REV.
ADN8830
–9–
Although the thermistor has a nonlinear relationship to tem-
perature, near optimal linearity over a specified temperature
range can be achieved with the proper value of R
X
. First, the
resistance of the thermistor must be known, where
RRTT
RTT
RTT
THERM T LOW
TMID
T HIGH
==
==
==
1
2
3
@
@
@
(2)
T
LOW
and T
HIGH
are the endpoints of the temperature range and
T
MID
is the average. These resistances can be found in most
thermistor data sheets. In some cases, only the coefficients
corresponding to the Steinhart-Hart equation are given. The
Steinhart-Hart equation is
1
11
3
T
abnR cnR=+
()
+
()
[]
(3)
where T is the absolute temperature of the thermistor in Kelvin
(K = °C + 273.15), and R is the resistance of the thermistor at
that temperature. Based on the coefficients a, b, and c, R
THERM
can be calculated for a given T, albeit somewhat tediously, by
solving the cubic roots of this equation
R
THERM
=++
++
exp
χχ
ψ
χχ
ψ
2427 2427
2
3
1
2
1
3
2
3
1
2
1
3
(4)
where
X
a
T
c
=
1
and
ψ=
b
c
R
X
is then found as
R
RR R R RR
RR R
X
TT T T TT
TT T
=
+
+
12 23 13
13 2
2
2
(5)
For the best accuracy as well as the widest selection range for
resistances, R
X
should be 0.1% tolerance. Naturally, the smaller
the temperature range required for control, the more linear
the voltage divider will be with respect to temperature. The
voltage at THERMIN is
V VREF
R
RR
X
THERM
THERM X
=
+
(6)
where VREF has a typical value of 2.47 V.
The ADN8830 control loop will adjust the temperature of the
TEC until V
X
equals the voltage at TEMPSET (Pin 4), which
we define as V
SET
. Target temperature can be set by
VmTT V
SET MID XMID
=
()
+
(7)
where T equals the target temperature, and
m
VV
TT
X HIGH X LOW
HIGH LOW
=
,,
(8)
V
X
for high, mid, and low are found by using Equation 6 and
substituting R
T3
, R
T2
, and R
T1
, respectively, for R
THERM
. The
variable m is the change in V
X
with respect to temperature and
is expressed in V/°C.
The setpoint voltage can be driven from a DAC or another
voltage source, as shown in Figure 4. The reference voltage
for the DAC should be connected to VREF (Pin 7) on the
ADN8830 to ensure best accuracy from device to device.
For a fixed target temperature, a voltage divider network can be
used as shown in Figure 5. R1 is set equal to R
X
, and R2 is
equal to the value of R
THERM
at the target temperature.
3.3V
ADN8830
8
4
7
30
AD7390
6
85
3.3V
7
1–4
C
Figure 4. Using a DAC to Control the Temperature
Setpoint
3.3V
ADN8830
8
7
4
30
R2
R1
Figure 5. Using a Voltage Divider to Set a Fixed
Temperature Setpoint
Design Example 1
A laser module requires a constant temperature of 25°C. From
the manufacturer’s data sheet, we find the thermistor in the laser
module has a value of 10 kΩ at 25°C. Because the laser is not
required to operate at a range of temperatures, the value of R
X
can be set to 10 kΩ. TEMPSET can be set by a simple resistor
divider as shown in Figure 5, with R1 and R2 both equal to 10 kΩ.
Design Example 2
A laser module requires a continuous temperature control from
5°C to 45°C. The manufacturer’s data sheet shows the thermistor
has a value of 10 kΩ at 25°C, 25.4 kΩ at 5°C, and 4.37 kΩ at
45°C. Using Equation 5, R
X
is calculated to be 7.68 kΩ to yield
the most linear temperature-to-voltage conversion. A DAC
will be used to set the TEMPSET voltage.
DAC Resolution for TEMPSET
The temperature setpoint voltage to THERMIN can be set from
a DAC. The DAC must have a sufficient number of bits to achieve
adequate temperature resolution from the system. The voltage
range for THERMIN is found by multiplying the variable m
from Equation 8 by the temperature range.
THERMIN Voltage Range m T T
MAX MIN
()
(9)
From Design Example 2, 40°C of the control temperature range
is achieved with a voltage range of only 1 V.
D
REV. –10–
ADN8830
To eliminate the resolution of the DAC as the principal source
of system error, the step size of each bit, V
STEP
, should be lower
than the desired system resolution. A practical value for absolute
DAC resolution is the equivalent of 0.05°C. The value of V
STEP
should be less than the value of m from Equation 8 multiplied
by the desired temperature resolution, or
VCm
STEP
×005.
(10)
where m is the slope of the voltage-to-temperature conversion
line, as found from Equation 8. From Design Example 2, where
m = 25 mV/°C, we see the DAC should have resolution better
than 1.25 mV per step.
The minimum number of bits required is then given as
Number of Bits
VV
FS STEP
=
() ( )
()
log – log
log 2
(11)
where V
FS
is the full-scale output voltage from the DAC, which
should be equal to the reference voltage from the ADN8830,
VREF = 2.47 V as given in the Specifications table for the
Reference Voltage. In this example, the minimum resolution is
11 bits. A 12-bit DAC, such as the AD7390, can be readily
found.
It is important that the full-scale voltage input to the DAC is tied
to the ADN8830 reference voltage, as shown in Figure 4. This
eliminates errors from slight variances of VREF.
Thermistor Fault and Temperature Lock Indications
Both the THERMFAULT (Pin 1) and TEMPLOCK (Pin 5)
outputs are CMOS compatible outputs that are active high.
THERMFAULT will be a logic low while the thermistor is
operating normally and will go to a logic high if a short or
open is detected at THERMIN (Pin 2). The trip voltage for
THERMFAULT is when THERMIN falls below 0.2 V or
exceeds 2.0 V. THERMFAULT provides only an indication of
a fault condition and does not activate any shutdown or protec-
tion circuitry on the ADN8830. To shut down the ADN8830, a
logic low voltage must be asserted on Pin 3, as described in the
Shutdown Mode section.
TEMPLOCK will output a logic high when the voltage at
THERMIN is within 2.5 mV of TEMPSET. This voltage can
be related to temperature by solving for m from Equation 8. For
most laser diode applications, 2.5 mV is equivalent to ±0.1°C.
If the voltage difference between THERMIN and TEMPSET is
greater than 2.5 mV, then TEMPLOCK will output a logic low.
The input offset voltage of the ADN8830 is guaranteed to within
250 μV, which for most applications is within ±0.01°C.
Setting the Switching Frequency
The ADN8830 has an internal oscillator to generate the switch-
ing frequency for the output stage. This oscillator can be either
set in free-run mode or synchronized to an external clock
signal. For free-run operation, SYNCIN (Pin 25) should be
connected to ground and COMPOSC (Pin 24) should be
connected to AVDD. The switching frequency is then set by a
single resistor connected from FREQ (Pin 26) to ground.
Table I shows R
FREQ
for some common switching frequencies.
Table I. Switching Frequencies vs. R
FREQ
f
SWITCH
R
FREQ
100 kHz 1.5 MΩ
250 kHz 600 kΩ
500 kHz 300 kΩ
750 kHz 200 kΩ
1 MHz 150 kΩ
For other frequencies, the value for this resistor, R
FREQ
, should
be set to
R
f
FREQ
SWITCH
=
×150 10
9
(12)
where f
SWITCH
is the switching frequency in Hz.
Higher switching frequencies reduce the voltage ripple across
the TEC. However, high switch frequencies will create more
power dissipation in the external transistors. This is due to the
more frequent charging and discharging of the transistors’ gate
capacitances. If large transistors are needed for a high output
current application, faster switching frequencies could reduce
the overall power efficiency of the circuit. This is covered in
detail in the Calculating Power Dissipation and Efficiency section.
The switching frequency of the ADN8830 can be synchronized
with an external clock by connecting the clock signal to SYNCIN
(Pin 25). Pin 24 should also be connected to an R-C network, as
shown in Figure 6. This network is simply used to compensate a
PLL to lock on to the external clock. To ensure the quickest
synchronization lock-in time, R
FREQ
should be set to 1.5 MΩ.
ADN8830
FREQ
COMPOSC
1.5M
26
24
0.1F
1k
1nF
Figure 6. Using an R-C Network on Pin 24 with
an External Clock
The relative phase of the ADN8830 internal oscillator compared
to the external clock signal can be adjusted. This is accomplished
by adjusting the voltage to PHASE (Pin 29) according to TPCs 3
and 4. The phase shift versus voltage can be approximated as
Phase Shift
V
VREF
PHASE
°= °×360
(13)
where V
PHASE
is the voltage at Pin 29, and VREF has a typical
value of 2.47 V.
To ensure the oscillator operates correctly, V
PHASE
should remain
higher than 100 mV and lower than 2.3 V. This is required for
either internal clock or external synchronization operation. A
resistor divider from VREF to ground can establish this voltage
easily, although any voltage source, such as a DAC, could be used
as well. If phase is not a consideration, for example with a single
ADN8830 being used, Pin 29 can be tied to Pin 6, which pro-
vides a 1.5 V reference voltage.
D
REV.
ADN8830
–11–
The phase adjusted output from the ADN8830 is available at
SYNCOUT (Pin 28). This pin can be used as a master clock
signal for driving other ADN8830 devices. Multiple ADN8830
devices can be either driven from a single master ADN8830
device by connecting its SYNCOUT pin to each slave’s SYNCIN
pin or daisy-chained by connecting each device’s SYNCOUT to
the next device’s SYNCIN pin.
Phase shifting is useful in systems that use more than one
ADN8830 TEC controller. It ensures the ADN8830 devices
will not switch at the same time, which could create excessive
ripple on the power supply voltage. By adjusting the phase of
each device, the switching transients can be spaced equally over
the clock period, reducing potential supply ripple and easing the
instantaneous current demand from the supply.
Using a single master clock, each slave ADN8830 should have a
different value phase shift. For example, with four TEC con-
trollers, one slave device should be set for 90° of phase shift,
another for 180°, and the last for 270°. In a daisy-chain configu-
ration, each slave device would be set with equal phase. Using
the previous example, each slave would be set to 90° with its
SYNCOUT pin connected to the next device’s SYNCIN pin.
Examples are shown in Figures 7 and 8.
0.1F
1k
1nF
24
1.5M
0.1F
1k
1nF
24
ADN8830
SLAVE
25
29
26
28
100k
7
100k
NC
ADN8830
MASTER
25
29 26
R
FREQ
28
ADN8830
SLAVE
25
29 26
1.5M
0.1F
1k
1nF
24
28
50k
7
150k
NC
ADN8830
SLAVE
25
29 26
28
150k
7
50k
NC
6
V
DD
24
Figure 7. Multiple ADN8830 Devices Driven from
a Master Clock
Soft Start on Power-Up
The ADN8830 can be programmed to ramp up for a specified
time after the power supply is applied or after shutdown is
de-asserted. This feature, known as soft start, is useful for
gradually increasing the duty cycle of the PWM amplifier. The
soft start time is set with a single capacitor connected from Pin 27
to ground according to Equation 14.
τ
SS SS
C150
(14)
where C
SS
is the value of the capacitor in microfarads, and
SS
is
the soft start time in milliseconds. To set a soft start time of 15 ms,
C
SS
should equal 0.1 μF. A minimum soft start time of 10 ms is
recommended to ensure proper initialization of the ADN8830
on power-up.
Shutdown Mode
The ADN8830 has a shutdown mode that deactivates the output
stage and puts the device into a low current standby state. The
current draw for the ADN8830 in shutdown is less than 100 μA.
The shutdown input, Pin 3, is active low. To shut down the
device, Pin 3 should be driven to logic low. Once a logic high is
applied, the ADN8830 will reactivate after the delay set by the
soft start circuitry. Refer to the Soft Start on Power-Up section
for more details on this feature.
Pin 3 should not be left floating as there are no internal pull-up
or pull-down resistors. If the shutdown function is not required,
Pin 3 should be tied to V
DD
to ensure the device is always active.
Compensation Loop
The ADN8830 TEC controller has a built-in amplifier dedicated
for loop compensation. The exact compensation network is set
by the user and can vary from a simple integrator to PI, PID, or
any other type of network. The type of compensation and com-
ponent values should be determined by the user since it will
depend on the thermal response of the object and the TEC. One
method for determining these values empirically is to input a step
function to TEMPSET, thus changing the target temperature,
and adjusting the compensation network to minimize the set-
tling time of the object’s temperature.
A typical compensation network used for temperature control
of a laser module is a PID loop, which consists of a very low
frequency pole and two separate zeros at higher frequencies.
Figure 9 shows a simple network for implementing PID com-
pensation. An additional pole is added at a higher frequency
than the zeros to reduce the noise sensitivity of the control loop.
The bode plot of the magnitude is shown in Figure 10.
29
6
ADN8830
MASTER
25
NC
26
R
FREQ
ADN8830
SLAVE
25
29 26
1.5M
28
50k
7
150k
28
25
29 26
1.5M
28
50k
7
150k
25
29 26
1.5M
28
50k
7
150k
NC
V
DD
24
242424
1k
0.1F
1nF
1k
0.1F
1nF
1k
0.1F
1nF
ADN8830
SLAVE
ADN8830
SLAVE
Figure 8. Multiple ADN8830 Devices Using a Daisy Chain
D

ADN8830ACPZ-REEL7

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Laser Drivers HIGH PRECISION/EFFICIENCY TEC CONTROLLER
Lifecycle:
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