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PTR100-1100-VM

产品描述General Purpose Inductor, 100uH, 15%, 1 Element, Iron-Core, RADIAL LEADED
产品类别无源元件    电感器   
文件大小229KB,共4页
制造商API Delevan
官网地址http://www.delevan.com/
标准  
下载文档 详细参数 全文预览

PTR100-1100-VM概述

General Purpose Inductor, 100uH, 15%, 1 Element, Iron-Core, RADIAL LEADED

PTR100-1100-VM规格参数

参数名称属性值
是否无铅不含铅
是否Rohs认证符合
厂商名称API Delevan
Reach Compliance Codecompliant
ECCN代码EAR99
型芯材料IRON
直流电阻0.05 Ω
标称电感 (L)100 µH
电感器应用POWER INDUCTOR
电感器类型GENERAL PURPOSE INDUCTOR
JESD-609代码e2
功能数量1
端子数量2
最大额定电流5.1 A
形状/尺寸说明CYLINDRICAL PACKAGE
屏蔽NO
表面贴装NO
端子面层Tin/Copper (Sn/Cu)
端子位置RADIAL
端子形状WIRE
测试频率0.001 MHz
容差15%

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Inductance
tested at 1 KHz, <10 gauss and 0 Adc
DC Resistance
at 25°C
Rated Idc
based on 40°C maximum rise from 25°C
ambient with 0 Arms
Windings
single layered to maximize operating
frequency and minimize board space
Self leads
solder coated to within .050" of seating plane
Other values
available on request
Packaging
Bulk only
Mounting
Standard mounting is self-lead radial per
Figure “1”. Optional mounting methods are self-leaded
horizontal per Figure “2” or vertical base mounted per
Figures “3” and “4”.
FIGURE
FIGURE
PA
RT
Power Toroids –
Horizontal or Vertical Mount
1
2
STANDARD
VERTICAL
FIGURE
FIGURE
HORIZONTAL
3
4
VERTICAL
2-LEAD
VERTICAL
4-LEAD
PT5-530
5
PT5-700
5
5
PT5-800
5
PT5-1000
10
PT10-530
10
PT10-680
10
PT10-820
10
PT10-990
25
PT25-680
25
PT25-800
25
PT25-900
25
PT25-1000
50
PT50-780
50
PT50-900
50
PT50-1020
50
PT50-1320
75
PT75-900
75
PT75-980
75
PT75-1260
75
PT75-1550
100
PT100-1000
100
PT100-1100
100
PT100-1260
100
PT100-1550
150
PT150-1040
150
PT150-1250
150
PT150-1500
150
PT150-2050
250
PT250-1200
250
PT250-1500
250
PT250-1800
300
PT300-1200
300
PT300-1500
300
PT300-1750
400
PT400-1200
400
PT400-1500
400
PT400-1750
500
PT500-1450
500
PT500-1750
500
PT500-2000
750
PT750-1400
750
PT750-1700
750
PT750-2050
PT1000-1400 1000
PT1000-1750 1000
PT1000-2050 1000
NU
MB
ER
PT Series
PT SERIES POWER TOROIDS
0.015
0.012
0.010
0.008
0.020
0.015
0.010
0.008
0.035
0.025
0.020
0.014
0.050
0.030
0.025
0.020
0.060
0.040
0.035
0.025
0.080
0.050
0.035
0.028
0.100
0.060
0.050
0.040
0.130
0.080
0.055
0.150
0.100
0.075
0.250
0.180
0.110
0.220
0.160
0.090
0.350
0.280
0.150
0.620
0.420
0.200
6.1
7.4
10.6
12.8
4.9
6.8
9.3
13.2
4.4
6.6
7.0
10.4
3.8
5.6
7.0
11.0
3.9
5.2
7.4
10.6
3.5
5.1
7.8
10.3
3.4
5.7
7.7
12.3
3.8
6.1
9.1
3.3
5.5
7.3
2.4
4.7
6.0
3.4
5.0
8.0
2.6
3.7
6.4
1.8
3.1
5.9
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
8
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8
8
IN
D.
H)
±
15
DC
%
R
@
MA
1K
X.
Hz
RA
(O
TE
HM
D
S)
Id
c(
FI
G
Am
VE . “1
ps
RT ” S
)
IC TA
FI
G. AL ND
AR
HO “2
D
RI ”
ZO
FI
G. NTA
VE “3 L
RT ” 2
I
FI CAL -LEA
G.
D
VE “4
RT 4
IC -L
AL EA
D
2/ 2002
MOUNTING AVAILABLE
POWER INDUCTORS
Notes to Figure 5 (Page 95)
The PT Toroid Series inductance is specified at AC and DC signal levels which have no significant effect
on the permeability of the powdered iron toroidal core. Superimposed AC and DC voltages will change the permeability and therefore
the inductance, under operating conditions. Typically, DC currents will reduce the inductance, while AC signals will increase the
inductance up to a point, before beginning to decrease. Supporting information is provided, detailing the AC or DC effects upon each
part. Saturation resulting from DC currents is specified with waveform having less than a 1% ripple content. When considering the AC
waveform, both the frequency and voltage level must be taken into account. As an aid in defining what effect the alternating sine wave
signal will have, the voltage/frequency factor curve can be used. To determine what change of inductance can be expected at a given
voltage level and frequency, simply divide the sinusoidal RMS voltage by the frequency. The voltage is in volts and the frequency is in
hertz. As an example, if using part number PT25-680 at a 1VRMS signal level, and a frequency of 25KHz, the voltage/frequency factor
is calculated to be: 1VRMS/25,000Hz = 40 x 10–6. Referring to the graph, a 39% increase in inductance would be expected.
Notes to Figure 6 (Page 95)
Typical saturation effects as a function of DC flowing through the part. Data is representative of a DC
waveform with less than 1% ripple, and an AC waveform less than 10 gauss.
Note
This information is intended to be used in assisting the designer in part selection. Each operating application may contain other
variables which must be considered in part selection; such as temperature effects, waveform distortion, etc.... Delevan Sales/Engin-
eering staff is available to provide information as needed to fit each application.
www
.
delevan
.
com
E-mail: apisales@delevan.com
270 Quaker Rd., East Aurora NY 14052 • Phone 716-652-3600 • Fax 716-652-4814
PAGE
92
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