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Optimizing Processes with RFID and Auto ID, 2009

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2 <strong>RF<strong>ID</strong></strong> technology<br />

2.3 Classification of <strong>RF<strong>ID</strong></strong> systems<br />

2.3.1 Passive systems<br />

For passive <strong>RF<strong>ID</strong></strong> systems, the transponder does not have its own energy<br />

source: energy is fed to most systems externally. Normally this<br />

takes place via high-frequency transmission, in rare cases also via<br />

light, sound, pressure, temperature, or other mechanisms. Special<br />

models of passive systems require no energy at all, in which they are<br />

simply based on physical effects.<br />

While the development of a high-performance passive transponder<br />

requires quite some effort, this principle provides a number of advantages:<br />

• It is easy to produce the transponder (only a chip <strong>and</strong> an antenna<br />

are required)<br />

• They have a virtually unrestricted life cycle <strong>and</strong> are service-free<br />

(no battery)<br />

• They can be extremely miniaturized<br />

• Very low costs are possible (to the order of < 0.10 euros)<br />

Systems <strong>with</strong> inductive coupling in the LF/HF range<br />

The oldest <strong>RF<strong>ID</strong></strong> systems are based on energy transfer via a high-frequency<br />

magnetic field <strong>with</strong> inductive coupling, i.e. using the transformation<br />

principle. Fig. 2.6 shows the principle: The transmitter in<br />

the reading device drives current through the antenna coil, thereby<br />

creating a high-frequency magnetic field. Alternating voltage is produced<br />

in the transponder coil by induction <strong>and</strong> is available for operating<br />

the transponder chip after rectification. Data is transferred to<br />

the reader via load modulation. At the same time, a resistive load is<br />

switched to the antenna coil in the transponder according to the modulation<br />

of data. This results in a voltage drop at the reader’s transmission<br />

coil – albeit minimal – can be detected <strong>and</strong> analyzed in the reader<br />

electronics (receiver).<br />

The frequencies that are usually used are 125 kHz (LF) or 13.56 MHz<br />

(HF), as these b<strong>and</strong>s are especially attractive combined <strong>with</strong> the high<br />

permissible output power <strong>and</strong> they can be used worldwide. Read<br />

ranges in excess of one meter can be accomplished. However, at the<br />

same time large antenna coils are required (e.g. 60 × 80 cm), which<br />

30

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