Fibre optical arrangement for measuring the intensity of an electric current

• US 4,255,018 A
• Filed: 08/13/1979
• Issued: 03/10/1981
• Est. Priority Date: 08/16/1978
• Status: Expired due to Term

• Current Assignee: Max-Planck-Gesellschaft Zur Foerderung Der Wissenschaften e.V. (Max-Planck-Gesellschaft zur Frderung der Wissenschaften e)
• Original Assignee: Max-Planck-Gesellschaft Zur Foerderung Der Wissenschaften e.V. (Max-Planck-Gesellschaft zur Frderung der Wissenschaften e)
• Inventors: Ulrich, Reinhard, Rashleigh, Scott C.
• Primary Examiner(s): Rosenberger, Richard A.
• Application Number:
  US06/066,282
• Time in Patent Office: 575 Days
• Field of Search: 350/150, 350/151, 350/96.29, 356/368, 324/96
• US Class Current: 385/12
• CPC Class Codes: G01R 15/246 based on the Faraday, i.e. linear magneto-optic, effect

Abstract

A fibre optical arrangement for measuring the intensity of an electric current using the Faraday effect, in which the path of light whose state of polarization is influenced by the magnetic field surrounding the conductor through which current flows is marked by the core of an optical fibre which is coiled round the conductor in a number of turns, the optical fibre used in the arrangement being one which has a circular double refraction α at least of the order of magnitude of a linear double refraction β determined by the structure of the fibre and its coiled arrangement. The fibre is preferably twisted about its longitudinal axis so that the twist is substantially evenly distributed over the length of the optical fibre.

Claims

1. A fiber optical arrangement for measuring the intensity of an electric current using the Faraday effect, in which the path of light for the light whose state of polarization is influenced by the magnetic field surrounding the conductor through which current flows is marked by the core of an optical fiber which is coiled round the conductor in a number of turns, the optical fiber used in the arrangement being one which has a circular double refraction α

at least of the order of magnitude of a linear double refraction β

determined by the structure of the fiber and its coiled arrangement.

2. A fiber optical arrangement according to claim 1, in which the core of the optical fiber consists of crystalline, optically active material having its optical axis extending in the direction of the axis of the fiber.

3. A fiber optical arrangement according to claim 1, in which the optical fiber is a liquid core fiber whose core liquid is optically active or contains optically active additives.

4. A fiber optical arrangement according to claim 1, in which the optical fiber is a solid core fiber which has the required circular double refraction α

imposed on it by being twisted about its longitudinal axis.

5. A fiber optical arrangement according to claim 4 in which the axial twist in rad/m is chosen according to the following relationship:

τ

>

3β

/g

wherein β

is the linear double refraction in rad/m resulting from the structure of the fiber and its coiled arrangement and g is a material constant which in the case of quartz glass has a value in the range of 0.13 to 0.16.

6. A fiber optical arrangement according to claim 4 in which the twist is uniformly distributed over the length of the optical fiber.

7. A process for the production of a fiber optical arrangement according to claim 4 including imparting the twist to the optical fiber in adjacent partial lengths by fixing the beginning of each fiber section to a support, twisting the section thus fixed and fixing the other end thereof to the support, and that section of the same or of another partial length of optical fiber which is adjacent to the fixed point being then twisted and having its end again fixed to the support so that it can no longer be twisted.

8. A process according to claim 7, including eliminating the attachment between the optical fiber and the support at the points of attachment situated between the beginning and end of the twisted fiber length when the fiber has been directly placed on the support and has been fixed and secured against twisting on the support at its point of attachment remote from the first point of attachment.

9. A process according to claim 8, in which an adhesive which can be softened by heat and/or dissolved chemically is used for fixing the optical fiber to the points of attachment situated between the beginning and end of is twisted length.

10. A fiber optical arrangement according to claim 1 in which the circular double refraction is at least three times greater than the linear double refraction of the optical fiber.

11. A fiber optical arrangement according to claim 1 in which the optical fiber surrounds the current carrying conductor in the manner of a tightly wound coil whose turns are arranged directly side by side and optionally one above the other and in parallel planes which are substantially at right angles to the longitudinal axis of the conductor.

12. A process for the production of a fiber optical arrangement according to claim 11, having a spirally wound fiber with m turns and a twist at the end of the fiber relative to its beginning of n·

360°

, including fixing the fiber at one end, and twisting it in the stretched state at its other end (n+m) times through 360° and

using the torsional stress thereby produced to produce the m turns of the coil.

13. A process according to claim 12, in which;

(a) one end of the optical fiber is attached in such a manner to one of the supporting elements at one end of a support which comprises, as supporting elements, rigid rods, stretched wires or threads extending along the edges of a prismatoid, the effective cross-section of which support can be increased by moving the supporting elements apart in the radial direction, that at its point of attachment the fiber can be pivoted about an axis extending radially to the longitudinal axis of the prismatoid but is held so that it cannot be turned about its longitudinal axis;

(b) the fiber is twisted n times while stretched, and thereafter, while the prismatoid is adjusted to its smallest cross-section, the fiber is placed spirally in m turns with a high thread pitch around the support, the free end of the fiber being carried round the support in such a manner that the same side of the circumferential surface of the end of the fiber is constantly facing the support, in order that the m subsequent turns through 360°

will be imparted to the fiber;

(c) the free end of the fiber, which has thus been twisted (n+m) times in relation to that end of the fiber which is already attached to the end of the support, is now fixed again to a part which can be displaced along one of the supporting elements, so that this end of the fiber, though capable of following a change in the pitch of the turns, cannot rotate about the axis of the fiber;

(d) then, while the distance between the ends of the fiber successively shortens and at the same time the radial distance of the supporting elements from the longitudinal axis of the support increases, the fiber turns, which correspondingly increase in diameter, are pushed together until they are in direct contact with each other.

14. A process for the production of a fiber optical arrangement according to claim 11 in which the fiber is carried round a core and has a given number of turns, the diameter of the turns being initially selected to be somewhat greater than the diameter of the core, and the free end of the fiber whose other end is non-rotatably attached to the support being then turned until the required degree of twist is obtained along the fiber, and the fiber is then stretched sp that it is in direct contact with the support and the free end of the fiber is then also attached to the support so that it can no longer be twisted.