2001 Oct 04 16
Philips Semiconductors Product specification
HITAG core module hardware HTCM400
11.2 Antenna coil
The inductance of the coil should be between
350 and 500 µH.
The antenna quality factor (Q) should be
approximately 40.
If the Q factor is too high, it must be reduced with an
additional resistor. It is better not to use this additional
resistor, but instead to use a smaller wire diameter of the
coil.
The following formula describes the approximate
calculation of the number of windings for a desired
inductance and antenna geometry:
where:
L is desired inductance in nH
a is antenna circumference in cm
D is wire diameter in cm
N is number of windings
K is a geometrical constant:
For a circular antenna K = 1.01
For a square antenna K = 1.47.
Remark: the factor Kis normally much smaller than and
can therefore be left out:
11.3 Measuring the inductance
The inductance of the coil designed according to the
instructions as given in Section 11.2 can be measured
using the measuring set-up as shown in Fig.13.
A sinus signal of 125 kHz is fed using a function generator.
If you measure the current I
a
and the antenna voltage V
L
you can calculate the inductance according to the formula:
where .
11.4 Antenna cable length
For optimal performance, the antenna cable length should
not exceed 5 m.
Q
2 π× f× L×
R
s
------------------------------
=
L2a× ln
a
D
----
K


× N
1.9
×=
a
D
----
N
L
2a× ln
a
D
----


×
----------------------------------
1.9
MGW275
handbook, halfpage
47
L
R
f = 125 kHz
I
a
V
L
Fig.13 Measuring the inductance of the coil.
L
V
L
ω I
a
×
--------------
= ω 2 π× f×=
2001 Oct 04 17
Philips Semiconductors Product specification
HITAG core module hardware HTCM400
11.5 Antenna tuning
You have to tune the antenna in its final form with the connecting cable. You must not make any changes to the antenna
coil or the connecting cable after you finished tuning because mechanical changes influence the electrical values and
the antenna is detuned again.
handbook, full pagewidth
47
R3
1
MGW274
f = 125 kHz
R2
R1
L
C
s
V
o
V
R
V
a
Fig.14 Tuning the antenna.
A sinus signal of 125 kHz is fed to the antenna using a
frequency generator. You measurethevoltages V
a
and V
R
with an oscilloscope. Then you change the frequency until
V
a
and V
R
are in phase. If the resonance frequency now is
too high, you have to increase C
S
. If it is too low, you have
to decrease C
S
.
The aim is to get a resonance frequency of 125 kHz
using C
S
.
The resonant frequency has to be in the range of
125 ± 4 kHz.
11.6 Determining the serial resistance of the
antenna
Use an oscilloscope to measure V
a
and V
R
at a frequency
of 125 kHz. You can calculate the serial resistance R
S
of
the antenna with the following formulas: and
11.7 Checking the antenna voltage V
L
Before connecting the antenna to the read and write
device in Fig.15, you must carry out a check calculation of
the input level of the read and write device according to the
next formulas in order to prevent damage.
I
a
V
R
R3
-------
=
R
s
V
a
I
a
------
=
handbook, full pagewidth
CORE
MODULE
R2
R1
TX1
RX
AGND
L
C
s
R
e
I
a
V
o
V
L
MGW276
Fig.15 Calculation check of the input level.
2001 Oct 04 18
Philips Semiconductors Product specification
HITAG core module hardware HTCM400
V
o
2.5 V
V
L
=L×ω×I
a
where ω =2×π×f (f = 125 kHz)
The maximum value for V
L
reads 32 V (p-p), safeguarding
against damage to the input level of the read/write device:
With V
L
< 32 V (p-p) the resistance R
e
can be omitted
With V
L
> 32 V (p-p) you have to calculate and insert R
e
according to the following formula:
and
R
e
L ×ω×0.078 22 R
s
11.8 Procedure for practical antenna design
The procedure how to design a HITAG proximity antenna
is described in the previous sections. The main steps are
the following:
The desired inductance for the antenna coil can be
chosen in a range between 350 and 500 µH; e.g.
L = 420 µH
The number of windings N can be calculated with the
following formula:
For L = 420 µH:
N=
Remark: the factor K (see Section 11.2) normally is
much smaller than and therefore can be left out.
Now the antenna can be built up with the desired
dimensions (circumference a) with the calculated
number of turns.
Remark: the antenna coil must be changed afterwards
because with the mechanical dimensions the electrical
specifications are changing too. That means the number
of turns, the shape, arrangement of the coil windings
and antenna supply cable must be in their final form.
Remark: metal influences the electrical characteristics
of the antenna very much. That is why all future tasks
have to be done with the antenna in its final environment
if metal will be in the antenna’s neighbourhood (distance
of the metal shorter than the maximum antenna
diameter)
Measurement of the inductance L of the antenna is
described in Section 11.3
Determination of the serial capacitor C
S
is described in
Section 11.5
Remark: the capacitance of the antenna supply cable
can be measured or found out in the data sheet of the
cable (e.g. C
p
= 180 pF/m)
Now the antenna has to be tuned according to
Section 11.5. The tuning is acceptable if the resonant
frequency is within a range of 125 ± 4 kHz
The serial resistance R
s
of the antenna is the impedance
of the tuned antenna and is an ohmic resistance at the
resonance frequency (f = 125 kHz). It can be calculated
as shown in Section 11.6
To get a satisfactory reading distance the quality factor
of the antenna coil (for non-metal environment) should
be approximately Q = 40. The quality factor of a coil is
calculated as follows:
By knowing R
S
and the dropping resistor (R1 = 22 k)it
is possible to calculate the current I
a
and the antenna
voltage V
L
.
It is very important to calculate the antenna voltage
before connecting the antenna to the HTCM400 to avoid
damage. Is the calculated value of V
L
higher
than 32 V (p-p) a resistor R
e
has to be integrated to
protect the module output circuit. The resistor has to be
placed as shown in Section 11.7
After checking the antenna voltage connect your
antenna to the HTCM400 and measure the read/write
distances with your transponders. If the read/write
distances do not fulfil your expectations, the following
points should be considered:
The size of the antenna and the size of the
transponder have to be in a defined ratio (between 3
and 1). That means, if you increase the antenna over
a certain size, the maximum read/write distances will
decrease by the use of the same transponder
The optimal shape of the antenna coil is a circle. The
performance of a square shaped coil is much better
than that of a rectangular shaped coil (with the same
circumference)
To get better read/write distances the quality factor of
the antenna coil should be increased, but it must not
be higher than Q = 40. This can be reached by the
following measures:
I
a
V
o
R1 R
s
R
e
++
----------------------------------
=
R
e
L ω×
V
o
V
L(max)
------------------
R1 R
s
×=
N
LnH()
2a× ln×
a
D
----


K×
--------------------------------------------------
1.9
=
420000
2a× ln
a
D
----


K×
--------------------------------------------
1.9
633
aln×
a
D
----


1.9
---------------------------------
=
a
D
----
Q
ω L×
R
s
-------------
2 π× f× L×
R
s
------------------------------
==

HTCM400/EAE,122

Mfr. #:
Manufacturer:
NXP Semiconductors
Description:
IC RFID READER 125KHZ MODULE
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
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