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MICRF505BML Datasheet(PDF) 24 Page - Micrel Semiconductor

Part # MICRF505BML
Description  868MHz and 915MHz ISM Band Transceiver
PDF  27 Pages
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Manufacturer  MICREL [Micrel Semiconductor]
Direct Link  http://www.micrel.com
Logo MICREL - Micrel Semiconductor

MICRF505BML Datasheet(HTML) 24 Page - Micrel Semiconductor

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MICRF505
Micrel
M9999-051304
24
May 13, 2004
Modulator Current
The current used during the rise- and fall times can be
programmed with the Mod_I4..Mod_I0 bit, the last one being
LSB. Figure 15 shows two waveforms generated with two
different currents, where Mod_Ia > Mod_Ib. Higher current
will give a higher frequency deviation and vice versa. The
effect of modulator clock and MOD_1 is illustrated by
To avoid saturation in the modulator it it important not to
exceed maximum Mod_I. Max Mod_I for a given fMOD_clk is
given by:
where min() returns the value of the smallest argument and
int() returns the integer part of the argument.
where int(x): integer and and f_MOD_CLK: Modulater clk
frequency.
Mod_la
Mod_lb
Mod_la > Mod_lb
Figure 17. Two Different Modulator Current Settings
Modulator Attenuator
A third way to set the deviation is by programming the
modulator attenuator, Mod_A2..Mod_A0, the last being LSB.
The purposes of the attenuator is to allow small deviations
when the bit rate is small and/or the BT is small (these settings
will give a relatively slow modulator clock, and therefore long
rise- and fall times, which in turn results in large frequency
deviations). In addition, the attenuator will improve the reso-
lution in the modulator.
Mod_Aa
Mod_Ab
Mod_Ab > Mod_Ab
Figure 18. Two different modulator attenuator settings
The attenuation is given by:
where VMOD2 and VMOD1 is the modulator amplitude after
and before the attenuator, respectively. Figure 16 shows two
waveforms with different attenuator setting; Mod_Aa <
Mod_Ab. If Mod_A is increased, the frequency deviation is
lowered and vice versa.
Modulator Filter
To reduce the high-frequency components in the generated
waveform, a filter with programmable cut-off frequency can
be enabled. This is done using Mod_F2..Mod_F0, the last
one being LSB. The Mod_F should be set according to the
formula:
MOD_F
BitRate
=
¥
150 10
3
Mod_filter on
Mod_filter off
Figure 19. Modulator Waveform with and Without
Filtering
Mod_F=0 disables the modulator filter and Mod_F=7 gives
most filtering. Figure 18 shows a waveform with and without
the filter.
Calculation of the Frequency Deviation
The parameters influencing the frequency deviation can be
summarized in the following equations:
f
f
Refclk_K
2
MOD_CLK
XCO
=
¥ ¥
()
7
Mod
clkS
_
where :
fDEV:
Single sided frequency deviation [Hz]
fXCO:
Crystal oscillator frequency [Hz]
fRF:
Center frequency [Hz]
Refclk_K:
6 bit divider, values between 1 and 63
Mod_clkS:
Modulator clock setting, values
between 0 and 7
fMOD_CLK:
Modulator clock frequency, derived
from the crystal frequency, Refclk_K
and Mod_clkS
Mod_I:
Modulator current setting, values
between 0 and 31
Mod_A:
Modulator attenuator setting, values
between 0 and 15
f
MOD_1
f
DEVIATION
MOD_CLK
a
MOD_Imax
INT(f_MOD_CLK 28e - 6) - 1
=
◊
V
1
1 MOD_A
MOD2
a
+
f
MOD_I
f
1 MOD_A
f
DEV
MOD_CLK
RF
=
◊
+
◊ -
◊◊
()
1
44 28 10 72
9
.



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