Data Sheet ADuM2210/ADuM2211
Rev. F | Page 13 of 17
APPLICATIONS INFORMATION
PCB LAYOUT
The ADuM2210/ADuM2211 digital isolator requires no external
interface circuitry for the logic interfaces. Power supply bypassing
is strongly recommended at the input and output supply pins
(see Figure 12). Bypass capacitors are most conveniently connected
between Pin 1 and Pin 3 for V
DD1
and between Pin 14 and Pin 16
for V
DD2
. The capacitor value should be between 0.01 μF and 0.1 μF.
The total lead length between both ends of the capacitor and
the input power supply pin should not exceed 20 mm. Bypassing
between Pin 3 and Pin 7 and between Pin 9 and Pin 14 should
be considered unless the ground pair on each package side is
connected close to the package.
GND
1
NC
V
DD1
V
IA
/V
OA
GND
2
NC
V
DD2
V
OA
/V
IA
V
IB
V
OB
NC
NC
GND
1
NC
NC
GND
2
09233-012
Figure 12. Recommended Printed Circuit Board Layout
In applications involving high common-mode transients, care
should be taken to ensure that board coupling across the isolation
barrier is minimized. Furthermore, the board layout should be
designed such that any coupling that does occur equally affects
all pins on a given component side. Failure to ensure this could
cause voltage differentials between pins exceeding the Absolute
Maximum Ratings of the device, thereby leading to latch-up or
permanent damage.
See the AN-1109 Application Note for board layout guidelines.
PROPAGATION DELAY-RELATED PARAMETERS
Propagation delay is a parameter that describes the length of
time it takes for a logic signal to propagate through a component.
The propagation delay to a logic low output can differ from the
propagation delay to logic high.
INPUT (
V
Ix
)
OUTPUT (V
Ox
)
t
PLH
t
PHL
50%
50%
09233-013
Figure 13. Propagation Delay Parameters
Pulse width distortion is the maximum difference between these
two propagation delay values and is an indication of how
accurately the input signals timing is preserved.
Channel-to-channel matching refers to the maximum amount
the propagation delay differs among channels within a single
ADuM2210/ADuM2211 component.
Propagation delay skew refers to the maximum amount the
propagation delay differs among multiple ADuM2210/ADuM2211
components operated under the same conditions.
DC CORRECTNESS AND MAGNETIC FIELD
IMMUNITY
Positive and negative logic transitions at the isolator input cause
narrow (~1 ns) pulses to be sent via the transformer to the
decoder. The decoder is bistable and is, therefore, either set or
reset by the pulses, indicating input logic transitions. In the
absence of logic transitions at the input for more than ~1 μs, a
periodic set of refresh pulses indicative of the correct input state
is sent to ensure dc correctness at the output. If the decoder
receives no internal pulses for more than approximately 5 μs,
the input side is assumed to be without power or nonfunctional;
in which case, the isolator output is forced to a default state (see
Table 20 and Table 21) by the watchdog timer circuit.
The limitation on the ADuM2210/ADuM2211 magnetic field
immunity is set by the condition in which induced voltage in the
transformer receiving coil is large enough to either falsely set or
reset the decoder. The following analysis defines the conditions
under which this can occur. The 3.3 V operating condition of
the ADuM2210/ADuM2211 is examined because it represents
the most susceptible mode of operation.
The pulses at the transformer output have an amplitude greater
than 1.0 V. The decoder has a sensing threshold at about 0.5 V,
therefore establishing a 0.5 V margin in which induced voltages
can be tolerated. The voltage induced across the receiving coil is
given by
V = (−/dt)Σπr
n
2
; n = 1, 2,…, N
where:
β is the magnetic flux density (gauss).
N is the number of turns in the receiving coil.
r
n
is the radius of the n
th
turn in the receiving coil (cm).
Given the geometry of the receiving coil in the ADuM2210/
ADuM2211 and an imposed requirement that the induced
voltage be at most 50% of the 0.5 V margin at the decoder, a
maximum allowable magnetic field is calculated as shown in
Figure 14.
MAGNETIC FIELD FREQUENCY (Hz)
100
MAXIMUM ALLOWABLE MAGNETIC FLUX
DENSITY (kgauss)
0.001
1M
10
0.01
1k 10k 10M
0.1
1
100M100k
09233-014
Figure 14. Maximum Allowable External Magnetic Flux Density
ADuM2210/ADuM2211 Data Sheet
Rev. F | Page 14 of 17
For example, at a magnetic field frequency of 1 MHz, the
maximum allowable magnetic field of 0.2 kgauss induces a
voltage of 0.25 V at the receiving coil. This is about 50% of the
sensing threshold and does not cause a faulty output transition.
Similarly, if such an event were to occur during a transmitted
pulse (and was of the worst-case polarity), it would reduce the
received pulse from >1.0 V to 0.75 V—still well above the 0.5 V
sensing threshold of the decoder.
The preceding magnetic flux density values correspond to
specific current magnitudes at given distances away from the
ADuM2210/ADuM2211 transformers. Figure 15 expresses
these allowable current magnitudes as a function of frequency
for selected distances. As can be seen, the ADuM2210/ADuM2211
is immune and can be affected only by extremely large currents
operated at high frequency and very close to the component.
For the 1 MHz example noted previously, one would have to
place a 0.5 kA current 5 mm away from the ADuM2210/
ADuM2211 to affect operation of the component.
MAGNETIC FIELD FREQUENCY (Hz)
MAXIMUM ALLOWABLE CURRENT (kA)
1000
100
10
1
0.1
0.01
1k 10k 100M100k 1M 10M
DISTANCE = 5mm
DISTANCE = 1m
DISTANCE = 100mm
09233-015
Figure 15. Maximum Allowable Current
for Various Current-to-ADuM2210/ADuM2211 Spacings
Note that at combinations of strong magnetic field and high
frequency, any loops formed by printed circuit board traces can
induce sufficiently large error voltages to trigger the thresholds
of succeeding circuitry. Care should be taken in the layout of
such traces to avoid this possibility.
POWER CONSUMPTION
The supply current at a given channel of the ADuM2210/
ADuM2211 isolator is a function of the supply voltage, the
channels data rate, and the channel’s output load.
For each input channel, the supply current is given by
I
DDI
= I
DDI (Q)
f ≤ 0.5f
r
I
DDI
= I
DDI (D)
× (2f − f
r
) + I
DDI (Q)
f > 0.5f
r
For each output channel, the supply current is given by
I
DDO
= I
DDO (Q)
f ≤ 0.5f
r
I
DDO
= (I
DDO (D)
+ (0.5 × 10
−3
) × C
L
× V
DDO
) × (2ff
r
) + I
DDO (Q)
f > 0.5f
r
where:
I
DDI (D)
, I
DDO (D)
are the input and output dynamic supply currents
per channel (mA/Mbps).
C
L
is the output load capacitance (pF).
V
DDO
is the output supply voltage (V).
f is the input logic signal frequency (MHz, half of the input data
rate, NRZ signaling).
f
r
is the input stage refresh rate (Mbps).
I
DDI (Q)
, I
DDO (Q)
are the specified input and output quiescent
supply currents (mA).
To calculate the total I
DD1
and I
DD2
, the supply currents for each
input and output channel corresponding to I
DD1
and I
DD2
are
calculated and totaled. Figure 6 and Figure 7 provide per-channel
supply currents as a function of data rate for an unloaded output
condition. Figure 8 provides per-channel supply current as a
function of data rate for a 15 pF output condition. Figure 9
through Figure 11 provide total I
DD1
and I
DD2
as a function of
data rate for ADuM2210/ADuM2211 channel configurations.
Data Sheet ADuM2210/ADuM2211
Rev. F | Page 15 of 17
INSULATION LIFETIME
All insulation structures eventually break down when subjected
to voltage stress over a sufficiently long period. The rate of
insulation degradation is dependent on the characteristics of the
voltage waveform applied across the insulation. In addition to
the testing performed by the regulatory agencies, Analog Devices
carries out an extensive set of evaluations to determine the
lifetime of the insulation structure within the ADuM2210/
ADuM2211.
Analog Devices performs accelerated life testing using voltage levels
higher than the rated continuous working voltage. Acceleration
factors for several operating conditions are determined. These
factors allow calculation of the time to failure at the actual
working voltage. The values shown in Table 19 summarize the
peak voltage for 50 years of service life for a bipolar ac operating
condition and the maximum CSA/VDE approved working volt-
ages. In many cases, the approved working voltage is higher than
a 50-year service life voltage. Operation at these high working
voltages can lead to shortened insulation life in some cases.
The insulation lifetime of the ADuM2210/ADuM2211 depends
on the voltage waveform type imposed across the isolation barrier.
The iCoupler insulation structure degrades at different rates,
depending on whether the waveform is bipolar ac, unipolar ac, or
dc. Figure 16, Figure 17, and Figure 18 illustrate these different
isolation voltage waveforms.
Bipolar ac voltage is the most stringent environment. The goal
of a 50-year operating lifetime under the ac bipolar condition
determines the Analog Devices recommended maximum
working voltage.
In the case of unipolar ac or dc voltage, the stress on the insulation
is significantly lower. This allows operation at higher working
voltages while still achieving a 50-year service life. The working
voltages listed in Table 19 can be applied while maintaining the
50-year minimum lifetime, provided the voltage conforms to
either the unipolar ac or dc voltage cases. Any cross-insulation
voltage waveform that does not conform to Figure 17 or Figure 18
should be treated as a bipolar ac waveform and its peak voltage
should be limited to the 50-year lifetime voltage value listed in
Table 19.
Note that the voltage presented in Figure 17 is shown as sinusoidal
for illustration purposes only. It is meant to represent any voltage
waveform varying between 0 V and some limiting value. The
limiting value can be positive or negative, but the voltage cannot
cross 0 V.
0V
RATED PEAK VOLTAGE
09233-016
Figure 16. Bipolar AC Waveform
0V
RATED PEAK VOLTAGE
09233-017
Figure 17. Unipolar AC Waveform
0V
RATED PEAK VOLTAGE
09233-018
Figure 18. DC Waveform

ADUM2210WTRWZ

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Analog Devices Inc.
Description:
Digital Isolators DUAL-CH DIGITAL ISOLATORS
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