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Trolleyponder®/EcoTag®

Technical notes - Transmission and reflection of energy

The propogation of electromagnetic energy between the reader and the transponder, passing through various bodies, is a complex situation. For the part of the path where the energy travels through air, the energy density available to the transponder drops off as the square of the distance (every doubling of range requires four times the amount of transmitter energy), and when the energy passes through solid items in the direct path between the reader and the transponder, much of the energy is reflected off the boundaries of the bodies and never reaches the transponder.

Reflected and transmitted energy at single interface with air

Materials in nature exhibit an electrical property called their dielectric contant. Comparing this to the dielectric constant of air gives the RELATIVE DIELECTRIC CONSTANT which is measured for various materials. For the non- RF engineer, think of dielectric constant as similar to the density property of a material.

Those engineers who have been involved in the development of short range high resolution radars, such as for detecting fissures in rocks in underground gold/coal mining operations - or for detecting blocks of explosives set in a road - know that the interface where two materials of different dielectric constant meet, causes some of the incident energy to reflect which can then be detected to locate the edge of the saught objects. Due to some of the energy reflecting, a weakened signal continues through the object, some of which will reflect at the next boundary.

The diagram on the left shows the mechanics of the situation, For example consider energy hitting the edge of a wooden plank which is held up in the path of transmission between a reader and the transponder. The energy travelling towards the reader (INCIDENT ENERGY) meets the interface between the air and the wooden plank. At this point some of the energy is reflected (REFLECTED ENERGY) which can be typically 27 % for a Mahogany plank, and the balance continues through the the plank.

The following tableshows the percentage of voltage energy that is reflected off the interface for different materials:

Material Relative dielectric constant Percentage energy reflected from air interface Percentage energy transmitted into object
Glass4.825446
Fibreglass3.094357
Porcelin5.005545
Foamed polystyrene1.03199
Polyethelene2.263367
Jet Fuel2.043070
Beeswax2.393565
Vulcanised Rubber2.153268
Balsawood1.22991
Mahogany1.882773
Paper2.703961
Sandy soil2.553763
Fresh snow1.20991
Pure Water788911
Ice1.20991
Voltage reflection and transmitted energy at single interface between air and object

Reflected and tranmitted energy for dual interface with air

When the energy which is now inside the object leaves the object into another material, for example air, a similar process happens and the more energy is diverted from reaching the transponder. This mechanism applies to objects that are sizeable compared to the wavelength of the operating frequency, say from a couple of centimeters upwards. It does not matter how thick the object is - just how much energy is lost at the two interfaces. This situation would arise whenever you are trying to read a transponder that is on the farside of the object being labelled, or where the energy has to pass through one object to read the transponder attached to another object.

The following table shows how the voltage energy will be reduced passing through a slab of different materials held in the path of the reader/transponder.

Material Relative dielectric constant Percentage of incident energy successfully passing through the body.
Glass4.8221
Fibreglass3.0932
Porcelin5.0020
Foamed polystyrene1.0397
Polyethelene2.2644
Jet Fuel2.0449
Beeswax2.3942
Vulcanised Rubber2.1547
Balsawood1.2282
Mahogany1.8853
Paper2.7037
Sandy soil2.5539
Fresh snow1.2083
Pure Water781
Ice1.2083
Percentage of incident voltage energy that passes through object having two interfaces to air.

Range versus sensitivity in air

Trolley Scan have a system that can read tags at distances as far as 13 meters in air. This is due to the very low powers needed to operate a Ecochiptag, just 200uWatt of power in the 149sq cm capturing area. This might appear to be an overkill, but once one analyses how the RF energy propogated from the transmitter in the reader to the transponder, one will realise that a very important quality factor for a transponder system is how little power is needed for the transponder to operate.


Impact of range with objects placed in the path The chart on the left shows how range is effected by goods placed in the path. Two different tag sensitivities are shown, namely 200uW and 1 milliwatt by way of example. As explained above, just by placing the object in the path causes a loss of a large percentage of the power at the boundaries of the object. In this example, both the 1 mW and the 200uW tags would be able to attached to the far side of the goods and still be read, the 1mW version just having sufficient sensitivity.

Developing a tag with low sensitivity comes from three criterea-

  • The DC power consumption must be lower than the RF power consumption required
  • The operating voltage of the chip must be as low as possible, preferably as low as 1 volt
  • The antenna impedance must be very high (A conventional dipole has 72 ohm impedance, while an Ecochiptag has 11000 ohm impedance)
  • For benchmarking a conventional 5 volt chip attached to a dipole would need 54mW. Hence even getting a 1 milliwatt transponder would be a major achievement.

    Due to the very low operating powers, Ecochiptags can be mounted on either side of objects as they will still be able to operate even when the large losses caused by the differences in dielectric constants of the objects in the path are taken into account. The operating range will be reduced dramatically from the 13 meter air situation to possibly 4 to 6 meters depending on the materials. Trolley Scan also produce Ecowoodtags which are ideally suited for wooden and paper objects allowing the transponder to be mounted on any side of the object.

    From the above explanation, the reader will realise that objects in the path cause a lot of reflected energy, which also bounces around the reading zone, and can result in transponders that are in difficult situations for the direct path still being read. The signals bounce particularly well off walls and floors as well as metal and water based items, giving UHF RFID a much better volumetric coverage than most of the competitive frequencies.

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