The MAX7031 crystal-based, fractional-N transceiver is
designed to transmit and receive FSK data at factorypreset carrier frequencies of 308MHz†, 315MHz, or
433.92MHz with data rates up to 33kbps (Manchester
encoded) or 66kbps (NRZ encoded). This device generates a typical output power of +10dBm into a 50Ω
load, and exhibits typical sensitivity of -110dBm. The
MAX7031 features separate transmit and receive pins
(PAOUT and LNAIN) and provides an internal RF switch
that can be used to connect the transmit and receive
pins to a common antenna.
The MAX7031 transmit frequency is generated by a 16bit, fractional-N, phase-locked loop (PLL), while the
receiver’s local oscillator (LO) is generated by an integer-N PLL. This hybrid architecture eliminates the need
for separate transmit and receive crystal reference
oscillators because the fractional-N PLL is preset to be
10.7MHz above the receive LO. Retaining the fixed-N
PLL for the receiver avoids the higher current-drain
requirements of a fractional-N PLL and keeps the
receiver current drain as low as possible.
The fractional-N architecture of the MAX7031 transmit
PLL allows the transmit FSK signal to be preset for
exact frequency deviations, and completely eliminates
the problems associated with oscillator-pulling FSK signal generation. All frequency-generation components
are integrated on-chip, and only a crystal, a 10.7MHz IF
filter, and a few discrete components are required to
implement a complete antenna/digital data solution.
The MAX7031 is available in a small, 5mm x 5mm, 32pin, thin QFN package, and is specified to operate in
the automotive -40°C to +125°C temperature range.
Stresses beyond those listed under “Absolute Maximum Ratings” may cause permanent damage to the device. These are stress ratings only, and functional
operation of the device at these or any other conditions beyond those indicated in the operational sections of the specifications is not implied. Exposure to
absolute maximum rating conditions for extended periods may affect device reliability.
HVIN to GND .........................................................-0.3V to +6.0V
PAVDD, AVDD, DVDD to GND..............................-0.3V to +4.0V
ENABLE, T/R, DATA, AGC0, AGC1,
AUTOCAL to GND ...............................-0.3V to (V
HVIN
+ 0.3)V
All Other Pins to GND .............................-0.3V to (V
= -40°C to +125°C, unless otherwise noted. Typical values are at V
PAV
DD
= V
AV
DD
= V
DV
DD
= V
HV
IN
= +2.7V,
T
A
= +25°C, unless otherwise noted.) (Note 1)
Note 1: Supply current, output power, and efficiency are greatly dependent on board layout and PAOUT match.
Note 2: 100% tested at T
A
= +125°C. Guaranteed by design and characterization over temperature.
Note 3: Guaranteed by design and characterization. Not production tested.
Note 4: Time for final signal detection; does not include baseband filter settling.
Note 5: Efficiency = P
OUT
/(VDDx IDD).
Note 6: Dependent on PCB trace capacitance.
Note 7: Input impedance is measured at the LNAIN pin. Note that the impedance at 315MHz includes the 12nH inductive degenera-
tion from the LNA source to ground. The impedance at 434MHz includes a 10nH inductive degeneration connected from the
LNA source to ground. The equivalent input circuit is 50Ω in series with ~2.2pF. The voltage conversion is measured with
the LNA input-matching inductor, the degeneration inductor, and the LNA/mixer tank in place, and does not include the IF
filter insertion loss.
Typical Operating Characteristics
(
Typical Operating Circuit
, V
PAVDD
= V
AVDD
= V
DVDD
= V
HVIN
= +3.0V, fRF= 433.92MHz, IF BW = 280kHz. 4kbps Manchester
Power-Amplifier Supply Voltage. Bypass to GND with 0.01µF and 220pF capacitors placed as close
as possible to the pin.
Envelope-Shaping Output. ROUT controls the power-amplifier envelope’s rise and fall times. Connect
ROUT to the PA pullup inductor or optional power-adjust resistor. Bypass the inductor to GND as
close as possible to the inductor with 680pF and 220pF capacitors as shown in the TypicalApplication Circuit.
Transmit/Receive Switch Throw. Drive T/R high to short TX/RX1 to TX/RX2. Drive T/R low to disconnect
TX/RX1 from TX/RX2. Functionally identical to TX/RX2.
Power-Amplifier Output. Requires a pullup inductor to the supply voltage (or ROUT if envelope
shaping is desired), which can be part of the output-matching network to an antenna.
Analog Power-Supply Voltage. AVDD is connected to an on-chip +3.0V regulator in 5V operation.
Bypass AVDD to GND with a 0.1µF and 220pF capacitor placed as close as possible to the pin.
Low-Noise Amplifier Source for External Inductive Degeneration. Connect an inductor to GND to set
the LNA input impedance.
Low-Noise Amplifier Output. Must be connected to AVDD through a parallel LC tank filter. AC-couple
to MIXIN+.
Transmit/Receive. Drive high to put the device in transmit mode. Drive low or leave unconnected to
put the device in receive mode. It is internally pulled down.
Enable. Drive high for normal operation. Drive low or leave unconnected to put the device into
shutdown mode.
Digital Power-Supply Voltage. Bypass to GND with a 0.01µF and 220pF capacitor placed as close as
possible to the pin.
High-Voltage Supply Input. For 3V operation, connect HVIN to AVDD, PAVDD, and DVDD. For 5V
operation, connect only HVIN to 5V. Bypass HVIN to GND with a 0.01µF and 220pF capacitor placed
as close as possible to the pin.
The MAX7031 308MHz, 315MHz, and 433.92MHz
CMOS transceiver and a few external components provide a complete transmit and receive chain from the
antenna to the digital data interface. This device is
designed for transmitting and receiving FSK data. All
transmit frequencies are generated by a fractional-Nbased synthesizer, allowing for very fine frequency
steps in increments of f
XTAL
/4096. The receive local
oscillator (LO) is generated by a traditional integer-Nbased synthesizer. Depending on component selection, data rates as high as 33kbps (Manchester
encoded) or 66kbps (NRZ encoded) can be achieved.
Receiver
Low-Noise Amplifier (LNA)
The LNA is a cascode amplifier with off-chip inductive
degeneration that achieves approximately 30dB of voltage gain that is dependent on both the antenna-matching network at the LNA input, and the LC tank network
between the LNA output and the mixer inputs.
The off-chip inductive degeneration is achieved by connecting an inductor from LNASRC to AGND. This inductor sets the real part of the input impedances at LNAIN,
allowing for a more flexible match for low-input impedances such as a PCB trace antenna. A nominal value
for this inductor with a 50Ω input impedance is 12nH at
315MHz and 10nH at 434MHz, but the inductance is
affected by PCB trace length. LNASRC can be shorted
to ground to increase sensitivity by approximately 1dB,
but the input match must then be reoptimized.
The LC tank filter connected to LNAOUT consists of L5
and C9 (see the
Typical Application Circuit
). Select L5
and C9 to resonate at the desired RF input frequency.
The resonant frequency is given by:
where L
TOTAL
= L5 + L
PARASITICS
and C
TOTAL
= C9 +
C
PARASITICS
.
L
PARASITICS
and C
PARASITICS
include inductance and
capacitance of the PCB traces, package pins, mixer
input impedance, LNA output impedance, etc. These
parasitics at high frequencies cannot be ignored, and
can have a dramatic effect on the tank filter center frequency. Lab experimentation should be done to optimize the center frequency of the tank. The parasitic
capacitance is generally 5pF to 7pF.
Automatic Gain Control (AGC)
When the AGC is enabled, it monitors the RSSI output.
When the RSSI output reaches 1.28V, which corresponds to an RF input level of approximately -55dBm,
the AGC switches on the LNA gain-reduction attenuator. The attenuator reduces the LNA gain by 36dB,
thereby reducing the RSSI output by about 540mV to
740mV. The LNA resumes high-gain mode when the
RSSI output level drops back below 680mV (approximately -59dBm at the RF input) for a programmable
interval called the AGC dwell time (see Table 1). The
AGC has a hysteresis of approximately 4dB. With the
AGC function, the RSSI dynamic range is increased.
AGC is not necessary for most FSK applications.
AGC Dwell Time Settings
The AGC dwell timer holds the AGC in a low-gain state
for a set amount of time after the power level drops
below the AGC switching threshold. After that set
amount of time, if the power level is still below the AGC
threshold, the LNA goes into high-gain state.
Pin Description (continued)
PINNAMEFUNCTION
28AUTOCALEnable (Logic-High) to Allow FSK Demodulator Calibration. Bypass to GND with a 10pF capacitor.
29AGC1AGC Enable/Dwell Time Control 1. See Table 1. Bypass to GND with a 10pF capacitor.
30AGC0AGC Enable/Dwell Time Control 0 (LSB). See Table 1. Bypass to GND with a 10pF capacitor.
31XTAL1Crystal Input 1. Bypass to GND if XTAL2 is driven by an AC-coupled external reference.
32XTAL2Crystal Input 2. XTAL2 can be driven from an external AC-coupled reference.
—EPExposed Pad. Solder evenly to the board’s ground plane for proper operation.
The MAX7031 uses the two AGC control pins (AGC0
and AGC1) to enable or disable the AGC and set three
user-controlled dwell timer settings. The AGC dwell
time is dependent on the crystal frequency and the bit
settings of the AGC control pins. To calculate the dwell
time, use the following equation:
where K is an integer in decimal, determined by the
control pin settings shown in Table 1.
For example, a receiver operating at 315MHz has a
crystal oscillator frequency of 12.679MHz. For K = 11
(AGC setting = 0, 1), the dwell timer is 162µs; for K =
14 (AGC setting = 1, 0), the dwell timer is 1.3ms; for K
= 20 (AGC setting = 1, 1), the dwell time is 83ms.
Mixer
A unique feature of the MAX7031 is the integrated
image rejection of the mixer. This eliminates the need
for a costly front-end SAW filter for many applications.
The advantage of not using a SAW filter is increased
sensitivity, simplified antenna matching, less board
space, and lower cost.
The mixer cell is a pair of double-balanced mixers that
perform an IQ downconversion of the RF input to the
10.7MHz intermediate frequency (IF) with low-side
injection (i.e., f
LO
= fRF- fIF). The image-rejection circuit
then combines these signals to achieve a typical 46dB
of image rejection over the full temperature range. Lowside injection is required as high-side injection is not
possible due to the on-chip image rejection. The IF output is driven by a source follower, biased to create a
driving impedance of 330Ω to interface with an off-chip
330Ω ceramic IF filter. The voltage conversion gain driving a 330Ω load is approximately 20dB. Note that the
MIXIN+ and MIXIN- inputs are functionally identical.
Integer-N, Phase-Locked Loop (PLL)
The MAX7031 utilizes a fixed integer-N PLL to generate
the receive LO. All PLL components, including the loop
filter, voltage-controlled oscillator, charge pump, asynchronous 24x divider, and phase-frequency detector
are internal. The loop bandwidth is approximately
500kHz. The relationship between RF, IF, and reference
frequencies is given by:
f
REF
= (f
RF
- fIF)/24
Intermediate Frequency (IF)
The IF section presents a differential 330Ω load to provide matching for the off-chip ceramic filter. The internal
six AC-coupled limiting amplifiers produce an overall
gain of approximately 65dB, with a bandpass filter-type
response centered near the 10.7MHz IF frequency with
a 3dB bandwidth of approximately 10MHz. The RSSI
circuit demodulates the IF to baseband by producing a
DC output proportional to the log of the IF signal level
with a slope of approximately 15mV/dB.
FSK Demodulator
The FSK demodulator uses an integrated 10.7MHz PLL
that tracks the input RF modulation and converts the
frequency deviation into a voltage difference. The PLL
is illustrated in Figure 1. The input to the PLL comes
from the output of the IF limiting amplifiers. The PLL
control voltage responds to changes in the frequency
of the input signal with a nominal gain of 2.0mV/kHz.
For example, an FSK peak-to-peak deviation of 50kHz
signal on the control line. This
control voltage is then filtered and sliced by the baseband circuitry.
The FSK demodulator PLL requires calibration to overcome variations in process, voltage, and temperature.
This is done by cycling the ENABLE pin when the
AUTOCAL pin is a logic 1. If the AUTOCAL pin is a
logic 0, calibration cannot occur.
Data Filter
The data filter for the demodulated data is implemented
as a 2nd-order, lowpass Sallen-Key filter. The pole
locations are set by the combination of two on-chip
resistors and two external capacitors. Adjusting the
value of the external capacitors changes the corner frequency to optimize for different data rates. Set the corner frequency in kHz to approximately 2 times the
fastest expected Manchester data rate in kbps from the
transmitter (1.0 times the fastest expected NRZ data
rate). Keeping the corner frequency near the data rate
rejects any noise at higher frequencies, resulting in an
increase in receiver sensitivity.
The configuration shown in Figure 2 can create a
Butterworth or Bessel response. The Butterworth filter
offers a very-flat-amplitude response in the passband
and a rolloff rate of 40dB/decade for the two-pole filter.
The Bessel filter has a linear phase response, which
works well for filtering digital data. To calculate the
value of the capacitors, use the following equations,
along with the coefficients in Table 2:
where fCis the desired 3dB corner frequency.
For example, choose a Butterworth filter response with
a corner frequency of 5kHz:
Choosing standard capacitor values changes CF1to
470pF and CF2to 220pF. In the
Typical Application
Circuit
, CF1and CF2are named C16 and C17,
respectively.
Table 2. Coefficients to Calculate C
F1
and C
F2
Figure 3. Generating Data Slicer Threshold Using a Lowpass
Filter
Figure 4. Generating Data Slicer Threshold Using the Peak
Detectors
The data slicer takes the analog output of the data filter
and converts it to a digital signal. This is achieved by
using a comparator and comparing the analog input to
a threshold voltage. The threshold voltage is set by the
voltage on the DS- pin, which is connected to the negative input of the data-slicer comparator.
Numerous configurations can be used to generate the
data-slicer threshold. For example, the circuit in Figure
3 shows a simple method using only one resistor and
one capacitor. This configuration averages the analog
output of the filter and sets the threshold to approximately 50% of that amplitude. With this configuration,
the threshold automatically adjusts as the analog signal
varies, minimizing the possibility for errors in the digital
data. The values of R and C affect how fast the threshold tracks the analog amplitude. Be sure to keep the
corner frequency of the RC circuit much lower (about
10 times) than the lowest expected data rate.
With this configuration, a long string of NRZ zeros or
ones can cause the threshold to drift. This configuration
works best if a coding scheme, such as Manchester
coding, which has an equal number of zeros and ones,
is used.
Figure 4 shows a configuration that uses the positive and
negative peak detectors to generate the threshold. This
configuration sets the threshold to the midpoint between
a high output and a low output of the data filter.
Peak Detectors
The maximum peak detector (PDMAX) and minimum
peak detector (PDMIN), with resistors and capacitors
shown in Figure 4, create DC output voltages equal to
the high- and low-peak values of the filtered demodulated signal. The resistors provide a path for the capacitors to discharge, allowing the peak detectors to
dynamically follow peak changes of the data filter output voltages.
The maximum and minimum peak detectors can be
used together to form a data slicer threshold voltage at
a value midway between the maximum and minimum
voltage levels of the data stream (see the
Data Slicer
section and Figure 4). Set the RC time constant of the
peak-detector combining network to at least 5 times the
data period.
If there is an event that causes a significant change in
the magnitude of the baseband signal, such as an AGC
gain switch or a power-up transient, the peak detectors
may “catch” a false level. If a false peak is detected,
the slicing level is incorrect. The MAX7031 peak detectors correct these problems by temporarily tracking the
incoming baseband filter voltage when an AGC state
switch occurs, or by forcing the peak detectors to track
the baseband filter output voltage until all internal circuits are stable following an enable pin low-to-high
transition. The peak detectors exhibit a fast attack/slow
decay response. This feature allows for an extremely
fast startup or AGC recovery.
Transmitter
Power Amplifier (PA)
The PA of the MAX7031 is a high-efficiency, opendrain, switch-mode amplifier. The PA with proper output- matching network can drive a wide range of
antenna impedances, which includes a small-loop PCB
trace and a 50Ω antenna. The output-matching network
for a 50Ω antenna is shown in the
Typical Application
Circuit
. The output-matching network suppresses the
carrier harmonics and transforms the antenna impedance to an optimal impedance at PAOUT (pin 5). The
optimal impedance at PAOUT is 250Ω.
When the output-matching network is properly tuned,
the PA transmits power with a high overall efficiency of
up to 32%. The efficiency of the PA itself is more than
46%. The output power is set by an external resistor at
PAOUT, and is also dependent on the external antenna
and antenna-matching network at the PA output.
Envelope Shaping
The MAX7031 features an internal envelope-shaping
resistor, which connects between the open-drain output
of the PA and the power supply. The envelope-shaping
resistor slows the turn-on/turn-off of the PA. Envelope
shaping is not necessary for FSK. For most applications, the PA pullup inductor should be connected to
PAVDD instead of ROUT.
Fractional-N Phase-Locked Loop (PLL)
The MAX7031 utilizes a fully integrated, fractional-N
PLL for its transmit frequency synthesizer. All PLL components, including the loop filter, are integrated internally. The loop bandwidth is approximately 200kHz.
Power-Supply Connections
The MAX7031 can be powered from a 2.1V to 3.6V supply or a 4.5V to 5.5V supply. If a 4.5V to 5.5V supply is
used, then the on-chip linear regulator reduces the 5V
supply to the 3V needed to operate the chip.
To operate the MAX7031 from a 3V supply, connect
PAVDD, AVDD, DVDD, and HVIN to the 3V supply.
When using a 5V supply, connect the supply to HVIN
only and connect AVDD, PAVDD, and DVDD together.
In both cases, bypass PAVDD, DVDD, and HVIN to
GND with a 0.01µF and 220pF capacitor and bypass
AVDD to GND with a 0.1µF and 220pF capacitor.
Bypass T/R, ENABLE, DATA, AGC0-1, and AUTOCAL
with 10pF capacitors to GND. Place all bypass capacitors as close to the respective pins as possible.
Transmit/Receive Antenna Switch
The MAX7031 features an internal SPST RF switch that,
when combined with a few external components, allows
the transmit and receive pins to share a common antenna (see the
Typical Application Circuit)
. In receive
mode, the switch is open and the power amplifier is
shut down, presenting a high impedance to minimize
the loading of the LNA. In transmit mode, the switch
closes to complete a resonant tank circuit at the PA output and forms an RF short at the input to the LNA. In
this mode, the external passive components couple the
output of the PA to the antenna to protect the LNA input
from strong transmitted signals.
The switch state is controlled by the T/R pin (pin 22).
Drive T/R high to put the device in transmit mode; drive
T/R low to put the device in receive mode.
Crystal Oscillator (XTAL)
The XTAL oscillator in the MAX7031 is designed to present a capacitance of approximately 3pF between the
XTAL1 and XTAL2 pins. In most cases, this corresponds to a 4.5pF load capacitance applied to the
external crystal when typical PCB parasitics are added.
It is very important to use a crystal with a load
capacitance that is equal to the capacitance of the
MAX7031 crystal oscillator plus PCB parasitics. If a
crystal designed to oscillate with a different load
capacitance is used, the crystal is pulled away from its
stated operating frequency, introducing an error in the
reference frequency. Crystals designed to operate with
higher differential load capacitance always pull the reference frequency higher.
In actuality, the oscillator pulls every crystal. The crystal’s natural frequency is really below its specified frequency, but when loaded with the specified load
capacitance, the crystal is pulled and oscillates at its
specified frequency. This pulling is already accounted
for in the specification of the load capacitance.
Additional pulling can be calculated if the electrical
parameters of the crystal are known. The frequency
pulling is given by:
where:
f
P
is the amount the crystal frequency is pulled in ppm.
For the latest package outline information and land patterns, go to www.maxim-ic.com/packages. Note that a “+”, “#”, or “-” in the
package code indicates RoHS status only. Package drawings may show a different suffix character, but the drawing pertains to the
package regardless of RoHS status.
MAX7031
Low-Cost, 308MHz, 315MHz, and 433.92MHz
FSK Transceiver with Fractional-N PLL
Maxim cannot assume responsibility for use of any circuitry other than circuitry entirely embodied in a Maxim product. No circuit patent licenses are
implied. Maxim reserves the right to change the circuitry and specifications without notice at any time.
20
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