. According to the present invention, a balanced direct-current resistance and a direct-current superposition saturation characteristic can be obtained, and the direct-current resistance is greatly decreased while an excellent direct-current superposition saturation characteristic is ensured.
Claims
1. A power inductor encapsulated through injection molding, comprising a coil winding, a soft magnetic ferrite middle column inserted in a middle of the coil winding, and a magnetic powder glue for encapsulating the coil winding and the soft magnetic ferrite middle column through injection molding; wherein the power inductor is square and meets:
L≧W 2r.sub.c>0.4×2W, wherein a section width of the soft magnetic ferrite middle column perpendicular to a height direction of the inductor is 2r.sub.c, a length of the power inductor is 2L, and a width of the power inductor is 2W;
4H/5>h.sub.c>H/2 wherein, h.sub.c is a height of the soft magnetic ferrite middle column along the height direction of the power inductor, and a height of the power inductor is H; and
h.sub.c≧H−2r.sub.c/3.
2. The power inductor encapsulated through injection molding according to claim 1, wherein the soft magnetic ferrite middle column is arranged in a centrosymmetric position of the power inductor.
3. The power inductor encapsulated through injection molding according to claim 2, wherein a section shape of the soft magnetic ferrite middle column perpendicular to the height direction of the power inductor comprises a circle, a square, a rectangle and a race track.
4. The power inductor encapsulated through injection molding according to claim 3, wherein materials of the soft magnetic ferrite middle column comprise manganese zinc ferrite and nickel zinc ferrite.
5. The power inductor encapsulated through injection molding according to claim 4, wherein the magnetic powder glue is formed by mixing resin and magnetic metal powder; materials of the resin comprise epoxy resin, silicone resin and phenolic resin; and materials of the magnetic metal powder comprise carbonyl iron, iron-silicon alloy, iron-silicon-aluminum alloy, iron-silicon-chromium alloy, iron-nickel alloy, iron-nickel-molybdenum alloy and amorphous alloy.
6. The power inductor encapsulated through injection molding according to claim 5, wherein a magnetic permeability of the magnetic powder glue is more than or equal to 5 and less than or equal to 20.
7. The power inductor encapsulated through injection molding according to claim 6, wherein a winding window height h.sub.w of the coil winding is less than or equal to h.sub.c.
8. The power inductor encapsulated through injection molding according to claim 1, wherein the power inductor further comprises two terminal parts, and the two terminal parts are welded with the coil winding and provide electrical connection between the power inductor and an external circuit.
Description
BRIEF DESCRIPTION OF DRAWINGS
[0026] For those skilled in the art, the above and other purposes, features and advantages of the present invention will be apparent below from detailed description of the present invention with reference to drawings.
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[0039]
LIST OF REFERENCE NUMERALS
[0040] 1—coil winding
[0041] 2—soft magnetic ferrite middle column
[0042] 3—magnetic powder glue
[0043] 4a—lead frame
[0044] 4—terminal part
[0045] 5—nozzle
[0046] 6—runner
[0047] 2L—inductor length
[0048] 2W—inductor width
[0049] H—inductor height
[0050] d—winding window width
[0051] h.sub.w—winding window height
[0052] r.sub.c—radius of soft magnetic ferrite middle column
[0053] h.sub.c—height of soft magnetic ferrite middle column along a height direction of the inductor; and
[0054] h—yoke position thickness of encapsulated magnetic powder glue
DETAILED DESCRIPTION
[0055] A brief introduction is given first. The present invention relates to an inductor comprising a coil winding, a soft magnetic ferrite middle column inserted in a middle of the coil winding, and a magnetic powder glue for encapsulating the coil winding and the soft magnetic ferrite middle column by injection molding. A size of the inductor is square, and a length, a width and a height of the inductor are respectively as follows:
2L.Math.2W.Math.H(L≧W),
[0056] wherein a section width 2r.sub.c of the soft magnetic ferrite middle column perpendicular to a height direction of the inductor needs to be more than 0.4 time that of an inductor width 2W; a height h.sub.c of the soft magnetic ferrite middle column along the height direction of the inductor needs to be more than ½ of an inductor height H and less than ⅘ of the inductor height; the height h.sub.c of the soft magnetic ferrite middle column along the height direction of the inductor needs to be not less than H−2r.sub.c/3; the soft magnetic ferrite middle column should be arranged in a centrosymmetric position of the inductor; a section shape of the soft magnetic ferrite middle column perpendicular to the height direction of the inductor may be a circle, a square, a rectangle and a race track, and a width of the soft magnetic ferrite middle column is 2r.sub.c; materials of the soft magnetic ferrite middle column comprise manganese zinc ferrite and nickel zinc ferrite; the magnetic powder glue is formed by mixing resin and magnetic metal powder; materials of the resin comprise but not limited to epoxy resin, silicone resin, phenolic resin and the like; and materials of the magnetic metal powder comprise but not limited to carbonyl iron, iron-silicon alloy, iron-silicon-aluminum alloy, iron-silicon-chromium alloy, iron-nickel alloy, iron-nickel-molybdenum alloy, amorphous alloy, and the like. A magnetic permeability of the magnetic powder glue is not less than 5 and not more than 20. A winding window height of the coil winding is not more than the height of the soft magnetic ferrite middle column, preferably equal to the height of the ferrite middle column. The inductor may further comprise two terminal parts which are welded with the coil winding and provide electrical connection between the inductor and an external circuit.
[0057] According to an energy storage formula of the inductor:
L.Math.I.sup.2=B.Math.J.Math.K.sub.u.Math.A.sub.e.Math.A.sub.w,
[0058] it can be seen that a magnetic flux density B and a current density J basically represent a saturation degree of the iron core and a heating degree of the winding under given energy storage conditions (an induction quantity L and a rated current I). In this case, if a filling rate K.sub.u of the winding window is a constant value, in order to achieve a better direct-current saturation characteristic and a lower direct-current resistance, a product of a sectional area Ae of the magnetic circuit and an area Aw of the window, i.e., AP=Ae.Math.Aw, is expected to be increased as much as possible.
[0059] A magnetic permeability μ of the material determines allocation of the values B and J under a condition that the product AP is given. For example, a needed number N of turns is small if the magnetic permeability .sub.11 of the material is high; then the value B is greater while the value J is smaller under a condition that the same induction quantity L and rated current I are reached; and if the magnetic permeability μ of the material is low, the value B is smaller while the value J is greater under a condition that the same induction quantity L and saturation current I are reached.
[0060] Since the inductor designed in the present invention is mainly used in the power inductor, in a general usage condition that a direct-current is high and a ripple rate is low under an application of an output filter circuit, the inductor designed in the present invention is expected to achieve a lower winding heating degree, that is, a smaller value J. Therefore, a high magnetic permeability μ of the material is expected to be obtained in the present invention. Since the present invention belongs to a mixed material and the magnetic permeability of the soft magnetic ferrite material is far higher than that of the encapsulated magnetic powder glue, an equivalent magnetic permeability of the whole inductor is determined by an equivalent magnetic circuit length Le of the encapsulated magnetic powder glue, and the smaller the Le is, the higher the equivalent magnetic permeability of the whole inductor is. If so, for the inductor design in the present invention, a greater value of Ae.Math.Aw/Le is expected to be obtained, and then both the magnetic flux density B and the current density J can be taken into account.
[0061]
2L.Math.2W.Math.H(L≧W).
[0062] Since the saturation characteristic of the inductor needs to be considered in the present invention and the inductor is difficult to be saturated due to a large dimension in a length direction, the schematic diagram is a sectional dimension perpendicular to the length direction. Assuming that the soft magnetic ferrite middle column has a circular section and a radius of r.sub.c, a yoke position thickness of the encapsulated magnetic powder glue is h, and an outer wall thickness of the encapsulated magnetic powder glue generally needs to consider winding terminal welding and other manufacturing procedures and is set as 1.5 h. A width of the winding window is d, and a height of the winding window is h.sub.w, so a sectional area of the magnetic circuit is as follows:
Ae=2πr.sub.c.Math.h;
[0063] an area of the window is as follows:
Aw=d.Math.(H−2h);
[0064] while a length of an equivalent magnetic circuit is as follows:
Le=2d+H,
then:
Ae.Math.Aw/Le=2π.Math.[rc.Math.d/(2d+H)].Math.h.Math.(H−2h)
[0065] A condition for obtaining a maximum value of h.Math.(H−2h) is estimated as follows:
h=H/4.
[0066] However, because:
r.sub.c+d=W−1.5h,
[0067] the smaller the yoke position thickness h of the encapsulated magnetic powder glue is, the higher the obtained value is, and then apparently, the condition for wholly obtaining the maximum value is the yoke position thickness of the encapsulated magnetic powder glue:
h<H/4.
[0068] If r.sub.c+d=W−1.5h is a constant value under a given yoke position thickness h of the encapsulated magnetic powder glue, as shown in
(W−1.5h)/2>d, r.sub.c>d.
[0069] Since the saturated magnetic flux density of the encapsulated magnetic powder glue is generally more than 1.5 times higher than saturated magnetic flux density of a soft magnetic ferrite material, in order to prevent the soft magnetic ferrite material from being saturated in advance during actual usage, considering continuity of the magnetic flux, the sectional area of the soft magnetic ferrite middle column needs to be increased to be more than 1.5 times that of the sectional area of the magnetic powder glue, and a condition may be met during calculation as follows:
r.sub.c>3h,
[0070] that is, the radius r.sub.c of the soft magnetic ferrite middle column should be more than 3 times that of the yoke position thickness of the magnetic powder glue. Several requirements mentioned above are comprehensively considered as follows:
r.sub.c+d=W−1.5h, r.sub.c>d and r.sub.c>3h.
[0071] A formula is calculated as follows:
r.sub.c>2W/5,
[0072] that is, the radius r.sub.c of the soft magnetic ferrite middle column needs to be more than 0.4 time that of a half width W of the inductor in the inductor design. Similarly, another condition h<H/4 means that the height h.sub.c=H−2h of the soft magnetic ferrite middle column in the inductor design needs to be greater than ½ of the height H of the inductor. The yoke position needs a certain thickness to prevent possible process damage, so the height of the soft magnetic ferrite middle column can not exceed ⅘ of the height H of the inductor. That is to say, 4H/5>h.sub.c>H/2. Meanwhile, a condition r.sub.c≧3h for avoiding saturation of the soft magnetic ferrite material also means that the height of the soft magnetic ferrite middle column is as follows:
h.sub.c=H−2h≧H−2r.sub.c/3.
[0073] The section of the soft magnetic ferrite middle column can also be a square. It can be proved that a side length of the square can correspond to an outer diameter 2r.sub.c of the soft magnetic ferrite middle column, and a better characteristic may be obtained by meeting the above dimensional limit condition. For the square, assuming that the side length of the square is correspondingly 2r.sub.c, the sectional area of the soft magnetic ferrite middle column is as follows:
2r.sub.c.Math.2r.sub.c,
[0074] while the sectional area of the magnetic powder glue can be calculated as a product of a perimeter of the soft magnetic ferrite middle column and the yoke position thickness of the magnetic powder glue, and can be expressed as follows:
4.Math.2r.sub.c.Math.h.
[0075] By considering that the sectional area of the soft magnetic ferrite middle column is more than 1.5 times that of the sectional area of the magnetic powder glue, a formula can be obtained through calculation as follows:
r.sub.c≧3h,
while:
Ae.Math.Aw/Le=8r.sub.c.Math.d.Math.h.Math.(H−2h)/(2d+H)
[0076] i.e., it can be deduced that an optimal value condition needs to satisfy r.sub.c>d and h<H/4; and meanwhile, the height h.sub.c≧H−2r.sub.c/3 of the soft magnetic ferrite middle column can be deduced. In other words, as long as the side length of the square is correspondingly 2r.sub.c, a related optimal value condition is still the same.
[0077] In an actual application, if the length of the inductor is larger than the width, the soft magnetic ferrite middle column in the present invention can be lengthened along the length direction of the inductor for avoiding waste of a space. As shown in
x.Math.2r.sub.c(x>0),
[0078] while the width is still kept at 2r.sub.c. It can be seen that the sectional area of the soft magnetic ferrite middle column is as follows:
(1+x).Math.2r.sub.c.Math.2r.sub.c
[0079] while the perimeter of the soft magnetic ferrite middle column is as follows:
8r.sub.c+2x.Math.2r.sub.c,
[0080] then the sectional area of the magnetic powder glue can be expressed as:
(8+4x).Math.r.sub.c.Math.h.
[0081] Then, as long as a relationship is met as follows:
r.sub.c≧3h,
[0082] the sectional area of the soft magnetic ferrite middle column can also meet the condition of being more than 1.5 times that of the sectional area of the magnetic powder glue. The reason is that the sectional area of the magnetic powder glue is in direct proportion to the perimeter of the soft magnetic ferrite middle column, while when the shape of the soft magnetic ferrite middle column is lengthened from the square to the rectangle, an increase speed of the sectional area of the ferrite middle column is higher than an increase speed of the perimeter of the ferrite middle column.
[0083] Moreover:
Ae.Math.Aw/Le=(8+4x).Math.r.sub.c.Math.d.Math.h.Math.(H−2h)/(2d+H)
[0084] that is, the optimal value condition still can be deduced to meet a relationship as follows:
r.sub.c>d.
[0085] In other words, as long as a width of a rectangular section of the ferrite middle column is correspondingly 2r.sub.c, the related optimal value condition is still the same.
[0086] As shown in
x.Math.2r.sub.c(x>0),
[0087] while the width is still kept at a diameter 2r.sub.c of the circle. It can be seen that the sectional area of the soft magnetic ferrite middle column is as follows:
x.Math.2r.sub.c.Math.2r.sub.c+π.Math.r.sub.c.sup.2,
[0088] while the perimeter of the soft magnetic ferrite middle column is as follows:
2x.Math.2r.sub.c+2π.Math.r.sub.c
[0089] then the sectional area of the magnetic powder glue can be expressed as:
(2π+4x).Math.r.sub.c.Math.h
[0090] then as long as a relationship is met as follows:
r.sub.c≧3h,
[0091] the sectional area of the soft magnetic ferrite middle column can also meet the condition of being more than 1.5 times that of the sectional area of the magnetic powder glue. The reason is that the sectional area of the magnetic powder glue is in direct proportion to the perimeter of the soft magnetic ferrite middle column, while when the shape of the soft magnetic ferrite middle column is lengthened from the circle to the race track, an increase speed of the sectional area of the ferrite middle column is higher than an increase speed of the perimeter of the ferrite middle column. Moreover:
Ae.Math.Aw/Le=(2π+4x).Math.r.sub.c.Math.d.Math.h.Math.(H−2h)/(2d+H)
[0092] that is, the optimal value condition still can be deduced to meet a relationship as follows:
r.sub.c>d.
[0093] In other words, as long as a width of a race track shaped section of the ferrite middle column is correspondingly 2r.sub.c, the related optimal value condition is still the same.
[0094] It can be seen from the above that as long as a width 2r.sub.c of the section of the soft magnetic ferrite middle column perpendicular to the height direction of the inductor needs to be more than 0.4 time that of the width 2W of the inductor, lengthening of the section may not change advantages of the design on the direct-current saturation characteristic and the direct-current resistance. The shape of the section of the soft magnetic ferrite middle column perpendicular to the height direction of the power inductor comprises but not limited to the circle, the square, the rectangle and the race track.
[0095] Meanwhile, it is considered that the ferrite middle column must be arranged in a centrosymmetric position of the inductor, that is, the ferrite middle column must be simultaneously arranged in a centrosymmetric position of the length-width direction and the height direction, so that a better direct-current saturation characteristic is easily obtained, and a partial saturation problem caused by asymmetry is difficult to appear. Materials of the soft magnetic ferrite middle column comprise manganese zinc ferrite and nickel zinc ferrite; the magnetic powder glue is formed by mixing resin and magnetic metal powder; materials of the resin material comprise but not limited to epoxy resin, silicone resin, phenolic resin and the like; and materials of the magnetic metal powder comprise but not limited to carbonyl iron, iron-silicon alloy, iron-silicon-aluminum alloy, iron-silicon-chromium alloy, iron-nickel alloy, iron-nickel-molybdenum alloy, amorphous alloy, and the like. Since the magnetic powder glue in the present invention encapsulates the coil winding and the soft magnetic ferrite middle column in an injection molding manner, the magnetic permeability of the magnetic powder glue cannot be higher than 20. If the magnetic permeability is too high, the magnetic powder glue is poor in fluidity and is unfavorable for a manufacturing procedure of the injection molding. Meanwhile, the magnetic permeability of the magnetic powder glue cannot be less than 5, and if the magnetic permeability is too small, the inductor may have a higher direct-current resistance. It can be seen from the above deduction that, the winding window height h.sub.w of the coil winding cannot be greater than the height h.sub.c of the soft magnetic ferrite middle column. If the winding window height h.sub.w of the coil winding is too large, the yoke position thickness h of the magnetic powder glue may be decreased, and then the magnetic flux of the soft magnetic ferrite middle column will be hindered. Preferably, the winding window height h.sub.w of the coil winding should be equal to the height h.sub.c of the ferrite middle column. The inductor may further comprise two terminal parts which are welded with the coil winding and provide electrical connection between the inductor and an external circuit.
[0096] Since the middle column adopts the soft magnetic ferrite material with a high magnetic permeability in the present invention, compared with a manufacturing procedure of an existing mold-pressing inductor, a magnetic permeability of outer encapsulation can be decreased, thereby easily adopting the manufacturing procedure of the injection molding, reducing molding pressure, increasing production efficiency and reliability and easily realizing automatic production. For the characteristic, a defect of easy saturation of the I-shaped magnetic glue inductor is overcome, and through the dimensional setting of the present invention, a balanced direct-current resistance and a direct-current saturation characteristic can be obtained.
Embodiment 1
[0097] A corresponding reference sample in the present embodiment is an I-shaped magnetic glue inductor NR6045-100M. A length, a width and a height of the reference sample are respectively 6 mm.Math.6 mm.Math.4.5 mm. As shown in
[0098] It can be clearly seen from
[0099] In the aspect of the manufacturing procedure, as shown in
Embodiment 2
[0100] A reference sample in the present embodiment is an integrally molded mold-pressing inductor in the prior art. A length, a width and a height of the reference sample are respectively 7 mm.Math.6.6 mm.Math.3 mm. As shown in
[0101] It can be seen from
Embodiment 3
[0102] The present embodiment shows how to achieve a better inductor level in an industry by using convenient manufacturing procedure conditions. Particularly, corresponding reference samples in the present embodiment are thin power inductors, wherein NR4012-2R2 is an I-shaped magnetic glue inductor, and MPI4442-2R2 is a metal powder mold-pressing molding inductor. It can be seen from
Embodiment 4
[0103] A length 2L and a width 2W of a power inductor involved in the present embodiment are respectively 2.5 mm and 2.0 mm, and a maximum height H of the power inductor is 1.2 mm. Since the length of the inductor in the present embodiment is greater than the width, a shape of a section of the soft magnetic ferrite middle column is designed as a race track in order to effectively utilize a space in a length direction of the inductor.
[0104] Description of preferred embodiments is provided above, so that the present invention can be used or utilized by any of those skilled in the art. Various modifications to these embodiments are apparent to those skilled in the art, and a general principle described herein can be applied to other embodiments without using creativeness. Therefore, the present invention is not limited to embodiments illustrated herein and should conform to a widest scope consistent with principles and new features disclosed herein.