参数资料
型号: ZL6100EVAL1Z
厂商: Intersil
文件页数: 18/34页
文件大小: 0K
描述: EVAL BOARD USB ZL6100
标准包装: 1
系列: *
ZL6100
As a starting point, apportion one-half of the output ripple
voltage to the capacitor ESR and the other half to
r DS(ON) of QL (lower output voltages and higher step-down
ratios will be closer to 5%):
C OUT =
8 × f sw ×
V orip
P QL = 0 . 05 × V OUT × I OUT
I botrms = I Lrms × 1 ? D
capacitance, as shown in Equations 10 and 11:
I opp
V orip
2
ESR =
2 × I opp
(EQ. 10)
(EQ. 11)
(EQ. 14)
Calculate the RMS current in QL as shown in Equation 15:
(EQ. 15)
Calculate the desired maximum r DS(ON) as shown in
Equation 16:
Use these values to make an initial capacitor selection, using
a single capacitor or several capacitors in parallel.
After a capacitor has been selected, the resulting output
R DS ( ON ) =
P QL
( I botrms ) 2
(EQ. 16)
voltage ripple can be calculated using Equation 12:
Note that the r DS(ON) given in the manufacturer ’s datasheet
V orip = I opp × ESR +
I opp
8 × f sw × C OUT
(EQ. 12)
is measured at +25°C. The actual r DS(ON) in the end-use
application will be much higher. For example, a Vishay
Si7114 MOSFET with a junction temperature of +125°C has
an r DS(ON) that is 1.4x higher than the value at +25°C. Select
I g = f SW × Q g
I CINrms = I OUT × D × ( 1 ? D )
P QL = f sw × Q g × V INM
Because each part of this equation was made to be less than
or equal to half of the allowed output ripple voltage, the V orip
should be less than the desired maximum output ripple.
INPUT CAPACITOR
It is highly recommended that dedicated input capacitors be
used in any point-of-load design, even when the supply is
powered from a heavily filtered 5V or 12V “bulk” supply from
an off-line power supply. This is because of the high RMS
ripple current that is drawn by the buck converter topology.
This ripple (I CINrms ) can be determined from Equation 13:
(EQ. 13)
Without capacitive filtering near the power supply circuit, this
current would flow through the supply bus and return planes,
coupling noise into other system circuitry. The input capacitors
should be rated at 1.2x the ripple current calculated above to
avoid overheating of the capacitors due to the high ripple
current, which can cause premature failure. Ceramic
capacitors with x7R or x5R dielectric with low ESR and 1.1x
the maximum expected input voltage are recommended.
a candidate MOSFET, and calculate the required gate drive
current as shown in Equation 17:
(EQ. 17)
Keep in mind that the total allowed gate drive current for both
QH and QL is 80mA.
MOSFETs with lower r DS(ON) tend to have higher gate
charge requirements, which increases the current and
resulting power required to turn them on and off. Since the
MOSFET gate drive circuits are integrated in the ZL6100,
this power is dissipated in the ZL6100 according to
Equation 18:
(EQ. 18)
QH SELECTION
In addition to the r DS(ON) loss and gate charge loss, QH also
has switching loss. The procedure to select QH is similar to
the procedure for QL. First, assign 2% to 5% of the output
power to be dissipated in the r DS(ON) of QH using
Equation 18. As was done with QL, calculate the RMS
current as shown in Equation 19:
BOOTSTRAP CAPACITOR SELECTION
The high-side driver boost circuit utilizes an external Schottky
I toprms = I Lrms × D
(EQ. 19)
diode (D B ) and an external bootstrap capacitor (C B ) to supply
Calculate a starting r DS(ON) as follows, in this example using
R DS ( ON ) =
( I )
sufficient gate drive for the high-side MOSFET driver. D B
should be a 20mA, 30V Schottky diode or equivalent device
and C B should be a 1μF ceramic type rated for at least 6.3V.
QL SELECTION
The bottom MOSFET should be selected primarily based on
5%
P QH = 0 . 05 × V OUT × I OUT
P QH
2
toprms
(EQ. 20)
(EQ. 21)
the device’s r DS(ON) and secondarily based on its gate
charge. To choose QL, use Equations 14, 15 and 16, and
allow 2% to 5% of the output power to be dissipated in the
18
Select a MOSFET and calculate the resulting gate drive
current. Verify that the combined gate drive current from QL
and QH does not exceed 80mA.
FN6876.3
August 29, 2012
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