Main advantage of fiber optic cable over co-axial cable is
Low loss
This explanation focuses on the primary benefits of using fiber optic cables compared to traditional coaxial cables. We will explore why the characteristic of 'low loss' is considered the most significant advantage.
Signal attenuation, commonly referred to as signal loss, is the decrease in the strength of a signal as it travels through a transmission medium. For effective data communication, especially over long distances or at high speeds, minimizing this loss is crucial. Signal loss is typically measured in decibels per kilometer (dB/km).
Fiber optic cables demonstrate remarkably low signal loss. For example, standard single-mode fiber optic cables usually have an attenuation rate of approximately $0.2$ dB/km to $0.35$ dB/km when using a wavelength of 1550 nm. In contrast, coaxial cables experience significantly higher losses, often ranging from $5$ dB/km up to $15$ dB/km or more, varying with the cable specifications and the frequency of the signal.
Here’s a comparison highlighting the differences:
The extremely low loss property of fiber optic cables is its principal benefit because it enables:
In summary, while factors like less weight offer practical installation benefits, the fundamental advantage that drives the adoption of fiber optic technology for modern high-performance networks is its superior performance in minimizing signal loss.
Fibre optic power meters have input for attaching fiber optic connector and detector:
The material used for making optic-fibre cable in general is-
Multimode step-index fiber with a core diameter of 80 μm and a relative index difference of 1.5% is operating at a wavelength of 0.85 μm. If the core refractive index is 1.48, then the normalized frequency for the fiber is
In a multimode fiber (step index), number of modes passing at an operating wavelength of 1300 nm are 1000, the refractive index of the core is 1.50 and that of the cladding is 1.48. The value of core diameter is:
In optical fibers, the Rayleigh scattering is proportional to: