electrical theory and electrical fundementals for all electrical related people . students , engineers, electrician #electricaltheorems,electrical,
The
architecture and the operation of the OTDR system
The OTDR is
the most important investigation tool for optical fibres, which is applicable
for the measurement of fibre loss, connector loss and for the determination of
the exact place and the value of cabel discontinuities. By means of very short
pulses it is also possible to measure the modal dispersion of multimodal
fibres. The structure of a typical OTDR equipment is shown below:
The
principal of the OTDR analyzer is the following: a short light pulse is
transmitted into the fibre under test and the time of the incidence and the
amplitude of the reflected pulses are measured. The commonly used pulse width
ranges from nanosecs to microsecs, the power of the pulse can exceed 10 mW. The
repetition frequency depends on the fibre length, typically is between 1 and 20
kHz, naturally it is smaller for longer fibres. The division by 2 at the inputs
of oscilloscope is needed since both the vertical (loss) and the horizontal
(length) scales correspond to the one-way length.
The components of the fibre loss and their importance in the OTDR measurements
There are
three reasons for the fibre loss:
•
absorption
• radiation
loss
• Rayleigh
scattering
The absorption creates 10-20% of the
fibre loss. It mainly originates from the OH- ions inside the fibre material
(impurities). With modern technologies the number of these contaminants, so the
loss can be kept at relatively low level. The fibre loss increases dinamically
for wavelengths above 1700 nm, thus this is the lowest frequency for optical
telecommunications. In practice the 1300 and 1550 nm wavelengths are used as
the insertion loss shows minimal values at these wavelengths. Naturally,
absorption does not induce reflection, so if this would be the only physical
phenomena, the fibre loss could be measured by the means of OTDR only with a
well known, calibrated termination
In
practice, the fibre continuously radiates backwards due to the Rayleigh
scattering, which will be described later, so the absorption loss is measured
together with the other losses.
Radiation
loss occurs when the geometrical parameters of the fibre abruptly change, or a mechanical
tension is present in the fibre material due to fabrication failure or
mechanical impact. Considering appropriate fabrication technologies and fibre
jacket, the radiation loss can be neglected and, like absorption, it does not
create reflections, so from the OTDR measurements point of view it can handle
as absorption losses. A high level discontinuity originated by e.g. strong
folding, can be shown by OTDR as it produces high loss.
During OTDR
measurements the most important loss is the one caused by Rayleigh scattering.
It generates the 80-90% of the total loss. The scattering is induced by the microscopic
inhomogenity of the refractive index of the fibre. These inhomogenities cause diffraction,
so a certain part of the light energy is radiated isotropically. The level of
the diffrection reaches its maximum when the wavelength is in the same range as
the dimensions of the microscopic inhomogenities. Thus the level of the
scattering decreases when the wavelength is increased. Among others this is the
reason for using the 1300 and the 1550 nm ranges instead of the 850 nm. A
certain part of the diffracted light propagates backwards in the fibre which
is, when measured, carries important information. In the following, we calculate
the ratio of the diffracted and the backward propagating light.