ISL97516IUZ-EVALZ Intersil, ISL97516IUZ-EVALZ Datasheet - Page 5

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ISL97516IUZ-EVALZ

Manufacturer Part Number
ISL97516IUZ-EVALZ
Description
EVALUATION BOARD FOR ISL97516IUZ
Manufacturer
Intersil

Specifications of ISL97516IUZ-EVALZ

Main Purpose
DC/DC, Step Up
Outputs And Type
1, Non-Isolated
Voltage - Output
5 ~ 25V
Current - Output
1A
Voltage - Input
2.3 ~ 5.5 V
Regulator Topology
Boost
Board Type
Fully Populated
Utilized Ic / Part
ISL97516
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Power - Output
-
Frequency - Switching
-
Typical Performance Curves
Applications Information
The ISL97516 is a high frequency, high efficiency boost
regulator operated at constant frequency PWM mode. The
boost converter stores energy from an input voltage source
and deliver it to a higher output voltage. The input voltage
range is 2.3V to 5.5V and output voltage range is 5V to 25V.
The switching frequency is selectable between 600kHz and
1.2MHz allowing smaller inductors and faster transient
response. An external compensation pin gives the user
greater flexibility in setting output transient response and
tighter load regulation. The converter soft-start characteristic
can also be controlled by external C
allows the user to completely shutdown the device.
Boost Converter Operations
Figure 10 shows a boost converter with all the key
components. In steady state operating and continuous
conduction mode where the inductor current is continuous,
V
IN
= 3.3V
FIGURE 7. TRANSIENT RESPONSE
V
O
= 12V
f
s
FIGURE 9. PACKAGE POWER DISSIPATION vs AMBIENT TEMPERATURE
5
= 1.2MHz
SS
I
O
capacitor. The EN pin
= 50mA TO 300mA
(Continued)
0.6
0.5
0.4
0.3
0.2
0.1
0.0
0
JEDEC JESD51-3 LOW EFFECTIVE THERMAL
CONDUCTIVITY TEST BOARD
486mW
25
AMBIENT TEMPERATURE (°C)
ISL97516
50
the boost converter operates in two cycles. During the first
cycle, as shown in Figure 11, the internal power FET turns
on and the Schottky diode is reverse biased and cuts off the
current flow to the output. The output current is supplied
from the output capacitor. The voltage across the inductor is
V
the inductance. The inductance is magnetized and energy is
stored in the inductor. The change in inductor current is
shown in Equation 1:
D
ΔI
Δt1
75
ΔV
IN
L1
=
FIGURE 8. PACKAGE POWER DISSIPATION vs AMBIENT
O
85
and the inductor current ramps up in a rate of V
Duty Cycle
=
=
=
--------- -
f
Δt1
SW
D
--------------- -
C
100
I
1.0
0.9
0.8
0.7
0.6
0.5
0.4
0.3
0.2
0.1
OUT
OUT
0
×
0
JEDEC JESD51-7 HIGH EFFECTIVE THERMAL
CONDUCTIVITY TEST BOARD
V
---------
870mW
TEMPERATURE
L
×
IN
Δt
125
1
25
AMBIENT TEMPERATURE (°C)
50
75
85
100
August 27, 2010
125
IN
/L, L is
FN9261.5
(EQ. 1)

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