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Heavy Wall Pipe Seam Annealing            Page 1                                 HES 2004


             New Magnetodielectric Materials for Magnetic Flux Control

                                  Mr. Robert T. Ruffini
                              Fluxtrol Manufacturing, Inc.
                    1388 Atlantic Blvd., Auburn Hills, MI 48326 USA
                       Phone +1 248 393 2202, www.fluxtrol.com

                      Dr. Valentin Nemkov, Dr. Nina Vyshinskaya
                          Centre for Induction Technology, Inc.
                    1388 Atlantic Blvd., Auburn Hills, MI 48326 USA
                       Phone +1 248 393 2200, www.induction.org

ABSTRACT
   Magnetodielectric materials play an important role in improvement of induction
systems for heat treatment, brazing, soldering, sealing and other technologies. This
presentation is a continuation of the report made at HIS-01. Current report shows the
results of development of new magnetodielectric materials for magnetic flux control and
intensive study of their properties.
   Presentation contains information on new MagnetoDielectric Materials (MDM’s)
Fluxtrol 25, Fluxtrol 50 and a third new material developed specifically for low
frequency (less than 10 kHz) applications. It is shown that some magnetodielectric
materials have significant property anisotropy. This anisotropy may be beneficially used
for optimal design of magnetic flux controllers. A presentation is accompanied by table-
top exhibition with samples of magnetodielectric materials and inductors with magnetic
flux controllers.

INTRODUCTION
   There are four main families of electromagnetic applications where soft magnetic
materials are used: electromechanical devices, low frequency industrial applications, high
frequency industrial applications, and telecommunications. Figure 1 shows the common
frequency ranges of different electromagnetic applications. The requirements for soft
magnetic materials are quite different depending upon the type of application.
   Electromechanical devices consist mainly of electrical motors, relays, solenoid and
drives, which generally work at frequencies between DC and several hundred hertz.
These products are typically relatively high volume (thousands of parts) and warrant
specific tooling for manufacturing.         The main requirements to materials in
electromagnetic devices are high permeability, high saturation flux density, low core
losses (if AC) and good mechanical strength. The core losses for these materials are
typically due to hysteresis losses.
   The low frequency industrial applications that utilize soft magnetic materials are
typically large induction installations for melting, mass heating, forging, etc. In these
applications, the processing temperature is high and the magnetic materials must be in
close proximity to the load. The frequency range for these applications is typically
between 50 Hz and 3 kHz. The number of installations of a given type is relatively small
due to the huge production rates and the shape of soft magnetic materials required varies.
The main requirements to materials in low frequency industrial applications are high
Heavy Wall Pipe Seam Annealing                               Page 2                          HES 2004


permeability, high saturation flux density, low core losses and good temperature
resistance.
   Communications applications often use soft magnetic materials for radio electronics
transformers, chokes, antennas and other devices. The frequency range for these
applications is above 500 kHz to several GHz. These applications typically are very high
volume and the shapes used are relatively simple.
   The high frequency industrial applications that use soft magnetic materials consist
mainly of a wide variety of induction heating processes including heat treating, small
quantity or low conductive material (ie glass) melting, preheating, joining, etc. This
family of applications is much more diverse than the low frequency industrial
applications. In addition, each of these applications require special know-how for proper
electromagnetic system design. The following sections discuss the role of soft magnetic
materials, the materials available and considerations for their use that must be taken into
account when working in this area of application with special attention paid to
magnetodielectric materials.


                                  Frequency Ranges for Different EM Applications

                                100000


                                 10000                            Communications
                                  1000
                                                                  High Frequency
              Frequency (kHz)




                                   100


                                    10                            Low Frequency
                                                                  Induction
                                     1
                                                                  Electromechanical
                                   0.1
                                                                  Devices
                                  0.01
                                              Applications




                                Figure 1 Frequency ranges for electromagnetic applications

ROLE OF MAGNETIC FLUX CONTROLLERS
   Magnetic flux controllers are a powerful tool in induction heating technology [1].
Recently, better understanding of their role in different induction heating systems has
been obtained through a comprehensive study using computer simulation and
experiments at Centre for Induction Technology, Inc. The results of this study show that
the proper use of a magnetic flux controller is always beneficial in an induction heating
system [1]. They can play different roles in induction heating installations and in various
applications are being named as concentrators, controllers, diverters, cores, impeders or
screens.
   Magnetic flux controllers may provide the following effects:
 improvement of the induction coil and process efficiency;
 improvement of the coil power factor;
 protection of machine components and certain workpiece zones against unwanted
    heating;
Heavy Wall Pipe Seam Annealing             Page 3                                                            HES 2004


                                                 precise control of the magnetic field and the resulting heat pattern
                                                 improvement in efficiency of the high frequency power supplying circuitry;
                                                 elimination of external magnetic fields in close proximity to the coil.
                                                 In most real applications more than one of these benefits usually occur. For processes
                                              such as case hardening, tempering or brazing where the results are very critical to
                                              operating conditions of heating process, quality improvement is usually the most
                                              important. Application of magnetic flux controllers strongly influences the power density
                                              value and its distribution along the surface of the workpiece enabling faster heating and
                                              better heat pattern control. In addition to improvements in metallurgical results and
                                              physical properties of parts, heat pattern control allows you to control stresses and
                                              strongly reduce part distortion.
                                                 To illustrate how magnetic flux controllers may be used in the optimal design of an
                                              induction heating process, we’ll describe shortly a real world installation for stress
                                              relieving of spiral welded heavy walled steel pipe for the oil and gas industry. The
                                              induction heating user purchased an installation for weld seam annealing on large
                                              diameter seam annealing (T>900 C) after arc spiral welding (figure 2). The unit was
                                              working fine for its intended application. Then, the specifications for the tube heat
                                              treatment were changed. Instead of full annealing of the weld seam, the process required
                                              was specified as a high temperature stress relieving (550-650 C) and the Heat Affected
                                              Zone (HAZ) was widened from 30 mm to 60 mm.

stluseR edahS roloC                                                                                                          Color Shade Results
  s uisleC . geD er utarepmeT : ytit na uQ                                                                           Quantity : Temperature Deg. Celsius

         0 :) geD( esa hP 71 : ).s( emiT                                                                             Time (s.) : 17 Phase (Deg): 0
                            r ol oC / elacS                                                                          Scale / Color
                75 2 7 3. 27 / 2 02 3.3 2                                                                            23.3202 / 72.37257
            3 9 42 4.1 2 1 / 7 5 27 3.2 7                                                                            72.37257 / 121.42493
          92 7 74. 07 1 / 39 4 24. 12 1                                                                              121.42493 / 170.47729
          66 9 25. 91 2 / 92 7 74. 07 1                                                                              170.47729 / 219.52966
          30 2 85. 86 2 / 66 9 25. 91 2                                                                              219.52966 / 268.58203
            4 4 36. 71 3 / 30 2 85. 86 2                                                                             268.58203 / 317.6344
            4 7 68 6.6 6 3 / 4 4 36. 71 3                                                                            317.6344 / 366.68674
          11 9 37. 51 4 / 47 6 86. 66 3                                                                              366.68674 / 415.73911
          74 1 97. 46 4 / 11 9 37. 51 4                                                                              415.73911 / 464.79147
          78 3 48. 31 5 / 74 1 97. 46 4                                                                              464.79147 / 513.84387
          81 6 98. 26 5 / 78 3 48. 31 5                                                                              513.84387 / 562.89618
          55 8 49. 11 6 / 81 6 98. 26 5                                                                              562.89618 / 611.94855
          29 0 00. 16 6 / 55 8 49. 11 6                                                                              611.94855 / 661.00092
          82 3 50. 01 7 / 29 0 00. 16 6                                                                              661.00092 / 710.05328
          56 5 01. 95 7 / 82 3 50. 01 7                                                                              710.05328 / 759.10565
          20 8 51. 80 8 / 56 5 01. 95 7                                                                              759.10565 / 808.15802




                                                  Figure 2.    Final temperature distribution for the weld seam stress relieving process
                                                                    using the same coil as for weld seam annealing

                                                 When the user tried to set up the new process, they found two things: the heat affected
                                              zone was too narrow and they were not able to get the inside of the weld seam up to the
                                              specified temperature without overheating the surface and there was no space for a longer
                                              coil. They tried slowing the process down significantly, but they were still unable to
                                              meet the new heat treating specifications. The reason for their difficulties can be easily
                                              explained using computer simulation. Figure 3 shows the color shade of the temperature
                                              distribution at the end of the heating process and the temperature on the inner and outer
                                              weld beads over the course of the process using their seam annealing inductor.
Heavy Wall Pipe Seam Annealing            Page 4                                  HES 2004




    Figure 3. Inner and outer weld bead temperature evolution for the existing stress
                                   relieving process

   Compared to the old process, the pipe is magnetic throughout the entire process so the
induced heat sources flowed only in a shallow surface layer of the workpiece. This
meant that the center of the workpiece was heated entirely by heat conduction from the
surface




   Figure 4. Final temperature distribution and inner and outer weld bead temperature
                      evolution for the optimized coil and process

    To provide the wider HAZ, the turns were separated. The best solution to get the
inside of the weld bead up to temperature is magnetic flux controller variation in the coil
length. Fluxtrol A magnetic flux concentrator was applied for this application. The initial
stage is a ramping to the maximum surface temperature and the full C-shape cross-
section is applied. After the maximum temperature is reached, we begin to cut back
some of the concentrator pole to hold the maximum temperature constant. More
concentrator is removed until the final stage is reached and we have no concentrator at
all. Figure 4 shows the temperature distribution in the weld seam area 6 seconds after the
Heavy Wall Pipe Seam Annealing             Page 5                                  HES 2004


point has left the coil. Figure 4 also shows the temperature on the inner and outer weld
beads over the heating process. You can see that the temperature is uniform in thickness
and in width with the new design.

MATERIALS FOR MAGNETIC FLUX CONTROL
   Requirements for magnetic flux contolling materials in induction heating processes
can be very severe in many cases. They must work in a very wide range of frequencies,
possess high permeabilities and saturation flux densities, have stable mechanical
properties and exhibit resistance to elevated temperatures from losses in the concentrator
and radiation from the heated part surface. In heat treating and brazing, the material must
withstand hot water attack, quenchants and active technological fluxes. Machinability is
also a very important property for successful application of flux controllers, because it
allows you to obtain the exact concentrator dimensions necessary to assure consistent
results and precise magnetic field control.
   As was discussed above, there is a very wide range of requirements for the various
induction heating applications and therefore more than one magnetic flux controlling
material is required to cover the whole range. Three groups of magnetic materials may
be used for magnetic flux control: laminations, ferrites and MagnetoDielectric Materials
(MDM) [2]. Laminations have long been used in electromagnetic systems and their
abilities and limitations, especially in manufacturing and frequency, are well
documented. The use of ferrites relatively uncommon in induction heating due to very
low machinability, sensitivity to thermal shock, and low saturation flux density. MDM’s
are well suited to induction requirements and have the potential for use in the entire
application range.

Special Properties of MDM’s
   MDM’s are an evolving material class and there is currently rapid progress in their
improvement and understanding. They have some special properties, that when properly
utilized, can lead to significant induction system parameter improvement. Two of these
properties that have not been adequately discussed before are electrical resistivity and
anisotropy.
   MDM’s are a wide family of materials ranging from good dielectrics to traditional
powder metal magnetics. Electrical resistivity is an important parameter of the material
which is contradictory to magnetic permeability. The higher the permeability is, the
lower the electrical resistivity when using the same materials and manufacturing
technology. The nature and proper evaluation of electrical resistivity are rather
complicated. At DC current and 50/60 Hz there are only galvanic currents due to random
contact between individual metal particles and defects of insulation layers. The resulting
resistivity is non-linear with declining values as applied voltage is increased. This effect
is especially strong for high-resistive, low permeability materials. At high frequency
(hundreds kHz) additional capacitive currents can result in a higher value of measured
resistivity.
   It is necessary to underline that electrical resistivity does not characterize correctly
losses in material. When using computer simulation, we calculate losses in concentrator
due to its electrical resistivity, those are only a fraction of total losses caused by
hysteresis and eddy-currents in individual particles of the composite. In properly
designed induction coils with concentrators, they are a small fraction of total magnetic
Heavy Wall Pipe Seam Annealing                        Page 6                               HES 2004


losses. Proper understanding of electrical properties of MDM is essential for prediction of
its performance under application conditions.
    Similar to electrical resistivity, anisotropy of MDM’s is also not well described in
literature. All pressed metal powder materials have certain anisotropy in mechanical,
electrical and magnetic properties. This anisotropy is caused by magnetic particle
alignment and deformation during the manufacturing process. Magnetic permeability is
minimal in direction of pressing and maximal in the perpendicular plane. For toroidal
parts, which are widely used in electronics, anisotropy does not play any role while for
induction heating applications it may be essential in many cases. Anisotropy may be
effectively used, especially in 3D magnetic fields in order to reduce field in less desirable
direction. The level of anisotropy depends on material composition, shape of particles
and pressure applied.
    It is more pronounced in high-permeability materials such as Fluxtrol A and the new
low frequency material manufactured by Fluxtrol Manufacturing, Inc. The difference in
permeability may be up to two times. Besides permeability, other properties essential for
successful concentrator application are also directionally dependent including thermal
conductivity and magnetic losses. For advice related to anisotropy of materials, please
contact Fluxtrol Manufacturing, Inc.

MDM’s for Magnetic Flux Control
   Since the HIS ’01 conference, Fluxtrol Manufacturing, Inc. has introduced 3 new
materials for magnetic flux control in induction systems. These new materials are
Fluxtrol 25, Fluxtrol 50, and a new low frequency material. The magnetization curves
for the main materials manufactured by Fluxtrol are shown in Figure 5. The curves of the
resulting relative magnetic permeability for these materials are shown in Figure 6.


                                             B vs H

           18000

           16000
                                                                           New LF
           14000
                                                                           Material
           12000
                                                                           Fluxtrol A
           10000
   B, Gs




            8000                                                           Fluxtrol 50
            6000
                                                                           Fluxtrol 25
            4000

            2000                                                           Ferrotron 559
              0
                   0   25   50   75   100   125   150   175    200   225

                                      H, A/cm



  Figure 5. Magnetization curves for MDM’s manufactured by Fluxtrol Manufacturing,
                                        Inc.
Heavy Wall Pipe Seam Annealing                                    Page 7                              HES 2004




                                            Permeability vs H

                  180

                  160

                  140

                  120                                                                   New LF
   Permeability




                                                                                        Material
                  100                                                                   Fluxtrol A

                  80                                                                    Fluxtrol 50

                  60                                                                    Fluxtrol 25

                  40                                                                    Ferrotron
                                                                                        559
                  20

                   0
                        0   20   40   60   80     100     120   140   160   180   200

                                                H, A/cm




     Figure 6. Permeabilities of MDM’s manufactured by Fluxtrol Manufacturing, Inc.

   The nomenclature for the new materials in the Fluxtrol family is based upon the
normal “working permeability” of the materials. The magnetic permeability of MDM’s
depends upon the magnetic field strength. The general trend is that the permeability
increases with field strength until reaching a maximum value and then the permeability
declines. For higher frequency MDM’s, this distribution is relatively smooth. The
“working permeability” is an average value of the permeability in the normal range of
field strengths the material was designed to work in.
   Fluxtrol 25 is a material that was designed to replace Fluxtrol B in medium and high
frequency applications (20 kHz to 500 kHz). The magnetic properties of Fluxtrol 25 are
the same as those of Fluxtrol B, making it possible for direct replacement. Fluxtrol 25
has improved temperataure resistance (250 C long term and 300 C short term compared
to 200 C long term and 250 C short term for Fluxtrol B), making it more reliable in heavy
duty applications, while maintaining its excellent machinability.
   Fluxtrol 50 is a material that was designed to fill a gap that was not currently covered
in Fluxtrol’s old product line. Fluxtrol 50 has high enough permeability for effective use
in low frequency applications (working permeability around 50, but it can also be used in
higher frequency applications (60 Hz to 500 kHz) and. Fluxtrol 50 has the same
temperature resistance as Fluxtrol 25. Fluxtrol 50 has very good machinability and is
relatively strong even in thin sections (1.5 – 2 mm).
   The other new material that is currently available was designed for use in low
frequency applications, such as mass heating, melting and continuous casting. The new
low frequency material has a lower price than the materials in the Fluxtrol and Ferrotron
families. This makes it cost effective in most cases to use it as a replacement for
laminations.
Heavy Wall Pipe Seam Annealing             Page 8                                  HES 2004


CONCLUSIONS
   Induction applications provide many challenges for soft magnetic materials. These
applications are typically low volume and there is a great degree of variation in process
type and material requirements. This makes properties such as machinability and
chemical stability more important than in other electromagnetic applications.
   MagnetoDielectric Materials (MDM’s) are a type of soft magnetic material that are
gaining increased acceptance in induction applications. They have special properties,
which make them very favorable for induction heating conditions. At the same time, the
specific features of these materials are not as well understood as for other soft magnetic
materials. Two of these properties, electrical resistivity and anisotropy, were discussed in
this paper.
   Since HIS ’01, Fluxtrol Manufacturing, Inc. has introduced 3 new materials for
magnetic flux control in induction heating systems: Fluxtrol 25, Fluxtrol 50 and a new
material for low frequency applications. These new materials have superior properties to
other soft magnetic materials in many applications.

REFERENCES
[1] Ruffini, R. T., Nemkov, V. S., Goldstein, R. C. Magnetic Flux Controllers-New
Materials, New Opportunities. ASTRA 2003. November 3–6, 2003. Hyderabad, India
[2] Nemkov V.S., Goldstein, R. C., Ruffini, R. T. Soft Magnetic Powdered Metal
Materials for High Frequency Industrial Applications. PMTec 2001. May 13-17, 2001.
New Orleans, La-USA.

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New Magnetodielectric Materials for Magnetic Flux Control in Induction Heating Systems

  • 1. Heavy Wall Pipe Seam Annealing Page 1 HES 2004 New Magnetodielectric Materials for Magnetic Flux Control Mr. Robert T. Ruffini Fluxtrol Manufacturing, Inc. 1388 Atlantic Blvd., Auburn Hills, MI 48326 USA Phone +1 248 393 2202, www.fluxtrol.com Dr. Valentin Nemkov, Dr. Nina Vyshinskaya Centre for Induction Technology, Inc. 1388 Atlantic Blvd., Auburn Hills, MI 48326 USA Phone +1 248 393 2200, www.induction.org ABSTRACT Magnetodielectric materials play an important role in improvement of induction systems for heat treatment, brazing, soldering, sealing and other technologies. This presentation is a continuation of the report made at HIS-01. Current report shows the results of development of new magnetodielectric materials for magnetic flux control and intensive study of their properties. Presentation contains information on new MagnetoDielectric Materials (MDM’s) Fluxtrol 25, Fluxtrol 50 and a third new material developed specifically for low frequency (less than 10 kHz) applications. It is shown that some magnetodielectric materials have significant property anisotropy. This anisotropy may be beneficially used for optimal design of magnetic flux controllers. A presentation is accompanied by table- top exhibition with samples of magnetodielectric materials and inductors with magnetic flux controllers. INTRODUCTION There are four main families of electromagnetic applications where soft magnetic materials are used: electromechanical devices, low frequency industrial applications, high frequency industrial applications, and telecommunications. Figure 1 shows the common frequency ranges of different electromagnetic applications. The requirements for soft magnetic materials are quite different depending upon the type of application. Electromechanical devices consist mainly of electrical motors, relays, solenoid and drives, which generally work at frequencies between DC and several hundred hertz. These products are typically relatively high volume (thousands of parts) and warrant specific tooling for manufacturing. The main requirements to materials in electromagnetic devices are high permeability, high saturation flux density, low core losses (if AC) and good mechanical strength. The core losses for these materials are typically due to hysteresis losses. The low frequency industrial applications that utilize soft magnetic materials are typically large induction installations for melting, mass heating, forging, etc. In these applications, the processing temperature is high and the magnetic materials must be in close proximity to the load. The frequency range for these applications is typically between 50 Hz and 3 kHz. The number of installations of a given type is relatively small due to the huge production rates and the shape of soft magnetic materials required varies. The main requirements to materials in low frequency industrial applications are high
  • 2. Heavy Wall Pipe Seam Annealing Page 2 HES 2004 permeability, high saturation flux density, low core losses and good temperature resistance. Communications applications often use soft magnetic materials for radio electronics transformers, chokes, antennas and other devices. The frequency range for these applications is above 500 kHz to several GHz. These applications typically are very high volume and the shapes used are relatively simple. The high frequency industrial applications that use soft magnetic materials consist mainly of a wide variety of induction heating processes including heat treating, small quantity or low conductive material (ie glass) melting, preheating, joining, etc. This family of applications is much more diverse than the low frequency industrial applications. In addition, each of these applications require special know-how for proper electromagnetic system design. The following sections discuss the role of soft magnetic materials, the materials available and considerations for their use that must be taken into account when working in this area of application with special attention paid to magnetodielectric materials. Frequency Ranges for Different EM Applications 100000 10000 Communications 1000 High Frequency Frequency (kHz) 100 10 Low Frequency Induction 1 Electromechanical 0.1 Devices 0.01 Applications Figure 1 Frequency ranges for electromagnetic applications ROLE OF MAGNETIC FLUX CONTROLLERS Magnetic flux controllers are a powerful tool in induction heating technology [1]. Recently, better understanding of their role in different induction heating systems has been obtained through a comprehensive study using computer simulation and experiments at Centre for Induction Technology, Inc. The results of this study show that the proper use of a magnetic flux controller is always beneficial in an induction heating system [1]. They can play different roles in induction heating installations and in various applications are being named as concentrators, controllers, diverters, cores, impeders or screens. Magnetic flux controllers may provide the following effects:  improvement of the induction coil and process efficiency;  improvement of the coil power factor;  protection of machine components and certain workpiece zones against unwanted heating;
  • 3. Heavy Wall Pipe Seam Annealing Page 3 HES 2004  precise control of the magnetic field and the resulting heat pattern  improvement in efficiency of the high frequency power supplying circuitry;  elimination of external magnetic fields in close proximity to the coil. In most real applications more than one of these benefits usually occur. For processes such as case hardening, tempering or brazing where the results are very critical to operating conditions of heating process, quality improvement is usually the most important. Application of magnetic flux controllers strongly influences the power density value and its distribution along the surface of the workpiece enabling faster heating and better heat pattern control. In addition to improvements in metallurgical results and physical properties of parts, heat pattern control allows you to control stresses and strongly reduce part distortion. To illustrate how magnetic flux controllers may be used in the optimal design of an induction heating process, we’ll describe shortly a real world installation for stress relieving of spiral welded heavy walled steel pipe for the oil and gas industry. The induction heating user purchased an installation for weld seam annealing on large diameter seam annealing (T>900 C) after arc spiral welding (figure 2). The unit was working fine for its intended application. Then, the specifications for the tube heat treatment were changed. Instead of full annealing of the weld seam, the process required was specified as a high temperature stress relieving (550-650 C) and the Heat Affected Zone (HAZ) was widened from 30 mm to 60 mm. stluseR edahS roloC Color Shade Results s uisleC . geD er utarepmeT : ytit na uQ Quantity : Temperature Deg. Celsius 0 :) geD( esa hP 71 : ).s( emiT Time (s.) : 17 Phase (Deg): 0 r ol oC / elacS Scale / Color 75 2 7 3. 27 / 2 02 3.3 2 23.3202 / 72.37257 3 9 42 4.1 2 1 / 7 5 27 3.2 7 72.37257 / 121.42493 92 7 74. 07 1 / 39 4 24. 12 1 121.42493 / 170.47729 66 9 25. 91 2 / 92 7 74. 07 1 170.47729 / 219.52966 30 2 85. 86 2 / 66 9 25. 91 2 219.52966 / 268.58203 4 4 36. 71 3 / 30 2 85. 86 2 268.58203 / 317.6344 4 7 68 6.6 6 3 / 4 4 36. 71 3 317.6344 / 366.68674 11 9 37. 51 4 / 47 6 86. 66 3 366.68674 / 415.73911 74 1 97. 46 4 / 11 9 37. 51 4 415.73911 / 464.79147 78 3 48. 31 5 / 74 1 97. 46 4 464.79147 / 513.84387 81 6 98. 26 5 / 78 3 48. 31 5 513.84387 / 562.89618 55 8 49. 11 6 / 81 6 98. 26 5 562.89618 / 611.94855 29 0 00. 16 6 / 55 8 49. 11 6 611.94855 / 661.00092 82 3 50. 01 7 / 29 0 00. 16 6 661.00092 / 710.05328 56 5 01. 95 7 / 82 3 50. 01 7 710.05328 / 759.10565 20 8 51. 80 8 / 56 5 01. 95 7 759.10565 / 808.15802 Figure 2. Final temperature distribution for the weld seam stress relieving process using the same coil as for weld seam annealing When the user tried to set up the new process, they found two things: the heat affected zone was too narrow and they were not able to get the inside of the weld seam up to the specified temperature without overheating the surface and there was no space for a longer coil. They tried slowing the process down significantly, but they were still unable to meet the new heat treating specifications. The reason for their difficulties can be easily explained using computer simulation. Figure 3 shows the color shade of the temperature distribution at the end of the heating process and the temperature on the inner and outer weld beads over the course of the process using their seam annealing inductor.
  • 4. Heavy Wall Pipe Seam Annealing Page 4 HES 2004 Figure 3. Inner and outer weld bead temperature evolution for the existing stress relieving process Compared to the old process, the pipe is magnetic throughout the entire process so the induced heat sources flowed only in a shallow surface layer of the workpiece. This meant that the center of the workpiece was heated entirely by heat conduction from the surface Figure 4. Final temperature distribution and inner and outer weld bead temperature evolution for the optimized coil and process To provide the wider HAZ, the turns were separated. The best solution to get the inside of the weld bead up to temperature is magnetic flux controller variation in the coil length. Fluxtrol A magnetic flux concentrator was applied for this application. The initial stage is a ramping to the maximum surface temperature and the full C-shape cross- section is applied. After the maximum temperature is reached, we begin to cut back some of the concentrator pole to hold the maximum temperature constant. More concentrator is removed until the final stage is reached and we have no concentrator at all. Figure 4 shows the temperature distribution in the weld seam area 6 seconds after the
  • 5. Heavy Wall Pipe Seam Annealing Page 5 HES 2004 point has left the coil. Figure 4 also shows the temperature on the inner and outer weld beads over the heating process. You can see that the temperature is uniform in thickness and in width with the new design. MATERIALS FOR MAGNETIC FLUX CONTROL Requirements for magnetic flux contolling materials in induction heating processes can be very severe in many cases. They must work in a very wide range of frequencies, possess high permeabilities and saturation flux densities, have stable mechanical properties and exhibit resistance to elevated temperatures from losses in the concentrator and radiation from the heated part surface. In heat treating and brazing, the material must withstand hot water attack, quenchants and active technological fluxes. Machinability is also a very important property for successful application of flux controllers, because it allows you to obtain the exact concentrator dimensions necessary to assure consistent results and precise magnetic field control. As was discussed above, there is a very wide range of requirements for the various induction heating applications and therefore more than one magnetic flux controlling material is required to cover the whole range. Three groups of magnetic materials may be used for magnetic flux control: laminations, ferrites and MagnetoDielectric Materials (MDM) [2]. Laminations have long been used in electromagnetic systems and their abilities and limitations, especially in manufacturing and frequency, are well documented. The use of ferrites relatively uncommon in induction heating due to very low machinability, sensitivity to thermal shock, and low saturation flux density. MDM’s are well suited to induction requirements and have the potential for use in the entire application range. Special Properties of MDM’s MDM’s are an evolving material class and there is currently rapid progress in their improvement and understanding. They have some special properties, that when properly utilized, can lead to significant induction system parameter improvement. Two of these properties that have not been adequately discussed before are electrical resistivity and anisotropy. MDM’s are a wide family of materials ranging from good dielectrics to traditional powder metal magnetics. Electrical resistivity is an important parameter of the material which is contradictory to magnetic permeability. The higher the permeability is, the lower the electrical resistivity when using the same materials and manufacturing technology. The nature and proper evaluation of electrical resistivity are rather complicated. At DC current and 50/60 Hz there are only galvanic currents due to random contact between individual metal particles and defects of insulation layers. The resulting resistivity is non-linear with declining values as applied voltage is increased. This effect is especially strong for high-resistive, low permeability materials. At high frequency (hundreds kHz) additional capacitive currents can result in a higher value of measured resistivity. It is necessary to underline that electrical resistivity does not characterize correctly losses in material. When using computer simulation, we calculate losses in concentrator due to its electrical resistivity, those are only a fraction of total losses caused by hysteresis and eddy-currents in individual particles of the composite. In properly designed induction coils with concentrators, they are a small fraction of total magnetic
  • 6. Heavy Wall Pipe Seam Annealing Page 6 HES 2004 losses. Proper understanding of electrical properties of MDM is essential for prediction of its performance under application conditions. Similar to electrical resistivity, anisotropy of MDM’s is also not well described in literature. All pressed metal powder materials have certain anisotropy in mechanical, electrical and magnetic properties. This anisotropy is caused by magnetic particle alignment and deformation during the manufacturing process. Magnetic permeability is minimal in direction of pressing and maximal in the perpendicular plane. For toroidal parts, which are widely used in electronics, anisotropy does not play any role while for induction heating applications it may be essential in many cases. Anisotropy may be effectively used, especially in 3D magnetic fields in order to reduce field in less desirable direction. The level of anisotropy depends on material composition, shape of particles and pressure applied. It is more pronounced in high-permeability materials such as Fluxtrol A and the new low frequency material manufactured by Fluxtrol Manufacturing, Inc. The difference in permeability may be up to two times. Besides permeability, other properties essential for successful concentrator application are also directionally dependent including thermal conductivity and magnetic losses. For advice related to anisotropy of materials, please contact Fluxtrol Manufacturing, Inc. MDM’s for Magnetic Flux Control Since the HIS ’01 conference, Fluxtrol Manufacturing, Inc. has introduced 3 new materials for magnetic flux control in induction systems. These new materials are Fluxtrol 25, Fluxtrol 50, and a new low frequency material. The magnetization curves for the main materials manufactured by Fluxtrol are shown in Figure 5. The curves of the resulting relative magnetic permeability for these materials are shown in Figure 6. B vs H 18000 16000 New LF 14000 Material 12000 Fluxtrol A 10000 B, Gs 8000 Fluxtrol 50 6000 Fluxtrol 25 4000 2000 Ferrotron 559 0 0 25 50 75 100 125 150 175 200 225 H, A/cm Figure 5. Magnetization curves for MDM’s manufactured by Fluxtrol Manufacturing, Inc.
  • 7. Heavy Wall Pipe Seam Annealing Page 7 HES 2004 Permeability vs H 180 160 140 120 New LF Permeability Material 100 Fluxtrol A 80 Fluxtrol 50 60 Fluxtrol 25 40 Ferrotron 559 20 0 0 20 40 60 80 100 120 140 160 180 200 H, A/cm Figure 6. Permeabilities of MDM’s manufactured by Fluxtrol Manufacturing, Inc. The nomenclature for the new materials in the Fluxtrol family is based upon the normal “working permeability” of the materials. The magnetic permeability of MDM’s depends upon the magnetic field strength. The general trend is that the permeability increases with field strength until reaching a maximum value and then the permeability declines. For higher frequency MDM’s, this distribution is relatively smooth. The “working permeability” is an average value of the permeability in the normal range of field strengths the material was designed to work in. Fluxtrol 25 is a material that was designed to replace Fluxtrol B in medium and high frequency applications (20 kHz to 500 kHz). The magnetic properties of Fluxtrol 25 are the same as those of Fluxtrol B, making it possible for direct replacement. Fluxtrol 25 has improved temperataure resistance (250 C long term and 300 C short term compared to 200 C long term and 250 C short term for Fluxtrol B), making it more reliable in heavy duty applications, while maintaining its excellent machinability. Fluxtrol 50 is a material that was designed to fill a gap that was not currently covered in Fluxtrol’s old product line. Fluxtrol 50 has high enough permeability for effective use in low frequency applications (working permeability around 50, but it can also be used in higher frequency applications (60 Hz to 500 kHz) and. Fluxtrol 50 has the same temperature resistance as Fluxtrol 25. Fluxtrol 50 has very good machinability and is relatively strong even in thin sections (1.5 – 2 mm). The other new material that is currently available was designed for use in low frequency applications, such as mass heating, melting and continuous casting. The new low frequency material has a lower price than the materials in the Fluxtrol and Ferrotron families. This makes it cost effective in most cases to use it as a replacement for laminations.
  • 8. Heavy Wall Pipe Seam Annealing Page 8 HES 2004 CONCLUSIONS Induction applications provide many challenges for soft magnetic materials. These applications are typically low volume and there is a great degree of variation in process type and material requirements. This makes properties such as machinability and chemical stability more important than in other electromagnetic applications. MagnetoDielectric Materials (MDM’s) are a type of soft magnetic material that are gaining increased acceptance in induction applications. They have special properties, which make them very favorable for induction heating conditions. At the same time, the specific features of these materials are not as well understood as for other soft magnetic materials. Two of these properties, electrical resistivity and anisotropy, were discussed in this paper. Since HIS ’01, Fluxtrol Manufacturing, Inc. has introduced 3 new materials for magnetic flux control in induction heating systems: Fluxtrol 25, Fluxtrol 50 and a new material for low frequency applications. These new materials have superior properties to other soft magnetic materials in many applications. REFERENCES [1] Ruffini, R. T., Nemkov, V. S., Goldstein, R. C. Magnetic Flux Controllers-New Materials, New Opportunities. ASTRA 2003. November 3–6, 2003. Hyderabad, India [2] Nemkov V.S., Goldstein, R. C., Ruffini, R. T. Soft Magnetic Powdered Metal Materials for High Frequency Industrial Applications. PMTec 2001. May 13-17, 2001. New Orleans, La-USA.