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MAX1711EEG 参数 Datasheet PDF下载

MAX1711EEG图片预览
型号: MAX1711EEG
PDF下载: 下载PDF文件 查看货源
内容描述: 高速,数字可调,降压型控制器,用于笔记本电脑 [High-Speed, Digitally Adjusted Step-Down Controllers for Notebook CPUs]
分类和应用: 稳压器开关式稳压器或控制器电源电路开关式控制器光电二极管电脑输入元件
文件页数/大小: 28 页 / 299 K
品牌: MAXIM [ MAXIM INTEGRATED PRODUCTS ]
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Hig h -S p e e d , Dig it a lly Ad ju s t e d  
S t e p -Do w n Co n t ro lle rs fo r No t e b o o k CP Us  
0/MAX71  
tor. In some cases, there may be no room for electrolyt-  
V
BATT  
ics, creating a need for a DC-DC design that uses noth-  
ing but ceramics.  
DH  
The all-ceramic-capacitor application of Figure 7 has the  
same basic performance as the 7A Standard Application  
Circuit, but replaces the tantalum output capacitors with  
ceramics. This design relies on having a minimum of  
5mparasitic PC board trace resistance in series with  
the capacitor in order to reduce the ESR zero frequency.  
This small amount of resistance is easily obtained by  
locating the MAX1710/MAX1711 circuit two or three inch-  
es away from the CPU, and placing all the ceramic  
capacitors close to the CPU. Resistance values higher  
tha n 5mjus t imp rove the s ta b ility (whic h c a n b e  
observed by examining the load-transient response  
c ha ra c te ris tic a s s hown in the Typ ic a l Op e ra ting  
Characteristics). Avoid adding excess PC board trace  
resistance, as theres an efficiency penalty. 5mis suffi-  
cient for the 7A circuit.  
V
OUT  
MAX1710  
DL  
R1  
R2  
FB  
FBS  
1k  
GNDS  
Figure 8. Setting V  
with a Resistor-Divider  
OUT  
Outp ut ove rs hoot d e te rmine s the minimum outp ut  
capacitance requirement. In this example, the switching  
frequency has been increased to 550kHz and the induc-  
tor value has been reduced to 0.5µH (compared to  
300kHz and 2µH for the standard 7A circuit) in order to  
minimize the energy transferred from inductor to capaci-  
tor during load-step recovery. Even so, the amount of  
overshoot is high enough (80mV) that for the MAX1710,  
it’s wise to disable OVP or use the MAX1711 with its fixed  
2.25V overvoltage protection threshold to avoid tripping  
the fault latch (see the overshoot equation in the Output  
Capacitor Selection section). The efficiency penalty for  
operating at 550kHz is about 2% to 3%, depending on  
the input voltage.  
propagation delays introduce an error to the TON K-fac-  
tor. This error is higher at higher frequencies (Table 5).  
Also, keep in mind that transient response performance  
of buck regulators operated close to dropout is poor,  
and bulk output capacitance must often be added (see  
V
SAG  
equation in the Design Procedure).  
Dropout Design Example: V  
= 3V min, V  
=
OUT  
BATT  
2V, f = 300kHz. The required duty is (V  
+ V ) /  
OUT  
SW  
(V  
BATT  
- V ) = (2V + 0.1V) / (3.0V - 0.1V) = 72.4%. The  
SW  
worst-case on-time is (V  
+ 0.075) / V  
· K =  
OUT  
BATT  
2.075V / 3V · 3.35µs-V · 90% = 2.08µs. The IC duty-fac-  
tor limitation is:  
t
ON(MIN)  
Two optional 1kresistors are placed in series with FB  
and FBS. These resistors prevent the negative output  
volta g e s p ike (tha t re s ults from trip p ing OVP) from  
pulling SHDN low via its internal ESD diode, which tends  
to clear the fault latch, causing hiccup” restarts.  
DUTY =  
= 2.08µs + 500ns = 80.6%  
t
+ t  
ON(MIN) OFF(MAX)  
which meets the required duty.  
Remember to include inductor resistance and MOSFET  
S e t t in g V  
w it h a Re s is t o r-Divid e r  
OUT  
on-state voltage drops (V ) when doing worst-case  
SW  
The output voltage can be adjusted with a resistor-  
divider rather than the DAC if desired (Figure 8). The  
drawback of this practice is that the on-time doesnt  
automatically receive correct compensation for changing  
output voltage levels. This can result in variable switch-  
ing frequency as the resistor ratio is changed and/or  
excessive switching frequency. The equation for adjust-  
ing the output voltage is:  
dropout duty-factor calculations.  
All-Ce ra m ic -Ca p a c it o r Ap p lic a t io n  
Ceramic capacitors have advantages and disadvan-  
tages. They have ultra-low ESR, are non-combustible,  
are relatively small, and are nonpolarized. On the other  
hand, theyre expensive and brittle, and their ultra-low  
ESR characteristic can result in excessively high ESR  
zero frequencies (affecting stability). In addition, they  
can cause output overshoot when going abruptly from  
full-load to no-load conditions, unless there are some  
bulk tantalum or electrolytic capacitors in parallel to  
absorb the stored energy in the induc-  
R1  
V
= V 1% 1+  
FB  
(
)
OUT  
R2  
______________________________________________________________________________________ 21  
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