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Technologies for Developing and Designing CRT Ferrite Core Materials |
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| The demand for optimal design technologies for cathode-ray tube (CRT) components is increasing, thus enabling TVs and other image-display equipment to have larger and wider screens, higher image quality, and lower power consumption. To achieve these goals, it is important to use low-loss ferrite components in deflection circuits, high-voltage circuits and other CRT sections, because low-loss ferrites reduce heat generation and thus ensure greater safety. We, therefore, report on the latest technologies applied to the development of low-loss ferrites, and introduce recent design technologies based on computer-simulated design of ferrite core materials and computer-simulated analyses of magnetic fields and heat generation. | |
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1. INTRODUCTION |
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| Television is one of the most popular inventions of the 20th century. Recently, however, there has been a growing need for new CRTs with brighter, higher definition, flatter and larger screens, as is evident in the commercialization of liquid crystal displays. In response, ferrite components for CRTs will have to become smaller and lighter while achieving higher performance levels. At the same time, Japanese ferrite component makers are being compelled to reduce production costs to overcome the yen's rising exchange rate. Accordingly, it is now imperative that CRT ferrite components incorporate both performance and cost advantages, starting with the design stage. Figure 1 shows a circuit diagram of a TV receiver with a built-in satellite broadcast tuner. TVs and other image displays incorporate a variety of ferrite components, such as deflection yokes, flyback transformers (FBT), convergence components, linearity coils, transformer choke coils and noise suppression devices. These components use Mn-Zn, Mg-Zn or Ni- Zn ferrites. In this report, we shall examine the ferrites used for deflection yokes and flyback transformers. | ![]() |
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2.FERRITE MATERIALS AND APPLICATIONS |
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| Figure 2 summarizes the major ferrite
technologies that have been developed since
the start of TV broadcasting. |
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2-1.Materials for Deflection Yoke Ferrites |
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| From 1955 to 1965, when ferrites were first applied to electron beam deflection, Mn-Zn or Ni-Zn ferrites were used. Providing lower resistance, Mn-Zn ferrites were used with saddle toroidal winding. But due to ringing problems, they were gradually replaced by Ni-Zn ferrites, which featured higher resistance. Currently, Japanese makers mainly select Mg-Zn ferrites for their low material costs. Tables 1 and 2 compare the characteristics of different ferrite core materials. Table 3 lists the ferrite core requirements as seen from the producers of deflection yokes. In displays with a 120 kHz horizontal scanning frequency, Mn- Zn ferrites may be employed and, in some special cases, slot- type core shapes are adopted to allow different winding patterns for better heat dissipation. | |
| Table-1 Comparison Table of Ferrite Material for DY Use |
| Property | Mg-Zn | Ni-Zn | Mn-Zn | |
| Core for Deflection Yoke | Core Loss | |||
| Saturated Magnetic Flux Density | ||||
| Resistivity | ||||
| AC Initial Permeability | ||||
| Curie Temperature | ||||
| Deflection Yoke Coil | Rise in Temperature | |||
| Ringing | ||||
| Cross Talk | ||||
| Beats | ||||
| Cost | ||||
| Total Cost Performance | ||||
| Table-2 Standard Material Characteristics of Ferrite Cores for Deflection Yokes |
| Property | Symbol | Unit | Condition | DY-1 Mg-Zn |
DY-2 Mg-Zn |
DY-3 Mn-Zn |
DY-4 Ni-Zn |
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| AC Initial Permeability | - | 0.1 MHz | 350 | 380 | 1800 | 500 | ||
| Saturation Magnetic Flux Density | Bs | mT | 23 |
230 | 250 | 500 | 360 | |
| 100 |
160 | 170 | 400 | 295 | ||||
| Corecivity | Hc | A/m | 23 |
50 | 30 | 20 | 36 | |
| Relative Loss Factor | 0.1 MHz | < 50 | <120 | < 5 | < 30 | |||
| Core Loss | Pc | kW/m3 | 25 kHz (100 mT) |
23 |
420 | 230 | 90 | 280 |
| 60 |
380 | 170 | 70 | 280 | ||||
| 100 |
430 | 170 | 60 | 260 | ||||
| 100 kHz (100 mT) |
23 |
1500 | 1000 | 270 | 960 | |||
| 60 |
1470 | 850 | 230 | 950 | ||||
| 100 |
1640 | 860 | 180 | 940 | ||||
| Curie Temperature | Tc | - | >145 | >145 | >180 | >200 | ||
| Resistivity | - | 105 | 105 | 1 | 105 | |||
| Table-3 Customer Needs for Deflection Yoke Cores |
| Field | Use | Customer's Request |
| Consumer TV |
Deflection Angel 110 |
Low Cost |
| Monitor | Horizontal Scanning Frequency |
Precision(Inner Dimension,Roundness)High Saturated Magnetic Flux Density Low Core Loss |
| High Frequency Monitor | Horizontal Scanning frequency 90-130 kHz |
Precision(Dimension)High Saturated Magnetic Flux Density Low Core Loss |
| HDTV |
Deflection Angel 110 |
Low Cost Precision(Dimension,Roundness) High Saturated Magnetic Flux Density Low Core Loss |
2-2.Materials for Flyback Transformers |
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| Mn-Zn ferrites have the advantage of low loss and high saturation flux density, making them suitable core materials for transformers. Furthermore, their core loss performance is being improved, using micro-crystal structure control technologies. Table 4 shows the characteristics of FBT ferrites in practical use over recent years. Since heat generation inside FBTs must be minimized to ensure safety, utmost efforts have been exerted to reduce core loss. In addition, efforts have been made to curb the core base diameter so as to reduce core material costs, core size and weight. Figure 5 presents the history of core loss reduction through the development of new production processes and new element technologies. Today, the average core loss is only one-fifth or one-sixth of the initial levels, when ferrite cores were first applied to FBTs. | |
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| Table-4 Standard material characteristics of ferrite cores for flyback transformers | |
| Property | Symbol | Unit | Condition | FBT-1 | FBT-2 | FBT-3 | |
| AC Initial Permeability | - | 100 KHz | 1800 | 2300 | 2200 | ||
| Saturation Magnetic Flux Density | Bs | mT | 23 |
520 | 500 | 500 | |
| 100 |
420 | 400 | 400 | ||||
| Corecivity | Hc | A/m | 23 |
13 | 13 | 13 | |
| Relative Loss Factor | 0.1 MHz | < 5 | < 5 | < 5 | |||
| Core Loss | Pc | kW/m3 | 16 kHz (150 mT) |
60 |
5.4 | 4.6 | 3.8 |
| 80 |
3.9 | 3.5 | 2.9 | ||||
| 100 |
3.5 | 3.3 | 2.7 | ||||
| 32 kHz (200 mT) |
60 |
24 | 22 | 18 | |||
| 80 |
19 | 18 | 15 | ||||
| 100 |
17 | 16 | 13 | ||||
| 50 kHz (200 mT) |
60 |
43 | 39 | 32 | |||
| 80 |
36 | 33 | 27 | ||||
| 100 |
32 | 29 | 24 | ||||
| 100 kHz (200 mT) |
60 |
110 | 100 | 82 | |||
| 80 |
95 | 88 | 72 | ||||
| 100 |
90 | 85 | 70 | ||||
| Curie Temperature | Tc | - | >200 | >200 | >200 | ||
| Temperature Coefficient in Permeability | X10-6 | 20 - 80 |
8 | 6 | 6 | ||
| Resistivity | - | 3 | 3 | 3 | |||
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3.HIGH-PRECISION PROCESSING TECHNOLOGIES |
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3-1.Precise Dimensions of Deflection Yoke Cores |
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| In the design of deflection yokes, the saddle-saddle winding method has been adopted in answer to the growing need for higher quality image displays. Since this requires greater convergence precision, it is increasingly important to achieve higher precision in core dimensions. Dimensional precision has been improved mainly by NC processing machines, which can grind the curved surfaces of cores with higher precision, so that the gaps between the coil and core are drastically reduced for higher convergence precision. | |
3-2.Gap Surface Grinding for FBT Cores |
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In recent years, core design has seen a rapid change, that is from split winding to layer winding in order to prevent rare shorting in high-voltage areas and to realize uniform winding density. While layer winding partially solves ringing problems, efforts are also being made to enhance gap surface grinding precision and to minimize sintering deformation for the correction of ringing. Furthermore, higher precision in grinding and sintering is in greater demand due to the ongoing changes in core coupling methods, from the use of metallic clamps to the use of glues. Because high-voltage FBT cores require wider gaps between the core and coil, the tolerance for inductance must be below +2.5%. Thus, gap grinding precision must be improved to a level that is no more than 10 um deviation in the case of high-voltage FBT cores. |
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4.DESIGN OF FERRITE COMPONENTS USING A CAE SYSTEM |
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| In order to put an end to the inefficient development of new ferrite components based on trial and error, we have been utilizing the computer-aided engineering (CAE) technique as a design tool for magnetic components since 1984. We now have a ferrite material design system (MAGSYS-F) and a magnetic field analysis system (S-FIAS). As a result, it has become possible to simulate heat generation in planned ferrite components, thus remarkably cutting the design time and improving the design accuracy. | |
4-1.Ferrite Material Design System (MAGSYS-F) |
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| MAGSYS-F is used to predetermine manufacturing conditions that will meet the customer's specification requirements. It adopts artificial intelligence technologies to enable the systematic utilization of theoretical, experimental and empirical data bases. By indicating the experimental conditions, the design engineer can obtain from MAGSYS-F suitable manufacturing conditions in the form of graphs and tables. For example, Figure 6 compares the actual measurement values and MAGSYS-F output values concerning the ferrite loss coefficient and disaccommodation of a Mn-Zn ferrite. | |
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4-2.General-purpose Magnetic Field Analysis System (S-FIAS) |
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We have developed a software program to simulate the electromagnetic characteristics of axial-symmetry coils, applying the marginal element method. By inputting customer specifications on core shape, materials, winding shape, input signals and ambient conditions, we can obtain from S-FIAS the data needed to design a coil. Through repeated simulations using varied input data, it is possible to determine the optimal design specifications for a coil product. Figure 7 provides a flow chart of simulation steps, from data input to output. Table 5 lists the output data items available from S-FIAS, for the design of coil products. These items include inductance, mutual inductance, leakage flux, DC overlap characteristics, and flux distribution. |
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| Table-5 Application & Output Items. | |
| Application | CAE System | FDK core name | Output Items | |||||
| Inductance | Mutual Inductance | Leackage Flux | DC Bias | Flux Density Distribusion | Core Heat Evolution | |||
| Deflection Yoke | SUPER- FIAS |
DY DP | - | - | - | |||
| Flyback Transformaer | SUPER- FIAS |
RU RUI | ||||||
| Switching Power Supply Transformer | SUPER- FIAS |
EI EP EED PM EE EER RM X UU UI |
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| Small Core for Radio | FIAS | B FR TP TF LP |
- | - | ||||
| Common Mode Choke Coil | SUPER- FIAS |
FR EE EI |
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4-3.Heat Generation Analysis System |
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Thanks to the development of the ferrite material design system and the general-purpose three-dimensional magnetic field analysis system, we are now able to determine the safe designs of various magnetic components, including deflection yokes and FBT ferrite cores. Especially in the case of deflection yokes and FBT ferrite cores, which are TV components, the prevention of excessive heat generation from coils is of crucial importance, since TVs operate with a large amount of electric power. By building up heat dissipation data bases in relation to the ambient conditions, coil conditions, component materials, and circuit layouts and by utilizing a load simulation system for ferrite cores, we have enabled the simulation of heat generation in magnetic components. Figure 8 shows a the simulated flux distribution inside a ferrite core for a 49cm-size display, when electricity of fH = 64 kHz and fV = 64 Hz is applied. Figure 9 shows the simulated heat distribution in that core, with the sizes of the core and coil reduced to one-fourth scale. |
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5.CONCLUSION |
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The first ferrites were invented in Japan about 60 years ago. Over the past ten years or so, we have rapidly increased our know-how in selecting the most suitable ferrite materials from a vast selection, a result of improved computer technology. To our delight, computer simulation has realized two-way design communication in which the maker designs ferrite materials in response to customer needs. Our CAE technology is also applied to the design of CRTs for Hi-Vision and other large-screen television receivers. With the CAE technology, new ferrite materials are being developed while constantly referring to customer needs. Our current challenge is to construct data bases intended for the design simulation of host equipment as well as of components. This should bring about an even higher level of simulation accuracy. |
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