欢迎访问ic37.com |
会员登录 免费注册
发布采购

LM2937IMP-3.3 参数 Datasheet PDF下载

LM2937IMP-3.3图片预览
型号: LM2937IMP-3.3
PDF下载: 下载PDF文件 查看货源
内容描述: 400毫安提供最大500mA电流稳压器 [400mA and 500mA Voltage Regulators]
分类和应用: 稳压器
文件页数/大小: 10 页 / 297 K
品牌: NSC [ National Semiconductor ]
 浏览型号LM2937IMP-3.3的Datasheet PDF文件第2页浏览型号LM2937IMP-3.3的Datasheet PDF文件第3页浏览型号LM2937IMP-3.3的Datasheet PDF文件第4页浏览型号LM2937IMP-3.3的Datasheet PDF文件第5页浏览型号LM2937IMP-3.3的Datasheet PDF文件第7页浏览型号LM2937IMP-3.3的Datasheet PDF文件第8页浏览型号LM2937IMP-3.3的Datasheet PDF文件第9页浏览型号LM2937IMP-3.3的Datasheet PDF文件第10页  
Application Hints  
The figure below shows the voltages and currents which are  
present in the circuit, as well as the formula for calculating  
the power dissipated in the regulator:  
EXTERNAL CAPACITORS  
The output capacitor is critical to maintaining regulator stabil-  
ity, and must meet the required conditions for both ESR  
(Equivalent Series Resistance) and minimum amount of ca-  
pacitance.  
MINIMUM CAPACITANCE:  
The minimum output capacitance required to maintain stabil-  
ity is 10 µF (this value may be increased without limit).  
Larger values of output capacitance will give improved tran-  
sient response.  
ESR LIMITS:  
DS100113-19  
The ESR of the output capacitor will cause loop instability if  
it is too high or too low. The acceptable range of ESR plotted  
versus load current is shown in the graph below. It is essen-  
tial that the output capacitor meet these requirements,  
or oscillations can result.  
=
=
÷
I
G
(V − V  
IN OUT  
I
P
I
IN  
L
) I + (V ) I  
IN G  
D
L
FIGURE 2. Power Dissipation Diagram  
The next parameter which must be calculated is the maxi-  
mum allowable temperature rise, TR (max). This is calcu-  
lated by using the formula:  
Output Capacitor ESR  
=
TR (max) TJ(max) − TA (max)  
where: TJ (max) is the maximum allowable junction tem-  
perature, which is 125˚C for commercial  
grade parts.  
TA (max) is the maximum ambient temperature  
which will be encountered in the applica-  
tion.  
Using the calculated values for TR(max) and PD, the maxi-  
mum allowable value for the junction-to-ambient thermal re-  
sistance, θ(J−A), can now be found:  
=
θ(J−A) TR (max)/PD  
DS100113-17  
IMPORTANT: If the maximum allowable value for θ(J−A) is  
found to be 53˚C/W for the TO-220 package, 80˚C/W for  
the TO-263 package, or 174˚C/W for the SOT-223 pack-  
age, no heatsink is needed since the package alone will dis-  
sipate enough heat to satisfy these requirements.  
FIGURE 1. ESR Limits  
It is important to note that for most capacitors, ESR is speci-  
fied only at room temperature. However, the designer must  
ensure that the ESR will stay inside the limits shown over the  
entire operating temperature range for the design.  
If the calculated value for θ(J−A)falls below these limits, a  
heatsink is required.  
For aluminum electrolytic capacitors, ESR will increase by  
about 30X as the temperature is reduced from 25˚C to  
−40˚C. This type of capacitor is not well-suited for low tem-  
perature operation.  
HEATSINKING TO-220 PACKAGE PARTS  
The TO-220 can be attached to a typical heatsink, or se-  
cured to a copper plane on a PC board. If a copper plane is  
to be used, the values of θ(J−A) will be the same as shown in  
the next section for the TO-263.  
Solid tantalum capacitors have a more stable ESR over tem-  
perature, but are more expensive than aluminum electrolyt-  
ics. A cost-effective approach sometimes used is to parallel  
an aluminum electrolytic with a solid Tantalum, with the total  
capacitance split about 75/25% with the Aluminum being the  
larger value.  
If a manufactured heatsink is to be selected, the value of  
heatsink-to-ambient thermal resistance, θ(H−A), must first be  
calculated:  
=
θ(H−A) θ(J−A) θ(C−H) θ(J−C)  
If two capacitors are paralleled, the effective ESR is the par-  
allel of the two individual values. The “flatter” ESR of the Tan-  
talum will keep the effective ESR from rising as quickly at low  
temperatures.  
Where: θ(J−C) is defined as the thermal resistance from  
the junction to the surface of the case. A  
value of 3˚C/W can be assumed for θ(J−C)  
for this calculation.  
HEATSINKING  
θ(C−H)  
is defined as the thermal resistance be-  
tween the case and the surface of the heat-  
sink. The value of θ(C−H) will vary from  
about 1.5˚C/W to about 2.5˚C/W (depend-  
ing on method of attachment, insulator,  
etc.). If the exact value is unknown, 2˚C/W  
A heatsink may be required depending on the maximum  
power dissipation and maximum ambient temperature of the  
application. Under all possible operating conditions, the junc-  
tion temperature must be within the range specified under  
Absolute Maximum Ratings.  
should be assumed for θ(C−H)  
.
To determine if a heatsink is required, the power dissipated  
by the regulator, PD, must be calculated.  
When a value for θ(H−A) is found using the equation shown,  
a heatsink must be selected that has a value that is less than  
or equal to this number.  
www.national.com  
6