数据搜索系统,热门电子元器件搜索
  Chinese  ▼
ALLDATASHEETCN.COM

X  

LTC3603 数据表(PDF) 12 Page - Linear Technology

部件名 LTC3603
功能描述  17V, 1A Synchronous Step-Down Regulator with 3.5關A Quiescent Current
PDF  16 Pages
Scroll/Zoom Zoom In 100%  Zoom Out
制造商  LINER [Linear Technology]
网页  http://www.linear.com
标志 LINER - Linear Technology

LTC3603 数据表(HTML) 12 Page - Linear Technology

Back Button LTC3603 Datasheet HTML 8Page - Linear Technology LTC3603 Datasheet HTML 9Page - Linear Technology LTC3603 Datasheet HTML 10Page - Linear Technology LTC3603 Datasheet HTML 11Page - Linear Technology LTC3603 Datasheet HTML 12Page - Linear Technology LTC3603 Datasheet HTML 13Page - Linear Technology LTC3603 Datasheet HTML 14Page - Linear Technology LTC3603 Datasheet HTML 15Page - Linear Technology LTC3603 Datasheet HTML 16Page - Linear Technology  
Zoom Inzoom in Zoom Outzoom out
 12 / 16 page
background image
LTC3621/LTC3621-2
12
3621f
For more information www.linear.com/LTC3621
applicaTions inForMaTion
2. The switching current is the sum of the MOSFET driver
and control currents. The power MOSFET driver current
resultsfromswitchingthegatecapacitanceofthepower
MOSFETs. Each time a power MOSFET gate is switched
from low to high to low again, a packet of charge dQ
moves from IN to ground. The resulting dQ/dt is a cur-
rent out of IN that is typically much larger than the DC
control bias current. In continuous mode, IGATECHG =
f(QT + QB), where QT and QB are the gate charges of
the internal top and bottom power MOSFETs and f is
the switching frequency. The power loss is thus:
Switching Loss = IGATECHG • VIN
The gate charge loss is proportional to VIN and f and
thus their effects will be more pronounced at higher
supply voltages and higher frequencies.
3. Other “hidden” losses such as transition loss and cop-
per trace and internal load resistances can account for
additional efficiency degradations in the overall power
system. It is very important to include these “system”
level losses in the design of a system. Transition loss
arises from the brief amount of time the top power
MOSFET spends in the saturated region during switch
node transitions. The LTC3621 internal power devices
switch quickly enough that these losses are not sig-
nificant compared to other sources. These losses plus
other losses, including diode conduction losses during
dead-time and inductor core losses, generally account
for less than 2% total additional loss.
Thermal Conditions
In a majority of applications, the LTC3621 does not dis-
sipate much heat due to its high efficiency and low thermal
resistance of its exposed pad package. However, in ap-
plications where the LTC3621 is running at high ambient
temperature, high VIN, high switching frequency, and
maximum output current load, the heat dissipated may
exceed the maximum junction temperature of the part. If
the junction temperature reaches approximately 160°C,
bothpowerswitcheswillbeturnedoffuntilthetemperature
drops about 15°C cooler.
To avoid the LTC3621 from exceeding the maximum junc-
tion temperature, the user will need to do some thermal
analysis. The goal of the thermal analysis is to determine
whether the power dissipated exceeds the maximum
junction temperature of the part. The temperature rise is
given by:
TRISE = PD • θJA
As an example, consider the case when the LTC3621
is used in applications where VIN = 12V, IOUT = 1A,
f = 2.25MHz, VOUT = 1.8V. The equivalent power MOSFET
resistance RSW is:
RSW =RDS(ON)TOP
VOUT
VIN
+RDS(ON)BOT • 1–
VOUT
VIN
=370mΩ•
1.8V
12V
+150mΩ • 1–
1.8V
12V
=183m
The VIN current during 2.25MHz force continuous opera-
tion with no load is about 5mA, which includes switching
and internal biasing current loss, transition loss, inductor
core loss and other losses in the application. Therefore,
the total power dissipated by the part is:
PD = IOUT2 • RSW + VIN • IIN(Q)
= 1A2 • 183mΩ + 12V • 5mA
= 243mW
TheDFN2mm
×3mmpackagejunction-to-ambientthermal
resistance,
θJA, is around 64°C/W. Therefore, the junction
temperature of the regulator operating in a 25°C ambient
temperature is approximately:
TJ = 0.243W • 64°C/W + 25°C = 40.6°C
Remembering that the above junction temperature is
obtained from an RDS(ON) at 25°C, we might recalculate
the junction temperature based on a higher RDS(ON) since
it increases with temperature. Redoing the calculation
assuming that RSW increased 5% at 40.6°C yields a new



Html Pages

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16


数据表 下载

Go To PDF Page


链接网址



ALLDATASHEET是否为您带来帮助?  [ DONATE ] 

关于 Alldatasheet   |   广告服务   |   联系我们   |   隐私政策   |   数据表链接    |   链接交换   |   制造商名单
All Rights Reserved©Alldatasheet.com


Mirror Sites
English : Alldatasheet.com  |   English : Alldatasheet.net  |   Chinese : Alldatasheetcn.com  |   German : Alldatasheetde.com  |   Japanese : Alldatasheet.jp
Russian : Alldatasheetru.com  |   Korean : Alldatasheet.co.kr  |   Spanish : Alldatasheet.es  |   French : Alldatasheet.fr  |   Italian : Alldatasheetit.com
Portuguese : Alldatasheetpt.com  |   Polish : Alldatasheet.pl  |   Vietnamese : Alldatasheet.vn
Indian : Alldatasheet.in  |   Mexican : Alldatasheet.com.mx  |   British : Alldatasheet.co.uk  |   New Zealand : Alldatasheet.co.nz
Family Site : ic2ic.com  |   icmetro.com