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ADP5135ACPZ-R7 数据表(PDF) 21 Page - Analog Devices

部件名 ADP5135ACPZ-R7
功能描述  Triple 1800 mA Buck Regulator with Precision Enables and Power-Good Outputs
PDF  24 Pages
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制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

ADP5135ACPZ-R7 数据表(HTML) 21 Page - Analog Devices

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Data Sheet
ADP5135
Rev. 0 | Page 21 of 24
POWER DISSIPATION AND THERMAL CONSIDERATIONS
The ADP5135 is a highly efficient micro PMU and, in most
cases, the power dissipated in the device is not a concern.
However, if the device operates at high ambient temperatures
and maximum loading conditions, the junction temperature
can reach the maximum allowable operating limit (125°C).
When the temperature exceeds 150°C, the ADP5135 turns off
all the regulators, allowing the device to cool down. When the
die temperature falls below 130°C, the ADP5135 resumes
normal operation.
This section provides guidelines to calculate the power dissi-
pated in the device and to ensure that the ADP5135 operates
below the maximum allowable operating junction temperature.
The efficiency for each regulator on the ADP5135 is given by
100%
IN
OUT
P
P
(1)
where:
η is the efficiency.
POUT is the output power.
PIN is the input power.
Power loss is given by
PLOSS = PIN − POUT
(2a)
or
PLOSS = POUT (1− η)/η
(2b)
Power dissipation can be calculated in several ways. The most
intuitive and practical is to measure the power dissipated at the
input and all the outputs. Perform the measurements at the
worst-case conditions (voltages, currents, and temperature).
The difference between input and output power is dissipated in
the device and the inductor. Use Equation 3 to derive the power
lost in the inductor and, from this, use Equation 7 to calculate
the power dissipation in the ADP5135 buck converter.
A second method to estimate the power dissipation uses the
efficiency curves provided for the buck regulator. When the
buck efficiency is known, use Equation 2b to derive the total
power lost in the buck regulator and inductor, use Equation 3 to
derive the power lost in the inductor, and then calculate the
power dissipation in the buck converter using Equation 7. Add
the power dissipated in the three bucks to find the total
dissipated power.
Note that the buck efficiency curves are typical values and may
not be provided for all possible combinations of VIN, VOUT, and
IOUT. To account for these variations, it is necessary to include a
safety margin when calculating the power dissipated in the buck.
A third way to estimate the power dissipation is analytical and
involves modeling the losses in the buck circuit provided by
Equation 8 to Equation 11.
BUCK REGULATOR POWER DISSIPATION
The inductor losses are external to the device, and they do not
have any effect on the die temperature.
The inductor losses are estimated (without core losses) by
PL ≈ IOUT1(RMS)2 × DCRL
(3)
where:
IOUT1(RMS) is the rms load current of the buck regulator.
DCRL is the inductor series resistance.
12
+
1
)
(
r
I
I
OUT1
RMS
OUT1
(4)
where r is the normalized inductor ripple current.
r = VOUT1 × (1 − D)/(IOUT1 × L × fSW)
(5)
where:
L is the inductance.
fSW is the switching frequency.
D is the duty cycle.
D = VOUT1/VIN1
(6)
The power loss of the buck regulator is approximated by
PLOSS = PDBUCK + PL
(7)
where:
PDBUCK is the power dissipation on one of the ADP5135 buck
regulators.
PL is the inductor power losses.
The ADP5135 buck regulator power dissipation, PDBUCK,
includes the power switch conductive losses, the switch losses, and
the transition losses of each channel. There are other sources of
loss, but these are generally less significant at high output load
currents, where the thermal limit of the application is. Equation 8
captures the calculation that must be made to estimate the
power dissipation in the buck regulator.
PDBUCK = PCOND + PSW + PTRAN
(8)
The power switch conductive losses are due to the output current,
IOUT1, flowing through the P-channel MOSFET and the N-channel
MOSFET power switches that have internal resistance, RDSON_P
and RDSON_N, respectively. The amount of conductive power
loss is found by
PCOND = [RDSON_P × D + RDSON_N × (1 − D)] × IOUT1(RMS)2
(9)
where RDSON_P is approximately 0.19 Ω, RDSON_N is approxi-
mately 0.14 Ω at a 25°C junction temperature, and VIN1 = VIN2 =
3.6 V. At VIN1 = VIN2 = 5.5 V, the values are 0.147 Ω and 0.122 Ω,
respectively.



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