LT-0200 Glass Fiber Optics

Topics:

  • Fiber stripping

  • Fiber cleaving and cutting

  • Diode Laser Characterization

  • Coupling Light to Fiber

  • Signal transfer

  • Numerical Aperture of Fiber

  • Speed of Light

  • Fiber spool with fiber connector

  • Connecting spools in series


LT-0200 Glass Fibre OpticsLT-0200 Glass Fiber Optics


The basic idea to use guided light for data communication was published in 1939 by H. Buchholz in his paper „Die Quasioptik der Ultrakurzwellenleiter“ (The quasi optical behavior of ultra short wave guides). However it took more than 20 years to develop first realistic technical solutions mainly encouraged by the first available diode lasers in 1962.
These new light sources are ideally suited as transmitter because of their ability to be modulated and in addition, as we know today, they can be produced in large numbers at low prices. Nowadays the world wide communication is based on fiber optics combined with laser diodes and the development in this area belongs to the most exciting ones in this century. In 1977 based on the experience and results rapid investigation in other fields than communications were initiated, leading for example in the development of fiber gyros for navigation purposes of air planes. In principle this new technology do not require a new understanding of the physics because the related phenomena are well known and can be considered as a combination of classical optics and lasers. However for the realization a lot of technical problems had to been solved. In the fibers mainly used in communication the light is guided within a „glass tunnel“ with a diameter of 9 µm only. The necessary mechanical components as well the production process of the fibers itself were subject of comprehensive developments. Considerable efforts today are undertaken to reduce fiber transmission losses by using so called active fibers and in the realization of integrated optical devices for distributing and receiving signals. The field of fiber optics is still expanding and of high common interest. Therefore this experiment is considered as a introduction to this important technology.
The trainees are introduced firstly to prepare a bare optical fiber in such a way that suitable end faces are obtained. This process of fiber stripping and cleaving is a recurrent practice either in research labs or telecommunication. In a next step the light of a diode laser is characterized by measuring the output power versus the injection current and the spatial intensity distribution by using the provided photodetector which is mounted onto a pivot arm. By means of collimation optics the beam of the diode laser is made almost parallel before it enters the microscope objective which focuses the light into the multi-mode fiber By observing the output at the exit of the fiber the coupling efficiency is optimized by adjusting the precise mounts. Once a strong signal has been obtained the numerical aperture of the fiber is measured by means of the photodetector mounted to the pivot arm. In a next step the photodetector is connected to an oscilloscope and the injection current of the diode laser is modulated. Both the diode laser signal and fiber output are displayed on the scope and the time of flight becomes apparent and can be measured. From this measurement either the speed of light or the length of the fiber is determined.

Principle of data transmission via Optical Glass Fiber

A. Principle of glass fiber optics experimental set-up

By means of collimation optics, the beam of the diode laser is made almost parallel before it enters the microscope objective which focuses the light into the multi-mode fiber By observing the output at the exit of the fiber the coupling efficiency is optimized by adjusting the precise mounts. Once a strong signal has been obtained the numerical aperture of the fiber is measured by means of the photodetector mounted to the pivot arm. In a next step the photodetector is connected to an oscilloscope and the injection current of the diode laser is modulated. Both the diode laser signal and fiber output are displayed on the oscilloscope and the time of flight becomes apparent and can be measured. From this measurement either the speed of light or the length of the fiber is determined.
Oscilloscope traces to determin the speed of ligth or the fibre length
B. Oscilloscope traces to determine the speed of light or the fiber length
The facility to modulate the injection current of the diode laser makes it possible to measure the time of flight Δt of a laser pulse via 1000m, 2000 m or 3000 m of fiber With the known length of the fiber even the speed of light can be determined and the index of refraction of the fiber calculated.
LT-0200 Glass Fiber Optics, consisting of:
Item Code Qty. Description
1 CA-0060 1 Infrared display card 0.8 -1.4 µm
2 CA-0450 2 BNC connection cable 1 m
3 CA-0620 1 Optical fiber scriber and breaker
4 CA-0630 1 Adjustable plastic cover stripper
5 DC-0040 1 Diode laser controller MK1
6 DC-0120 1 Si-PIN Photodetector, BPX61
7 MM-0490 1 Translation stage with bare fiber holder
8 MM-0494 1 Rotation stage with bare fiber mount
9 MP-0150 1 Optical Bench MG-65, 500 mm
10 OC-2040 1 Set of 10 ST pigtailed MM fiber
11 OC-2450 1 Multi-mode fiber 1000 m, 50/125 µm, ST panel jacks
12 OM-0620 1 Collimating optics on carrier MG20
13 OM-0950 1 MO coupling optics, 4 axes kinematic mount
14 OM-L500 1 Diode laser module 808 nm on C20
15 UM-LT02 1 Manual Glass Fiber Optics
Required Option (order separately)
16 CA-0200 1 Oscilloscope 100 MHz digital, two channel
Option (order separately)
17 OC-2440 1 Single-mode fiber, 1000 m, 9/125 µm, ST panel jacks
18 OC-2460 1 Multi-mode fiber, 2000 m 50/125 µm, ST panel jacks
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