LPS6235-564 [COILCRAFT]

General Purpose Inductor,;
LPS6235-564
型号: LPS6235-564
厂家: Coilcraft lnc.    Coilcraft lnc.
描述:

General Purpose Inductor,

文件: 总2页 (文件大小:163K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
•ꢀ LOGꢀisꢀtheꢀnaturalꢀLOGꢀ(basee)  
                                                                             
Document 267  
SPICE Model – LPS6235  
This lumped-element (SPICE) model data simulates  
The value of the frequency-dependent variable resistor  
RVAR1 is calculated from:  
the frequency-dependent behavior of Coilcraft power  
inductors within the frequency range shown in the ac-  
companying table for each individual inductor.  
RVAR1 = k1  
*
•ꢀ k1isshownꢀforꢀeachꢀvalueꢀinꢀtheꢀaccompanyingꢀtable.  
•ꢀ fꢀisꢀtheꢀfrequencyꢀinꢀHz  
The data represents de-embedded measurements, as  
described below.Effects due to different customer circuit  
board traces, board materials, ground planes or interac-  
tions with other components are not included and can  
have a significant effect when comparing the simulation  
to measurements of the inductors using other production  
verification instruments and fixtures.  
•ꢀ RVAR1 is the resistance in Ohms  
The value of the frequency-dependent variable resistor  
RVAR2 is calculated from:  
RVAR2 = k2  
*
•ꢀ k2isshownꢀforꢀeachꢀvalueꢀinꢀtheꢀaccompanyingꢀtable.ꢀ  
•ꢀ fꢀisꢀtheꢀfrequencyꢀinꢀHz  
Lumped Element Modeling Method  
Measurements were made using a 50 Ohm impedance  
analyzer.Fixturecompensationwasperformedtoremove  
fixture effects. No DC bias current was applied in any of  
the measurements. The lumped element values were  
determined by optimizing the simulation model to an  
average of the measurements. This method results in a  
model that represents as closely as possible the typical  
frequency-dependent behavior of the component within  
the model frequency range.  
•ꢀ RVAR2 is the resistance in Ohms  
Note: The log function in the following equation is the  
natural logarithm, base e, not base 10.  
The value of the frequency-dependent inductance LVAR  
is calculated from:  
LVAR = k3 k4 * LOG (k5 f)  
*
•ꢀ k3,ꢀk4,ꢀandꢀk5ꢀareꢀshownꢀinꢀtheꢀaccompanyingꢀtable.  
•ꢀ fꢀisꢀtheꢀfrequencyꢀinꢀHz  
Theequivalentlumpedelementmodelschematicisshown  
below. Each model should only be analyzed at the input  
and output ports. Individual elements of the model are  
not determined by parameter measurement. The ele-  
ments are determined by the overall performance of the  
lumped element model compared to the measurements  
taken of the component.  
•ꢀ LVARꢀisꢀtheꢀinductanceꢀinꢀµH  
Disclaimer  
Coilcraft makes every attempt to provide accurate mea-  
surement data and software, representative of our com-  
ponents, in a usable format.Coilcraft, however, disclaims  
all warrants relating to the use of its data and software,  
whether expressed or implied, including without limita-  
tion any implied warranties of merchantability or fitness  
for a particular purpose. Coilcraft cannot and will not be  
liable for any special, incidental, consequential, indirect  
or similar damages occurring with the use of the data  
and/or software.  
R
VAR2  
C
R1  
L
R2  
R
VAR1  
VAR  
Document 267-1 Revised 07/22/11  
Document 267  
SPICE Model for Coilcraft LPS6235 Power Inductors  
Frequency limit  
of model (MHz)  
LVAR Coefficients  
Part number Lower Upper  
R1()  
R2()  
C (pF)  
k1  
k2  
2.2  
2.56  
3.22 10  
3.74 12  
4.95 15  
5.76 18  
6.68 22  
7.74 33  
k3  
6.8  
8.2  
k4  
k5  
LPS6235-682  
LPS6235-822  
LPS6235-103  
LPS6235-123  
LPS6235-153  
LPS6235-183  
LPS6235-223  
LPS6235-333  
LPS6235-473  
LPS6235-563  
LPS6235-683  
LPS6235-823  
LPS6235-104  
LPS6235-124  
LPS6235-154  
LPS6235-224  
LPS6235-334  
LPS6235-474  
LPS6235-564  
LPS6235-684  
LPS6235-824  
LPS6235-105  
LPS6235-155  
LPS6235-185  
LPS6235-225  
LPS6235-335  
LPS6235-475  
LPS6235-565  
LPS6235-685  
LPS6235-825  
LPS6235-106  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
0.1  
60  
50  
40  
40  
30  
30  
30  
30  
30  
30  
30  
20  
20  
20  
10  
10  
200  
178  
115  
75  
50  
65  
45  
14  
13  
12  
14  
20  
20  
22  
18  
24  
100  
130  
70  
190  
160  
120  
180  
120  
70  
180  
30  
250  
50  
0.075  
0.095  
0.100  
0.110  
0.125  
0.140  
0.145  
0.180  
0.245  
0.280  
0.345  
0.315  
0.375  
0.435  
0.535  
0.72  
1.02  
1.58  
1.75  
1.97  
2.70  
3.20  
4.60  
5.42  
1.93  
2.53  
2.85  
3.24  
3.79  
3.06  
3.32  
3.61  
4.00  
3.92  
3.91  
3.13  
2.86  
3.21  
3.85  
3.64  
4.19  
5.05  
5.18  
4.67  
6.00  
5.20  
4.72  
5.41  
5.52  
6.67  
5.76  
6.82  
5.72  
6.62  
8.05  
9.00E-05  
1.80E-04  
1.00E-04  
1.80E-04  
3.00E-04  
2.20E-04  
2.60E-04  
2.80E-04  
1.40E-03  
1.00E-03  
4.00E-04  
4.00E-04  
7.50E-04  
9.00E-04  
1.90E-03  
1.20E-03  
6.00E-04  
4.00E-04  
1.60E-03  
2.00E-03  
2.60E-03  
3.80E-03  
4.20E-03  
6.90E-03  
9.50E-03  
1.10E-02  
0.06  
0.10  
0.11  
0.17  
0.19  
0.22  
0.24  
0.36  
0.68  
0.88  
0.92  
0.90  
0.92  
0.94  
1.2  
1.8  
2.5  
2.8  
3.2  
3.4  
4.7  
5.5  
7.7  
9.85E-06  
9.85E-06  
9.88E-06  
9.92E-06  
9.92E-06  
9.92E-06  
9.92E-06  
9.92E-06  
9.80E-06  
9.90E-06  
9.99E-06  
9.97E-06  
9.94E-06  
1.00E-05  
1.00E-05  
1.02E-05  
1.06E-05  
1.15E-05  
1.19E-05  
1.25E-05  
1.37E-05  
1.42E-05  
1.68E-05  
2.30E-05  
3.18E-05  
4.26E-05  
1.55E-04  
4.25E-04  
3.02E-04  
1.32E-03  
4.59E-03  
10.2  
47  
56  
68  
82  
12.4  
16.2  
17.0  
20.2 100  
26.6 120  
30.0 150  
41.0 220  
67.0 330  
96.0 470  
6.0  
5.0  
4.0  
3.0  
3.0  
3.0  
3.0  
3.0  
3.0  
2.0  
2.0  
1.0  
1.0  
1.0  
1.0  
102  
560  
680  
820  
131  
178  
215  
303  
380  
435  
640  
1000  
1500  
1800  
2200  
3300  
4700  
5600  
6800  
8200  
8.0  
8.8  
19.3  
18.0  
22.0  
30.0  
35.0  
50.0  
6.40  
8.90  
14.0  
16.4  
21.4  
24.0  
29.0  
1.10E-02 1200  
1.10E-02 1100  
1.20E-02 1500  
1.50E-02 1600  
60  
60  
1.40E-02 1700 10000  
Document 267-70 Revised 04/12/11  

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