Method and apparatus for breaking an optical fiber

Claim 2

In the method of breaking an optical fiber in which the fiber is weakened at the desired break location and the fiber is then stressed to cause the fiber to break at the desired break location, the method being characterized in that: elastomeric material is placed in completely surrounding relationship to a portion of the fiber extending from the desired break location in opposite directions along the longitudinal axis of the fiber so that the elastomeric material has ends which are spaced from the desired break location, the elastomeric material is compressed radially towards the axis of the fiber so that the interface surfaces of the fiber and the elastomeric material are pressed against each other to the extent that relative movement of the fiber and the elastic material is prevented, and the elastomeric material is further compressed and elongated in both axial directions away from the desired break location as a result of the compression so that the fiber is placed in tension by the elastomeric material causing the fiber to break by propagation of a crack from the desired break location across the diameter of the fiber.

Claim 3

A method of breaking an optical fiber as set forth in claim 1 characterized in that the elastomeric material is compressed by first applying radially directed compressive forces to a limited zone of the elastomeric material at the desired break location of the fiber, and the zone of application of the compressive forces is progressively increased in both axial directions from the desired break location.

Claim 4

The method of breaking an optical fiber as set forth in claim 1 characterized in that the fiber is weakened at the desired break location by scribing a notch in the fiber.

Claim 5

The method of breaking an optical fiber as set forth in claim 1 characterized in that the elastomeric material is placed in surrounding relationship to a portion of the fiber by placing the portion of the optical fiber between the opposed surfaces of two blocks of elastomeric material.

Claim 6

The method of breaking an optical fiber as set forth in claim 4 characterized in that a curvature is imparted to the fiber and to the elastomeric material during compression of the elastomeric material.

Claim 7

Apparatus for breaking an optical fiber which has been weakened at the desired break location, the apparatus being of the type which places the fiber in tension so that a crack travels across the fiber at the desired break location, the apparatus comprising: a body of elastomeric material having a fiber-receiving opening extending therethrough between its ends and having major surfaces which extend parallel to the fiber-receiving opening and between the ends, an actuator having a recess therein for reception of the body of elastomeric material and having force applying surfaces for applying compressive forces of increasing magnitude to the major surfaces of the body of elastomeric material whereby, upon placement of the optical fiber in the fiber-receiving opening of the body of elastomeric material with the desired break location substantially midway between the ends thereof and upon the imposition of compressive forces of increasing magnitude to the major surfaces of the body of elastomeric material, the body of elastomeric material will be compressed onto the optical fiber and will be elongated, and the optical fiber will thereby be gripped in the body of elastomeric material, and the optical fiber will be placed in tension as a result of the elongation of the elastomeric material and a crack will travel across the fiber at the desired break location.

Claim 8

Apparatus for breaking an optical fiber which has been weakened at the desired break location, the apparatus being of the type which places the fiber in tension so that a crack travels across the fiber at the desired break location, the apparatus comprising: a body of elastomeric material having a fiber-receiving opening extending therethrough between its ends and having major surfaces which extend parallel to the fiber-receiving opening and between the ends, an actuator having a recess therein for reception of the body of elastomeric material and having force applying surfaces for applying compressive forces of increasing magnitude to the major surfaces of the body of elastomeric material whereby, upon placement of the optical fiber in the fiber-receiving opening of the body of elastomeric material with the desired break location substantially midway between the ends thereof and upon the imposition of compressive forces of increasing magnitude to the major surfaces of the body of elastomeric material, the body of elastomeric material will be compressed onto the optical fiber and will be elongated, and the optical fiber will thereby be gripped in the body of elastomeric material, and the optical fiber will be placed in tension as a result of the elongation of the elastomeric material and a crack will travel across the fiber at the desired break location.

Claim 9

Apparatus for breaking an optical fiber as set forth in claim 6 characterized in that the body of elastomeric material comprises at least two blocks of elastomeric material in side-by-side juxtaposed relationship, the two blocks having opposed surfaces, the fiber-receiving opening being on the opposed surfaces.

Claim 10

Apparatus for breaking an optical fiber as set forth in claim 6 characterized in that the actuator comprises at least two rigid actuator blocks, one of the actuator blocks having the recess therein which is dimensioned to receive the body of elastomeric material, the other actuator block having a compressing rib which is dimensioned snugly to enter the recess.

Claim 11

Apparatus for breaking an optical fiber as set forth in claim 6 characterized in that the force-applying surfaces of the actuator are shaped to impart a curvature to at least portions of the body of elastomeric material in the vicinity of the desired break location of a fiber held in the fiber receiving opening during the application of compressive forces to the major surfaces.