Fiber-optic gyro

• US 4,621,925 A
• Filed: 09/20/1983
• Issued: 11/11/1986
• Est. Priority Date: 11/11/1982
• Status: Expired due to Fees

• Current Assignee: Fujitsu Limited
• Original Assignee: Fujitsu Limited
• Inventors: Masuda, Shigefumi, Iwama, Takeo
• Primary Examiner(s): Willis, Davis L.
• Assistant Examiner(s): TURNER, SAMUEL A
• Application Number:
  US06/534,126
• Time in Patent Office: 1,148 Days
• Field of Search: 356/350, 356/351, 350/96.18
• US Class Current: 356/460
• CPC Class Codes: G01C 19/72 with counter-rotating light beams in a passive ring, e.g. fibre laser gyrometers

Abstract

A fiber-optic gyro includes a laser diode, a light detector, first and second lenses arranged on both sides of a half mirror, and a coil-like optical fiber which is arranged so that the two ends of the optical fiber confront the first and second lenses, respectively. Light from the laser diode is incident on the half mirror through the first lens, the light reflected from the half mirror is incident from one end of the coil-like optical fiber through the first lens, and the light transmitted through the half mirror is incident from the other end of the coil-like optical fiber through the second lens. Therefore the light is propagated through the coil-like optical fiber in opposite directions, light from the coil-like optical fiber is synthesized and is incident on the light detector, and the speed of the rotation angle is detected by the output of the light detector.

Claims

1. A fiber-optic gyro comprising

a laser diode,

a light detector,

a half-mirror,

first and second lenses arranged on both sides of said half-mirror, and

first and second optical fibers each having two ends, a respective first of said ends of each of said fibers being aligned with a respective end of the other fiber, and said half-mirror being interposed between said aligned ends,

a third optical fiber having two ends, said third optical fiber being arranged in a coil and so that said two ends are arranged to be parallel to respective portions of said first ends of the first and second optical fibers,

wherein light from the laser diode is incident on the half-mirror through the first lens to produce two light beams, the first of said light beam being reflected from the half-mirror and incident on a first one of said ends of the third optical fiber through the first lens, and the second light beam being transmitted through the half-mirror and incident on the other end of the third optical fiber through the second lens, so that said light beams are propagated through the third optical fiber in opposite directions, and

means for synthesizing the light beams from the third optical fiber into a combined beam that is incident on the light detector,

wherein the speed of the rotation angle is detector by the output of the light detector.

2. A fiber-optic gyro according to claim 1, wherein each said lens is formed of a monoaxial crystal.

3. A fiber-optic gyro according to claim 1, wherein said third optical fiber is a polarization plane storing fiber.

4. A fiber-optic gyro according to claim 3, wherein a control portion for the polarization plane is formed between said laser diode and said first lens for providing fine adjustment of the polarization plane of incident light and a polarization maintaining axis of the third optical fiber.

5. A fiber-optic gyro according to claim 4, wherein another control portion for providing fine adjustment of the polarization plane is formed on a part of said third optical fiber.

6. A fiber-optic gyro according to claim 1, wherein said laser diode is provided with a narrow-band reflection filter.

7. A fiber-optic gyro according to claim 6, wherein an etalon formed with a single-mode optical fiber having a plane reflecting mirror arranged on one end face is used as the narrow-band reflection filter.

8. A fiber-optic gyro according to claim 1, wherein said third optical fiber comprises a fiber of quartz and has a triple structure including a core, a clad and a jacket in which the difference of the refractive index between the core and clad (in terms of ##EQU25## in which n1 represents the refractive index of the core and n2 stands for the refractive index of the clad) is 0.13±

0.05, said third optical fiber being wound on a drum to provide said coil.

9. A fiber-optic gyro according to claim 3, wherein a control portion for the polarization plane is formed on a part of said third optical fiber for providing fine adjustment of the polarization plane.

11. A fiber-optic gyro according any one of claims 1 to 10, wherein the position of said half-mirror is changed by an electrostriction element, for providing a phase difference between said light beams incident on said ends of said third optical fiber, and, only when the light synthesized by said half-mirror is converted to an electric signal, is phase detection carried out and the phase difference measured.

12. A fiber-optic gyro according to claim 11, comprising

means for adjusting the coil delay time τ

coil, which is determined by the length L of said third optical fiber and the light propagation speed c of said third optical fiber, and the light emission time interval D of said laser beam, so that the following relation is established;

space="preserve" listing-type="equation">D≧

τ

coil,

said light detector including an electric gate,

wherein the light emission time interval D is made equal to a time interval D_det for opening said electric gate in the light detector, and the time deviation between said interval D and said interval D_det is made equal to said coil delay time τ

coil.

14. A fiber-optic gyro according to any one of claims 1, 10 and 13, wherein at least one reflecting member is arranged to confront a respective light emitting parts of at least one end portion of said laser diode so that at least one etalon is constructed.

15. A fiber-optic gyro according to claim 14, wherein said at least one reflecting member is a reflecting film formed on the respective end face of said the respective optical fiber.

10. A fiber-optic gyro comprising

a half-mirror including a dielectric multilayer film formed on one surface of an optical substrate,

first and second optical fibers each having two ends, a respective first of said ends of each of said fibers being aligned with a respective end of the other of said fibers, said half-mirror being interposed between said aligned ends,

a third optical fiber fiber having a single-mode and a polarization-plane storing-property and forming a coil, said third optical fiber having two ends and being arranged so that each of said ends of the single-mode fiber are parallel to a respective portion of a respective one of said first ends of the first and second optical fibers, with the half-mirror being interposed between both said ends of said third optical, and between said aligned ends of the first and second fibers, and both said ends of said third optical fiber being tilted with respect to the optical axes of said respective portions of said first and second optical fibers, and

a light detector,

wherein a single-mode laser beam of a predetermined polarization is incident on the second end of the first optical fiber, a laser beam emerging from said first end of the first optical fiber is divided into two light beams by said half-mirror, said two light beams are incident on respective ones of said ends of said third optical fiber and propagate through said third optical fiber in opposite directions, the light beams emergent from both ends of said third optical fiber are synthesized into a combined beam that is incident on said first end of the second optical fiber, and a light beam emerging from the other end of the second optical fiber is detected by said light detector.

13. A fiber-optic gyro, which comprises

a Rochon prism having the same tilt angle α

₁ on respective incident and emergent end faces thereof,

an input optical fiber having a core, an optical axis parallel to the mechanical axis of the Rochon prism and a tilt angle θ

p on the emergent end face arranged at a point separated by a distance h from said mechanical axis of the Rochon prism,

a first lens having a focal distance F, which is interposed between the input optical fiber and the Rochon prism and has a center at a point separated by a distance I₁ from said incident end face of the Rochon prism on said mechanical axis of the Rochon prism,

two output optical fibers having cores and being arranged at points separated by a distance h from an axis parallel to said mechanical axis passing through the equivalent light branching point of the Rochon prism and having respective tilt angles of θ

p and -θ

p on said incident end faces thereof, and

a second lens having a focal distance F, which is interposed between both the optical fibers and the Rochon prism and has the center on an axis parallel to said mechanical axis of the Rochon prism and separated by a distance I₁ from said equivalent light branching point,

wherein the tilt angle α

₁ of the Rochon prism, the emergent angle θ

o of the input optical fiber, the incident angle θ

r of the output optical fiber, and the focal distance F of both the lenses are determined by the following relations;

##EQU26## wherein n_e represents the refractive index of the Rochon prism with respect to an abnormal light beam, n_o represents the refractive index of the Rochon prism with respect to a normal light beam, δ

stands for a separation angle in the Rochon prism as between abnormal and normal light beams, n_c stands for the refractive index of said inlet and outlet optical fiber cores, and n_a stands for the refractive index of air.