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PDF BL8521 Data sheet ( Hoja de datos )

Número de pieza BL8521
Descripción 3A Synchronous Buck Converter
Fabricantes SHANGHAI BELLING 
Logotipo SHANGHAI BELLING Logotipo



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BL8521
5.5V, 1.4MHz,
3A Synchronous Buck Converter
DESCRIPTION
The BL8521 is a synchronous, 1.4MHz, fix
frequency PWM Buck converter. It is ideal for
powering portable equipment that powered by
a single cell Lithium-ion batter, or USB port.
The BL8521 can provide up to 3A of load
current with output voltage as low as 0.8V. It
can operate at 100% duty cycle for low
dropout application.
With its peak current mode control and
outside compensation, the BL8521 is stable
with ceramic capacitors and small inductors.
BL8521 comprises a cycle-by-cycle current
limit and thermal shutdown to protect itself
from fault application.
BL8521 is available in DFN 3x3 -10 package.
FEATURES
Adjustable Output Voltage, 0.8 - Vin
High efficiency, up to 96%
Output voltage accuracy 2%
0.1ohm Rdson of internal MOSFET
3A maximum output current
Up to 1.5MHz fix switching frequency
5.5V maximum operation voltage
Short circuit protection
Thermal shutdown protection
10mV Load regulation at 3A load
Compatible with ceramic output capacitor
Excellent load transient performance
In-rush current suppression
Reverse current suppression for light load
Available in DFN3x3-10 package
APPLICATIONS
3G network modem
Smart phone, PDA
Digital camera
LCDTV
Portable devices
TYPICAL APPLICATION
REV2.0
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BL8521 pdf
BL8521
5.5V, 1.4MHz, 3A Synchronous Buck Converter
requirements. Dry tantalum, special polymer,
aluminum electrolytic and ceramic capacitors are all
available in surface mount packages. Special
polymer capacitors offer very low ESR but have
lower capacitance density than other types.
Tantalum capacitors have the highest capacitance
density but it is important to only use types that have
been surge tested for use in switching power
supplies. Aluminum electrolytic capacitors have
significantly higher ESR but can be used in cost-
sensitive applications provided that consideration is
given to ripple current ratings and long term
reliability. Ceramic capacitors have excellent low
ESR characteristics but can have a high voltage
coefficient and audible piezoelectric effects. The
high Q of ceramic capacitors with trace inductance
can also lead to significant ringing.
Using Ceramic Input and Output Capacitors
Higher values, lower cost ceramic capacitors are
now becoming available in smaller case sizes. Their
high ripple current, high voltage rating and low ESR
make them ideal for switching regulator applications.
However, care must be taken when these capacitors
are used at the input and output. When a ceramic
capacitor is used at the input and the power is
supplied by a wall adapter through long wires, a load
step at the output can induce ringing at the input, VIN.
At best, this ringing can couple to the output and be
mistaken as loop instability. At worst, a sudden
inrush of current through the long wires can
potentially cause a voltage spike at VIN large enough
to damage the part.
Checking Transient Response
The regulator loop response can be checked by
looking at the load transient response. Switching
regulators take several cycles to respond to a step
in load current. When a load step occurs, VOUT
immediately shifts by an amount equal to ILOAD(ESR),
where ESR is the effective series resistance of COUT.
ILOAD also begins to charge or discharge COUT
generating a feedback error signal used by the
regulator to return VOUT to its steady-state value.
During this recovery time, VOUT can be monitored for
overshoot or ringing that would indicate a stability
problem. The COMP pin external components and
output capacitor shown in Typical Application Circuit
will provide adequate compensation for most
applications.
Efficiency Considerations
The efficiency of a switching regulator is equal to the
output power divided by the input power times 100%.
It is often useful to analyze individual losses to
determine what is limiting the efficiency and which
change would produce the most improvement.
Efficiency can be expressed as :
Efficiency = 100% (L1+ L2+ L3+ ...) where L1, L2,
etc. are the individual losses as a percentage of
input power. Although all dissipative elements in the
circuit produce losses, two main sources usually
account for most of the losses: VDD quiescent
current and I2R losses.
The VDD quiescent current loss dominates the
efficiency loss at very low load currents whereas the
I2R loss dominates the efficiency loss at medium to
high load current. In a typical efficiency plot, the
efficiency curve at very low load currents can be
misleading since the actual power lost is of no
consequence.
1. The VDD quiescent current is due to two
components: the DC bias current as given in the
electrical characteristics and the internal main switch
and synchronous switch gate charge currents. The
gate charge current results from switching the gate
capacitance of the internal power MOSFET switches.
Each time the gate is switched from high to low to
high again, a packet of charge Q moves from VDD
to ground. The resulting Q/t is the current out of
VDD that is typically larger than the DC bias current.
In continuous mode, IGATECHG = f(QT+QB) where QT
and QB are the gate charges of the internal top and
bottom switches.
Both the DC bias and gate charge losses are
proportional to VDD and thus their effects will be
more pronounced at higher supply voltages.
2. I2R losses are calculated from the resistances of
the internal switches, RSW and external inductor RL.
In continuous mode the average output current
flowing through inductor L is choppedbetween the
main switch and the synchronous switch. Thus, the
series resistance looking into the LX pin is a function
of both top and bottom MOSFET RDS(ON) and the
duty cycle (D) as follows :
RSW = RDS(ON)TOP x D + RDS(ON)BOT x (1"D)
The RDS(ON) for both the top and bottom MOSFETs
can be obtained from the Typical Performance
Characteristics curves. Thus, to obtain I2R losses,
simply add RSW to RL and multiply the result by the
square of the average output current. Other losses
including CIN and COUT ESR dissipative losses and
REV2.0
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