Method of splitting non-metallic materials

• US 5,609,284 A
• Filed: 09/30/1994
• Issued: 03/11/1997
• Est. Priority Date: 04/02/1992
• Status: Expired due to Fees

• Current Assignee: Litchford & Christopher PA (Baker Donelson Bearman Caldwell & Berkowitz PC)
• Original Assignee: Fonon Technology Limited, UK
• Inventors: Kondratenko, Vladimir S.
• Primary Examiner(s): Jones, Eugenia
• Assistant Examiner(s): Goodman, Charles
• Application Number:
  US08/355,078
• Time in Patent Office: 893 Days
• Field of Search: 225/1, 225/2, 225/93.5, 225/96, 219/121.67, 219/121.72, 219/121.73, 219/121.75
• US Class Current: 225/1
• CPC Class Codes: B23K 2103/50 Inorganic material, e.g. metals, not provided for in B23K2103/02 – B23K2103/26
• CPC Class Codes: B23K 26/0736 into an oval shape, e.g. elliptic shape
• CPC Class Codes: B23K 26/40 taking account of the properties of the material involved
• CPC Class Codes: B26F 3/00 Severing by means other than cutting; Apparatus therefor severing by grinding B24B27/06
• CPC Class Codes: B26F 3/06 Severing by using heat
• CPC Class Codes: C03B 33/091 using at least one focussed radiation beam, e.g. laser beam C03B33/0955 takes precedence
• CPC Class Codes: Y02P 40/57 Improving the yield, e-g- reduction of reject rates
• CPC Class Codes: Y10T 225/10 Methods
• CPC Class Codes: Y10T 225/12 With preliminary weakening
• CPC Class Codes: Y10T 225/304 Including means to apply thermal shock to work
• CPC Class Codes: Y10T 225/321 Preliminary weakener

Abstract

A method of cutting non-metallic materials, specifically glass, resides in the heating of the material by an incident beam of radiation being effected to a temperature short of its softening point, with the rate of relative displacement of the beam and of the material, and the region of the heated zone which is locally cooled being selected to form a blind crack in the material. The method provides for increasing substantially the cutting speed and accuracy, and also for controlling the depth, shape and angle of the cut face formed by the crack. The method can be employed in the automotive industry for making glass windows and mirrors, in the electronics industry for making precision backings and substrates for LED indicator panels and masks, magnetic and optomagnetic disks, in watch-making for making protective glasses, in the aircraft and space industry for making structural optics components, in construction and architecture for dimensional pattern-cutting of glass, including its integration in the glass manufacturing technology, and also in other fields of production and technologies where precision of non-metallic materials are made.

Claims

1. A method of separating two portions of a body of brittle non-metallic material from each other including the step of forming a blind crack extending into the body to a given depth from a surface thereof, and in an intended direction along the surface, by effecting relative movement at a rate of relative displacement between the body and an elliptical target area on the surface thereof, said target area having a transverse minor axis and a longitudinal major axis, and being formed by directing an elliptical beam of coherent radiation towards the surface, the elliptical beam incident on the surface forming a spot, the spot having a major axis aligned substantially along the intended direction of the crack, and controlling the energy of the beam so that the beam heats the surface to a temperature below the softening point of the material while simultaneously directing a stream of fluid coolant at an area of the heated surface which constitutes a cooling zone in the intended direction, the fluid coolant being displaced behind the heated target area by a chosen distance, wherein the rate of relative displacement between the beam and the body satisfies the equation:

space="preserve" listing-type="equation">V=ka(b+L)/δ

where

V is the rate of relative displacement of the beam spot and the body;

k is a proportionality factor dependent on the thermophysical properties of the material of the body and a beam power density of the beam;

a is the length of said transverse minor axis;

b is the length of said longitudinal major axis;

L is the distance from the rear edge of the heat beam spot to the from edge of the cooling zone; and

δ

is the depth of the blind crack.

2. The method of claim 1 in which at least a volume of the body containing and bordering the intended direction of the crack is preheated.

3. The method of claim 2 in which the body is preheated to a chosen temperature related to a desired depth of the crack.

4. The method of claim 3 in which the body is preheated to a temperature satisfying the condition:

space="preserve" listing-type="equation">T=(0.4 to 1.0)T

where T is the thermal resistance of the body of material to cooling.

5. The method of claim 1 and including the further step of post heating the body, after the blind crack has been formed, along the direction of the crack and to an extent sufficient to cause the depth of the crack to increase further.

6. The method of claim 5 in which the post heating is effected by means of a second beam of radiation impinging on the same surface and moved relatively to the body along a path coincident with, or parallel to, the crack.

7. The method of claim 1 in which, when commencing forming the blind crack, the elliptical beam is initially incident at a point spaced inwardly from the borders of the body.

8. The method of claim 7 in which the elliptical beam traces out a closed curve on the body surface, and in which the direction of the major axis of the elliptical target area is kept at a constant orientation to a tangent to the curve at the centre of the target area.

9. The method of claim 8 in which the major axis is coincident with, or parallel to, the tangent.

10. The method of claim 8 in which the major axis extends at a fixed angle to the tangent.

11. The method of claim 10 in which, in order to produce articles with a decorative raised-pattern edge face, the major axis of the elliptical target area is at an angle of 3°

to 45°

to the tangent.

12. The method of claim 1 wherein the material has a thickness h and the size of the target area satisfies the condition of maintaining the beam power density over the area within the range of (0.3 to 20.0)×

10⁶ Wm^-2, with the following proportions being observed;

space="preserve" listing-type="equation">a=(0.2 to 2.0)h,

space="preserve" listing-type="equation">b=(1.0 to 10.0)h,

where

a and b are, respectively, the lengths of the minor and major axes of the elliptical target area.

13. A method of separating two portions of a body of brittle non-metallic material from each other along a curvilinear outline of relatively small curvature radii including the step of forming a blind crack extending into the body to a given depth from a surface thereof, and in an intended direction along the surface, by effecting relative movement at a rate of relative displacement between the body and an elliptical target area on the surface thereof, said target area having a transverse minor axis and a longitudinal major axis, and being formed by directing an elliptical beam of coherent radiation towards the surface, the elliptical beam incident on the surface forming a spot, the spot having a major axis aligned substantially along the intended direction of the crack, and controlling the energy of the beam so that the beam heats the surface to a temperature below the softening point of the material while simultaneously directing a stream of fluid coolant at an area of the heated surface which constitutes a cooling zone in the intended direction, the fluid coolant being displaced behind the heated target area by a chosen distance, wherein the rate of relative displacement between the beam and the body satisfies the equation:

space="preserve" listing-type="equation">V=ka(b+L)/δ

where

V is the rate of relative displacement of the beam spot and the body;

k is a proportionality factor dependent on the thermophysical properties of the material of the body and a beam power density of the beam;

a is the length of said transverse minor axis;

b is the length of said longitudinal major axis;

L is the distance from the rear edge of the heat beam spot to the front edge of the cooling zone; and

δ

is the depth of the blind crack;

and including the further step of post heating the body, after the blind crack has been formed, along the line of the crack and to an extent sufficient to cause the depth of the crack to increase further, the post heating step being effected by means of a second beam of radiation impinging on the surface and moved relatively to the body along a path coincident with, or parallel to, the crack, yet offset from the centre of a curvilinear outline when cutting along the curvilinear outline.

14. A method of separating two portions of a body of brittle non-metallic material from each other including the step of forming a blind crack along a closed curve extending into the body to a given depth from a surface thereof, and in an intended direction along the surface, by effecting relative movement at a rate of relative displacement between the body and an elliptical target area on the surface thereof, said target area having a transverse minor axis and a longitudinal major axis, and being formed by directing an elliptical beam of coherent radiation towards the surface, the elliptical beam incident on the surface forming a spot, the spot having a major axis aligned substantially along the intended direction of the crack, and controlling the energy of the beam so that the beam heats the surface to a temperature below the softening point of the material while simultaneously directing a stream of fluid coolant at an area of the heated surface which constitutes a cooling zone in the intended direction, the fluid coolant being displaced behind the heated target area by a chosen distance, wherein the rate of relative displacement between the beam and the body satisfies the equation:

space="preserve" listing-type="equation">V=ka(b+L)/δ

where

V is the rate of relative displacement of the beam spot and the body;

k is a proportionality factor dependent on the thermophysical properties of the material of the body and a beam power density of the beam;

a is the length of said transverse minor axis;

b is the length of said longitudinal major axis;

L is the distance from the rear edge of the heat beam spot to the front edge of the cooling zone; and

δ

is the depth of the blind crack;

and including the further step of first scoring the surface of the body along an incremental part of the desired crack to form a score, with the depth of the score being different at opposite ends thereof, and in which the beam of radiation is initially directed at that part of the score which is of greater depth.

15. The method of claim 14 including the preliminary step of making the score with a sharp body of hard material which is able to gouge out material from the surface of the body to a predetermined depth.