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Introduction
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HUBER+SUHNER 15
The voltage across the gas discharge tube then rises
very rapidly. When the dynamic spark-over voltage
has been reached (typ. 675 V at 1 kV/ěs for 230 V
GDT), the gas discharge tube will ignite and become
conductive. At this moment, the voltage across the GDT
(called the glow-arc voltage) is between 72 and 90 V.
This collapses to 10 –
20 V (called the arc voltage), as
the current rises. The dynamic spark-over voltage of the
GDT is a function of the pulse rise time.
The gas discharge tube, once it sparks over, creates a
potential equalization between the inner and the outer
conductor (ground) of the coaxial transmission line. The
current flows along the path of least resistance through
the GDT to the ground. Only a very small portion of the
energy, the so-called residual pulse, reaches the equipment.
Its magnitude is determined by the GDT characteristics,
the interference pulse rise time, and the ground
conductor impedance (determined by the quality of the
lightning protection system).
After the interference has subsided, the gas discharge
tube is extinguished, reverting to its original high-ohmic
condition.
Gas discharge tube protectors can generally be used
in wideband applications from DC to over 2.5 GHz,
latest designs up to 6.0 GHz. The upper limit for the
operating frequency range is determined by the capacitive
characteristics of the GDT.
GDT protectors allow DC to be carried and thus towermounted
electronic equipment to be fed power via the
coax line.
Lightning EMP protectors with quarter-wave (ë/4)
shorting stub
This technology is based on a quarter-wave transformation
line. The coaxial shorting stub applied for this
purpose is short-circuited at its end, and its length is
matched to the mid-band frequency of the operation
band. It thereby forms a bandpass filter. Its bandwidth
can be adjusted up to ± 50% of the centre frequency.
Operating principle of quarter-wave lightning EMP protectors
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