ADP2125
Rev. A | Page 13 of 16
OUTPUT CAPACITOR SELECTION
The output capacitor selection affects both the output voltage
ripple and the loop dynamics of the converter. For a given loop
crossover frequency (the frequency at which the loop gain drops
to 0 dB), the maximum voltage transient excursion (overshoot)
is inversely proportional to the value of the output capacitor.
When choosing output capacitors, it is also important to account
for the loss of capacitance due to output voltage dc bias. This
may result in using a capacitor with a higher rated voltage to
achieve the desired capacitance value. Additionally, if ceramic
output capacitors are used, the capacitor rms ripple current
rating should always meet the application requirements. The
rms ripple current is calculated as follows:
()
)(
)(
32
1
MAXIN
SW
OUT
MAXIN
OUT
COUTRMS VfL
VVV
I××
−×
×= (5)
At nominal load currents, the converter operates in forced
PWM mode, and the overall output voltage ripple is the sum of the
voltage spike caused by the output capacitor ESR plus the voltage
ripple caused by charging and discharging the output capacitor.
VOUT = IL × (ESR + 1/(8 × COUT × fSW)) (6)
The largest voltage ripple occurs at the highest input voltage.
The ADP2125 is designed to operate with small 4.7 µF ceramic
capacitors that have low ESR and ESL. These components are
therefore able to meet tight output voltage ripple specifications.
X5R or X7R dielectrics with a voltage rating of 4 V or higher are
recommended.
THERMAL LIMIT CALCULATIONS
The operating junction temperature (TJ) of the device is
dependent on the ambient operating temperature (TA) of the
application, the power dissipation of the ADP2125 (PD), and the
junction-to-ambient thermal resistance of the package (θJA).
The operating junction temperature (TJ) is calculated using the
following equation:
TJ = TA + (PD × θJA) (7)
where θJA is 120°C/W, as provided in Table 3.
The ADP2125 can be damaged when the operating junction
temperature limits are exceeded. Monitoring ambient tempera-
ture does not guarantee that the junction temperature (TJ) is
within the specified temperature limits.
• In applications with high PD and poor PCB thermal
resistance, the maximum ambient temperature may need
to be derated.
• In applications with moderate PD and good PCB thermal
resistance, the maximum ambient temperature can exceed
the maximum limit as long as the junction temperature is
within specification limits.
The power dissipation (PD) of the ADP2125 is only a portion of
the power loss of the overall application. For a given application
with known operating conditions, the application power loss
can be calculated by combining the following equations for
power loss (PLOSS) and efficiency (η):
PLOSS = PIN − POUT (8)
100×=
IN
OUT
P
P
η
(9)
The resulting equation uses the output power and the efficiency
to determine the PLOSS.
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛−= 1
100
η
OUT
LOSS PP (10)
The power loss calculated using this approach is the combined
loss of the ADP2125 device (PD), the inductor (PL), input
capacitor (PCIN), and the output capacitor (PCOUT), as shown in
the following equation:
PLOSS = PD + PL + PCIN + PCOUT (11)
The power loss for the inductor, input capacitor, and output
capacitor can be calculated as follows:
PL = IRMS2 × DCR (12)
CIN
RMS
CIN ESR
I
P×
⎟
⎠
⎞
⎜
⎝
⎛
=
2
2 (13)
PCOUT = (∆IOUT)2 × ESRCOUT (14)
If multilayer chip capacitors with low ESR are used, the power
loss in the input and output capacitors is negligible and
PD + PL >> PCIN + PCOUT (15)
PLOSS ≈ PD + PL (16)
The final equation for calculating PD can be used in Equation 7
to ensure that the operating junction temperature is not
exceeded.
L
OUT
L
LOSS
DPPPPP −
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛−≈−≈ 1
100
η
(17)