IP Library Granted Patent US 10,241,850
Granted Patent B2
US 10,241,850 · App. 14/459,096 · Granted Mar 26, 2019

Non-magnetodielectric flux concentrator

Inventor: Matthew J. Holcomb (Metamora, MI)
Assignee: Grid Logic Incorporated
G06F11/073B29C64/153H05B6/101H05B6/40B33Y10/00B33Y30/00
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Quick Facts
Patent No.
US 10,241,850
App. No.
14/459,096
Granted
Mar 26, 2019
Kind
B2
Abstract

The invention also provides a heating apparatus including a holder capable of holding at least one part, an electric current generator and a flux concentrator electrically connected to the electric current generator, the flux concentrator being made of a non-magneto-dielectric material and having a coil with at least one turn forming an inductor to generate an alternating magnetic field that is driven by the alternating electric field, the alternating magnetic field resonating at a frequency of at least 1 MHz in response to the alternating electric current.

Claims (158)

1. A heating method comprising:

holding a flux concentrator and at least one part in proximity to one another; and

generating an alternating electric current, the flux concentrator comprising a plate of non-magnetodielectric material, the plate having a slot and a hole at an end of the slot, the hole defining the single turn having a diameter of less than 10 mm forming an inductor to generate an alternating magnetic field that is driven by the alternating electric current, the alternating magnetic field resonating at a high frequency of at least 1 MHz that is selected such that d/δ is at least 4, wherein

δ

=

ρ

π

f

μ

ρ is the resistivity and μ is the permeability of the material,

μ is the permeability of the material;

f is the frequency of the magnetic field, and

d is an outer dimension of the part.

2. The method of claim 1 , wherein d/δ is at least 4, wherein the part is a spherical particle with an axis aligned with a flux field in line of the magnetic field through the spherical particle, wherein:

d/δ is at least 6 at an equator of the spherical particle; and

d/δ is at least 6 at poles of the spherical particle.

3. The method of claim 2 , the coil having a diameter and a thickness, wherein the diameter is less than 10 mm and the alternating magnetic field has a toroidal shape with a cross-section of revolution forming a circle, the circle having a diameter of less than 50 percent of the diameter of the coil.

4. The method of claim 1 , wherein the flux concentrator has a magnetic flux density of at least 1 mT at 0.5 mm.

5. The method of claim 1 , wherein the coil has an inductance of less than 5 nH.

6. The method of claim 1 , wherein the part is between 45 and 55 percent of a diameter of the coil from the coil.

7. The method of claim 1 , further comprising:

collecting and releasing a charge with at least one capacitor in parallel with the inductor to form a tank circuit.

8. The method of claim 7 , further comprising:

a plate, wherein a plurality of capacitors are mounted to the plate in parallel with the inductor.

9. The method of claim 7 , wherein the tank circuit has a resonant frequency f R , wherein

f

R

=

1

2

π

L

C

where:

L is the inductance of the coil; and

C is the capacitor of the at least one capacitor.

10. The method of claim 1 , wherein the coil is a high frequency coil, further comprising:

pre-heating the part with a low frequency coil.

11. The method of claim 1 , further comprising:

monitoring coupling of the alternating magnetic field to the part by monitoring a normalized voltage standing wave (VSWR) ratio θ as:

θ

=

1

-

(

V

S

W

R

K

>

0

V

S

W

R

K

=

0

)

where VSWR K>0 is the VSWR of circuit having the coil when it is coupled to the powder bed, and VSWR K=0 is the VSWR of the circuit when it is completely de-coupled from the powder bed.

12. A heating method comprising:

holding a flux concentrator and at least one part in proximity to one another; and

generating an alternating electric current, the flux concentrator being made of a non-magnetodielectric material and having a coil with at least one turn having a diameter of less than 10 mm forming an inductor to generate an alternating magnetic field that is driven by the alternating electric current, the alternating magnetic field resonating at a high frequency of at least 1 MHz that is selected such that d/δ is at least 4, wherein

δ

=

ρ

π

f

μ

ρ is the resistivity and μ is the permeability of the material,

μ is the permeability of the material;

f is the frequency of the magnetic field, and

d is an outer dimension of the part; and

monitoring coupling of the alternating magnetic field to the part by monitoring a normalized voltage standing wave (VSWR) ratio θ as:

θ

=

1

-

(

V

S

W

R

K

>

0

V

S

W

R

K

=

0

)

where VSWR K>0 is the VSWR of circuit having the coil when it is coupled to the powder bed, and VSWR K=0 is the VSWR of the circuit when it is completely de-coupled from the powder bed.

13. The method of claim 12 , wherein d/δ is at least 4, wherein the part is a spherical particle with an axis aligned with a flux field in line of the magnetic field through the spherical particle, wherein:

d/δ is at least 6 at an equator of the spherical particle; and

d/δ is at least 6 at poles of the spherical particle.

14. The method of claim 13 , the coil having a diameter and a thickness, wherein the diameter is less than 10 mm and the alternating magnetic field has a toroidal shape with a cross-section of revolution forming a circle, the circle having a diameter of less than 50 percent of the diameter of the coil.

15. The method of claim 12 , wherein the flux concentrator has a magnetic flux density of at least 1 mT at 0.5 mm.

16. The method of claim 12 , wherein the coil has an inductance of less than 5 nH.

17. The method of claim 12 , wherein the part is between 45 and 55 percent of a diameter of the coil from the coil.

18. The method of claim 12 , further comprising:

collecting and releasing a charge with at least one capacitor in parallel with the inductor to form a tank circuit.

19. The method of claim 18 , wherein a plurality of capacitors are mounted to the plate in parallel with the inductor.

20. The method of claim 18 , wherein the tank circuit has a resonant frequency f R , wherein

f

R

=

1

2

π

L

C

where:

L is the inductance of the coil; and

C is the capacitor of the at least one capacitor.

21. The method of claim 12 , wherein the coil has only a single turn.

22. The method of claim 21 , wherein the flux concentrator comprises a plate of non-magnetodielectric material, the plate having a slot and a hole at an end of the slot, the hole defining the single turn.

23. The method of claim 12 , wherein the coil is a high frequency coil, further comprising:

pre-heating the part with a low frequency coil.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 20, 2014
From: HOLCOMB, MATTHEW J
To: GRID LOGIC INCORPORATED
Reel/Frame 033571/0129 →
Continuity (6)
Provisional Application 61977395 · Apr 9, 2014
Provisional Application 61885806 · Oct 2, 2013
Provisional Application 61896896 · Oct 29, 2013
Provisional Application 61898054 · Oct 31, 2013
Related Publication 20150296571A1 · Oct 15, 2015
Related Publication 20180343706A9 · Nov 29, 2018