Resistance element and method for manufacturing the same

Patent metadata

Field	Value
Publication number	US-2018197664-A1
Application number	US-201715842336-A
Country	US
Kind code	A1
Filing date	Dec 14, 2017
Priority date	Jan 6, 2017
Publication date	Jul 12, 2018
Grant date	—

Abstract

A frequency-dependent resistance element includes an element assembly composed of a sintered magnetic material and a coil conductor embedded in the element assembly. The sintered magnetic material is composed of a primary component containing Fe, Zn, Ni, and Cu and a secondary component containing Co. In the primary component, on a percent by mole basis, the Fe content is 46.79 to 47.69, the Zn content is 12.60 to 24.84, and the Ni content is 19.21 to 32.36 in terms of Fe 2 O 3 , ZnO, and NiO, respectively. The molar ratio (Ni:Zn) of Ni to Zn is (1−X):X, where X is from about 0.28 to about 0.56. The content of Co in terms of Co 3 O 4 is 1.0 to 10.0 parts by mass relative to 100 parts by mass of the primary component containing Fe, Zn, Ni, and Cu in terms of Fe 2 O 3 , ZnO, NiO, and CuO, respectively.

First claim

What is claimed is:

1 . A frequency-dependent resistance element comprising:
an element assembly composed of a sintered magnetic material; and a coil conductor embedded in the element assembly, the sintered magnetic material is composed of a primary component containing Fe, Zn, Ni, and Cu and a secondary component containing Co, in the primary component, an Fe content is from 46.79 percent by mole to 47.69 percent by mole in terms of Fe 2 O 3 , the Zn content is from 12.60 percent by mole to 24.84 percent by mole in terms of ZnO, and the Ni content is from 19.21 percent by mole to 32.36 percent by mole in terms of NiO, a molar ratio (Ni:Zn) of the Ni content to the Zn content is (1−X):X, where X is from 0.28 to 0.56, and a content of Co serving as the secondary component in terms of Co 3 O 4 is from 1.0 part by mass to 10.0 parts by mass relative to 100 parts by mass of the primary component containing Fe, Zn, Ni, and Cu in terms of Fe 2 O 3 , ZnO, NiO, and CuO, respectively.

2 . The frequency-dependent resistance element according to claim 1 , wherein X is from 0.44 to 0.56.

3 . The frequency-dependent resistance element according to claim 1 , wherein a pore area percentage of the element assembly is from 3% to 20%.

4 . The frequency-dependent resistance element according to claim 1 , wherein a formula 1 is satisfied:
f 1= A×Y+B   (formula 1)

and in the formula 1:
f1 represents a frequency (MHz) that provides R 2 ,
where R 2 represents a resistance component (Q) corresponding to a real part of an impedance of the frequency-dependent resistance element and satisfies R 2 =R 1 +17, and
R 1 represents a resistance component (Q) corresponding to the real part of the impedance of the frequency-dependent resistance element at 1 MHz,

Y represents the content (part by mass) of Co in terms of Co 3 O 4 relative to 100 parts by mass of the primary component containing Fe, Zn, Ni, and Cu in terms of Fe 2 O 3 , ZnO, NiO, and CuO, respectively, in the sintered magnetic material,
A is from 36.8 to 38.0, and
B is from 14.0 to 56.0.

5 . The frequency-dependent resistance element according to claim 1 , wherein a formula 2 is satisfied:
f 2= C×Y 2 +D×Y+E   (formula 2)

and in the formula 2:
f2 represents a frequency (MHz) at which μ″ is 2, where μ″ is an imaginary part of the complex permeability of the frequency-dependent resistance element,
Y represents the content (part by mass) of Co in terms of Co 3 O 4 relative to 100 parts by mass of the primary component containing Fe, Zn, Ni, and Cu in terms of Fe 2 O 3 , ZnO, NiO, and CuO, respectively, in the sintered magnetic material,
C is from 1.78 to 2.60,
D is from 30.00 to 40.00, and
E is from 10.00 to 35.00.

6 . The frequency-dependent resistance element according to claim 4 , wherein a formula 3 and a formula 4 are satisfied:
A= 0.046× Z+ 36.828  (formula 3)
B= 2.32× Z+ 6.63  (formula 4)

and in the formulae 3 and 4:
A and B are the same as in claim 4 , and
Z represents a pore area percentage.

7 . The frequency-dependent resistance element according to claim 5 , wherein a formula 5, a formula 6, and a formula 7 are satisfied:
C= 0.046× Z+ 1.61  (formula 5)
D= 0.567× Z+ 28.37  (formula 6)
E= 1.385× Z+ 5.74  (formula 7)

and in the formulae 5, 6 and 7:
C, D, and E are the same as in claim 5 , and
Z represents a pore area percentage.

8 . The frequency-dependent resistance element according to claim 4 , wherein f1 is 50 MHz or more.

9 . The frequency-dependent resistance element according to claim 1 , wherein the element assembly is a multilayer body composed of a plurality of layers of the sintered magnetic material.

10 . The frequency-dependent resistance element according to claim 9 , wherein the plurality of layers of the sintered magnetic material are stacked with conductor layers interposed therebetween, and the layers define holes via which the conductor layers electrically connect to each other.

11 . The frequency-dependent resistance element according to claim 2 , wherein a pore area percentage of the element assembly is from 3% to 20%.

12 . The frequency-dependent resistance element according to claim 2 , wherein a formula 1 is satisfied:
f 1= A×Y+B   (formula 1)

and in the formula 1:
f1 represents a frequency (MHz) that provides R 2 ,
where R 2 represents a resistance component (Q) corresponding to a real part of an impedance of the frequency-dependent resistance element and satisfies R 2 =R 1 +17, and
R 1 represents a resistance component (Q) corresponding to the real part of the impedance of the frequency-dependent resistance element at 1 MHz,

Y represents the content (part by mass) of Co in terms of Co 3 O 4 relative to 100 parts by mass of the primary component containing Fe, Zn, Ni, and Cu in terms of Fe 2 O 3 , ZnO, NiO, and CuO, respectively, in the sintered magnetic material,
A is from 36.8 to 38.0, and
B is from 14.0 to 56.0.

13 . The frequency-dependent resistance element according to claim 2 , wherein a formula 2 is satisfied:
f 2= C×Y 2 +D×Y+E   (formula 2)

and in the formula 2:
f2 represents a frequency (MHz) at which μ″ is 2, where μ″ is an imaginary part of the complex permeability of the frequency-dependent resistance element,
Y represents the content (part by mass) of Co in terms of Co 3 O 4 relative to 100 parts by mass of the primary component containing Fe, Zn, Ni, and Cu in terms of Fe 2 O 3 , ZnO, NiO, and CuO, respectively, in the sintered magnetic material,
C is from 1.78 to 2.60,
D is from 30.00 to 40.00, and
E is from 10.00 to 35.00.

14 . The frequency-dependent resistance element according to claim 2 , wherein the element assembly is a multilayer body composed of a plurality of layers of the sintered magnetic material.

15 . A method for controlling frequency characteristics of a frequency-dependent resistance element including an element assembly composed of a sintered magnetic material and a coil conductor embedded in the element assembly, the sintered magnetic material being composed of a primary component containing Fe, Zn, Ni, and Cu and a secondary component containing Co, and in the primary component, the Fe content being from 46.79 percent by mole to 47.69 percent by mole in terms of Fe 2 O 3 , the Zn content being from 12.60 percent by mole to 24.84 percent by mole in terms of ZnO, and the Ni content being from 19.21 percent by mole to 32.36 percent by mole in terms of NiO, the method comprising:
controlling a rising frequency of a resistance component R corresponding to a real part of the impedance or an imaginary part μ″ of the complex permeability of the frequency-dependent resistance element by adjusting a molar ratio (Ni:Zn) denoted by (1−X):X of the Ni content to the Zn content, where X is within a range from 0.28 to 0.56, and by adjusting an amount of Co added as the secondary component.

16 . The method according to claim 15 , wherein the controlling a rising frequency of a resistance component R includes adjusting the molar ratio (Ni:Zn) where X is from 0.44 to 0.56.

17 . The method according to claim 15 , wherein in the controlling a rising frequency of a resistance component, a formula 1 is satisfied:
f 1= A×Y+B   (formula 1)

and in the formula 1:
f1 represents a frequency (MHz) that provides R 2 ,
where R 2 represents a resistance component (Q) corresponding to a real part of an impedance of the frequency-dependent resistance element and satisfies R 2 =R 1 +17, an

Assignees

• Murata Manufacturing Co

Inventors

• Koizumi Kazuya
• Sugii Kazutoshi

Classifications

• H01F2027/2809

  on stacked layers · CPC title

• H01C17/06

  adapted for coating resistive material on a base · CPC title

• H01F1/344

  Ferrites, e.g. having a cubic spinel structure (X2+O)(Y23+O3), e.g. magnetite Fe3O4 · CPC title

• H01F27/255

  made from particles (H01F27/26 takes precedence) · CPC title

• C04B35/2666

  Other ferrites containing nickel, copper or cobalt · CPC title