Using your Attenuator as a Variable Back Reflector

Setting Up the Software

4.2 Setting Up the Software

There are four factors that influence the back reflection of the attenuator. These are

1.the insertion loss of the attenuator (INS LOSS),

2.the return loss of the attenuator (RL INPUT),

3.the reference return loss you are using (RL REF), and

4.the filter attenuation.

The return loss (RL) is calculated according to the equation

RL ( dB) = –10 log 10

R L In pu t( d B)

-------------------------------------

10

 

----R----L----I--n----p---u----t--(--d----B---)-

 

----(--2----(--A----t--t--(---d---B----)----+-----I--n----s---L---o----s---s--(---d---B----)--)----+-----R----L----R----e---f---(--d---B----)--)-

1 – 10

10

10

10

+

 

 

 

 

 

 

You edit the values for the insertion loss, the reference return loss, and the return loss of the attenuator while you are setting up the application.

You edit the value for the return loss while the application is executing. The instrument calculates and sets the required value for the filter attenuation.

Editing the Setup

Before you start setting up the back reflector application, you may need to measure the following values, if you do not already know them:

The insertion loss of the instrument (see “Example, Setting the Calibration” on page 42,

The return loss of the instrument (with the output properly terminated), and

The reference return loss value.

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Agilent Technologies 8156A manual Setting Up the Software, Editing the Setup

8156A specifications

Agilent Technologies 8156A is a high-performance optical source offering advanced capabilities for testing and characterizing optical systems. Specifically designed for applications in telecommunications and data communications, the 8156A stands out due to its precision, versatility, and reliability, making it an essential tool for engineers and researchers in the telecommunications industry.

One of the main features of the 8156A is its ability to generate a stable, accurate, and tunable optical signal. This optical source operates across a wide wavelength range, typically from 1260 nm to 1675 nm, covering key regions used in fiber optics. The tunable laser module is particularly beneficial for applications requiring the testing of fiber optic components, systems, and networks, enabling users to specify any wavelength within this range.

The device employs advanced technologies, including distributed feedback (DFB) laser technology, offering low noise and high output power while ensuring minimal phase and frequency jitter. This results in precise measurements that are crucial for evaluating the performance of optical devices. The 8156A also features a built-in optical power meter, allowing for seamless integration and real-time monitoring of optical power levels during testing.

Another significant characteristic of the 8156A is its user-friendly interface, which includes easy-to-read displays and intuitive controls. This design simplifies operation, allowing users to set up tests quickly and efficiently. Additionally, it provides various output options, including single-mode and multi-mode fiber interface compatibility, expanding its usability across different applications.

The 8156A is equipped to handle numerous protocols and systems, including passive optical networks (PON), optical transport networks (OTN), and traditional wavelength-division multiplexing (WDM) technologies. Its agility in adapting to various protocols enhances its role in research and development settings.

Moreover, the device offers a range of automation features, enabling users to script complex measurement sequences, making it an adaptable solution for both laboratory and field environments. Combined with its robust build quality, the Agilent Technologies 8156A optical source not only ensures reliable operation but also provides a long service life, making it a valuable investment for any optical testing application.