Untitled
Abstract: No abstract text available
Text: FINE MESH PMT SERIES for HIGH MAGNETIC FIELD ENVIRONMENTS PMT's for THE OPERATION in HIGH MAGNETIC FIELDS over 1 TESLA In recent years, the demand for photodetectors, that can be operated in strong magnetic fields has increased, especially in the field of high energy physics. Conventional PMT's electrons
|
Original
|
S-164
TPMH1110E01
|
PDF
|
LL1671
Abstract: line output transformer se 130 n high end amplifier schematics high frequency transformer push pull SMALL high frequency transformer a887 LUNDAHL tesla TRANSFORMER 9- 0-9
Text: LUNDAHL TRANSFORMERS Tibeliusgatan 7 S-761 50 NORRTÄLJE SWEDEN International +46 - 176 13930 +46 - 176 13935 Phone Fax Domestic 0176-13930 0176-13935 High Current Tube Amplifier Interstage / Line Output Transformer LL1671 LL1671 is a high current interstage / line output transformer for tube amplifiers. The transformer is available
|
Original
|
S-761
LL1671
LL1671
LL1671PP
line output transformer
se 130 n
high end amplifier schematics
high frequency transformer push pull
SMALL high frequency transformer
a887
LUNDAHL
tesla
TRANSFORMER 9- 0-9
|
PDF
|
LL1660
Abstract: LL1660PP LUNDAHL line output transformer Ll1660 transformer TRANSFORMER 9- 0-9 220 in Line transformer 290H Tesla high frequency transformer push pull
Text: LUNDAHL TRANSFORMERS Tibeliusgatan 7 S-761 50 NORRTÄLJE SWEDEN Phone Fax International +46 - 176 13930 +46 - 176 13935 Domestic 0176-13930 0176-13935 Tube Amplifier Interstage Transformer / Line Output Transformer LL1660 LL1660 is an interstage / line output transformer for tube amplifiers. The transformer is available with different
|
Original
|
S-761
LL1660
LL1660
LL1660PP
LL1660,
R030211
LUNDAHL
line output transformer
Ll1660 transformer
TRANSFORMER 9- 0-9
220 in Line transformer
290H
Tesla
high frequency transformer push pull
|
PDF
|
LL1689
Abstract: LUNDAHL line output transformer LL1689PP audio output transformer high current transformer audio output transformers audio output transformers inter-stage ALT EPM7064LC68-15
Text: LUNDAHL TRANSFORMERS Tibeliusgatan 7 S-761 50 NORRTÄLJE SWEDEN Phone Fax International +46 - 176 13930 +46 - 176 13935 Domestic 0176-13930 0176-13935 Line Output Transformer LL1689 LL1689 is a line output transformer for tube amplifiers. The transformer is available with different core air gap
|
Original
|
S-761
LL1689
LL1689
LL1689PP
LL1689,
LUNDAHL
line output transformer
audio output transformer
high current transformer
audio output transformers
audio output transformers inter-stage
ALT EPM7064LC68-15
|
PDF
|
LL1671
Abstract: 220 in Line transformer LUNDAHL LL1692A LL1660 R080124 LUNDAHL LL1692A TRANSFORMER 9- 0-9 LL166 125H
Text: Tibeliusgatan 7 S-761 50 NORRTÄLJE SWEDEN LUNDAHL TRANSFORMERS Phone Fax International +46 - 176 13930 +46 - 176 13935 Domestic 0176-13930 0176-13935 Tube Amplifier Interstage Transformer / Line Output Transformer LL1692A LL1692A is an interstage transformer for tube amplifiers, impedance-wise placed between LL1660 and LL1671.
|
Original
|
S-761
LL1692A
LL1692A
LL1660
LL1671.
R080124
LL1671
220 in Line transformer
LUNDAHL LL1692A
R080124
LUNDAHL
TRANSFORMER 9- 0-9
LL166
125H
|
PDF
|
variable resistor 104
Abstract: Q65412-L100
Text: Differential Magneto Resistor FP 412 L 100 Dimensions in mm Features Typical applications • • • • • • • • • • • Accurate intercenter spacing High operating temperature range High output voltage Signal amplitude independent of speed Compact construction
|
Original
|
Q65412-L100
R01-2
R02-3
variable resistor 104
Q65412-L100
|
PDF
|
TESLA 1
Abstract: 104Gauss
Text: Differential Magneto Resistor FP 412 D 250 Dimensions in mm Features Typical applications • • • • • • • • • • • Accurate intercenter spacing High operating temperature range High output voltage Signal amplitude independent of speed Compact construction
|
Original
|
Q65412-D
R01-3,
R04-6
R01-2
R02-3
TESLA 1
104Gauss
|
PDF
|
Q65420-L90
Abstract: Q65420-L0090E001 r046 q65420l90 magneto R023
Text: Double Differential Magneto Resistor FP 420 L 90 Dimensions in mm Features Typical applications • • • • • • • • • • • Double differential magneto resistor on one carrier Accurate intercenter spacing High operating temperature range High output voltage
|
Original
|
Q65420-L90
Q65420-L0090E001
R01-2
R02-3
R04-5
R05-6
R01-3,
Q65420-L90
Q65420-L0090E001
r046
q65420l90
magneto
R023
|
PDF
|
Q65110-L80F
Abstract: Q65410-L80E TESLA 1
Text: Double Differential Magneto Resistor FP 410 L 4 x 80 FM Version 2.0 Dimensions in mm Features Typical Applications • Double differential magneto resistor on same carrier • Accurate intercenter spacing • High operating temperature range • High output voltage
|
Original
|
Q65410-L80E
Q65110-L80F
R01-2
R02-3
R04-5
R05-6
R01-3,
Q65110-L80F
Q65410-L80E
TESLA 1
|
PDF
|
magneto resistor
Abstract: Q65425-L90 R01-3 Q65425-L0090E001 magneto
Text: Differential Magneto Resistor FP 425 L 90 Dimensions in mm Features Typical applications • • • • • • • • • • • Double differential magneto resistor on one carrier Accurate intercenter spacing High operating temperature range High output voltage
|
Original
|
Q65425-L90
Q65425-L0090E001
R01-2
R02-3
R04-5
R05-6
R01-3,
magneto resistor
Q65425-L90
R01-3
Q65425-L0090E001
magneto
|
PDF
|
Q65110-L80F
Abstract: Q65410-L80E
Text: Double Differential Magneto Resistor FP 410 L 4 x 80 FM Dimensions in mm Features Typical applications • Double differential magneto resistor on same carrier • Accurate intercenter spacing • High operating temperature range • High output voltage
|
Original
|
Q65410-L80E
Q65110-L80F
R01-2
R02-3
R04-5
R05-6
R01-3,
Q65110-L80F
Q65410-L80E
|
PDF
|
FP17L200E
Abstract: SFP17 magneto resistor 200E L200 2.00E 02 Q65017-L200-E
Text: F P 1 7 L 200E Magneto resistor F P 1 7 L 2 0 0 E is a magneto resistor made of indium antimonide — nickel antimonide w ith a basic resistance R0 of 200 fl. The " L " material has a smaller temperature coefficient TC and a lower relative resistance variation /?B//?0 in the magnetic field
|
OCR Scan
|
FP17L
FP17L200E
Q65017-L200-E
SFP17
magneto resistor
200E
L200
2.00E 02
Q65017-L200-E
|
PDF
|
FP17D500E
Abstract: 500E D500E 104Gauss magneto resistor
Text: FP17D 500E Magneto resistor F P 1 7 D 5 0 0 E is a magneto resistor made of indium antimonide — nickel antimonide w ith a basic resistance R0 of 500 i l The " D " material produces the largest resistance change R B/R0 in the magnetic field. The temperature coefficient TC, however, is
|
OCR Scan
|
FP17D500E
Q65017-D
500-E
FP17D500E
500E
D500E
104Gauss
magneto resistor
|
PDF
|
FP30L100J
Abstract: magneto resistor Tesla Resistor
Text: FP30L100J Magneto resistor F P 3 0 L 1 0 0 J is a magneto resistor made of indium antimonide — nickel antimonide w ith a basic resistance R0 of 100 £2. The " L " material has a smaller temperature coefficient TC and a lower relative resistance variation R B/R 0 in the magnetic field
|
OCR Scan
|
FP30L100J
FP30L100J
Q65030-L100-J
magneto resistor
Tesla Resistor
|
PDF
|
|
|
FP30N60E
Abstract: FTP100 Q6503 30N60 ftp-100 30 N 60
Text: FP 30 N 60 E Magneto resistor F P 3 0 N 6 0 E is a m agneto resistor made of indium antimonide — nickel antimonide with a basic resistance R 0 of 6 0 fi. In case of " N " material the temperature coefficient TC and the relative resistance variation R B/R 0 in the magnetic field are
|
OCR Scan
|
FP30N60E
Q65030-N
30-z--â
FP30N60F
0TIF70
ftp-100
FTP100
Q6503
30N60
30 N 60
|
PDF
|
magneto resistor
Abstract: FP30L50E 30L50 Q65030-L50-E
Text: FP 30 L 50 E Magneto resistor F P 3 0 L 5 0 E is a magneto resistor made of indium antimonide — nickel antimonide with a basic resistance R 0 of 50 0 . The " L " material has a smaller temperature coefficient TC and a lower relative resistance variation R B/R0 in the magnetic field
|
OCR Scan
|
FP30L50E
Q65030-L50-E
FP30L50E
magneto resistor
30L50
Q65030-L50-E
|
PDF
|
G005
Abstract: FP17L200J magneto resistor
Text: F P 1 7 L 200J M agne to resistor F P 1 7 L 2 0 0 J is a magneto resistor made of indium antimonide — nickel antimonide with a basic resistance R 0 of 200 fi. The " L " material has a smaller temperature coefficient TC and a lower relative resistance variation R B/ R 0 in the magnetic field
|
OCR Scan
|
FP17L
FP17L200J
Q65017-L200-J
FP17L200J
G005
magneto resistor
|
PDF
|
FP30D50E
Abstract: magneto resistor 65030-D
Text: FP 30 D 50 E M agneto resistor F P 3 0 D 5 0 E is a magneto resistor made of indium antimonide — nickel antimonide with a basic resistance R 0 of 50 Q. The " D " material produces the largest resistance variation R B/R0 in the magnetic field. The temperature coefficient TC, however, is
|
OCR Scan
|
FP30D50E
65030-D
magneto resistor
|
PDF
|
magneto resistor
Abstract: Q6503 FP38L40E
Text: FP 38 L 40 E F P 3 8 L 4 0 E is a magneto resistor made of indium antimonide — nickel antimonide with a basic resistance R 0 of 40 Q. The " L " material has a smaller temperature coefficient TC and a lower relative resistance variation R B/ R 0 in the magnetic field
|
OCR Scan
|
FP38L40E
Q65038-L40-E
FP38L40F
magneto resistor
Q6503
|
PDF
|
magneto resistor
Abstract: tesla FP30L100E Q65030-L100-E tesla resistor L100 TC25 magneto Q6503 tc-2b
Text: FP 30 L 100 E Magneto resistor FP30L100E is a m agneto resistor made of indium antimonide — nickel antimonide with a basic resistance R 0 of 1 0 0 Q . The " L " material has a smaller temperature coefficient TC and a lower relative resistance variation R B/R0 in the magnetic field
|
OCR Scan
|
FP30L100E
Q65030-L100-E
FP30L100E
magneto resistor
tesla
Q65030-L100-E
tesla resistor
L100
TC25
magneto
Q6503
tc-2b
|
PDF
|
we381
Abstract: magneto resistor
Text: Infineon technologies FP 410 L 4 X 80 FM Double Differential Magneto Resistor Dimensions in mm Features Typical Applications • Double differential magneto resistor on same carrier • Accurate intercenter spacing • High operating temperature range • High output voltage
|
OCR Scan
|
Q65410-L80E
Q65110-L80F
flE35b05
013437b
we381
magneto resistor
|
PDF
|
Q65111-L100-D
Abstract: FP111L100 L100
Text: FR 111 L100 Center-tap magneto resistor The center-tap magneto resistor FP 111 L 100 is a magnetically controllable resistor made of InSb/NiSb and having a basic resistance R0 of 2 x 100Q. It is mounted on an insulated iron substrate. The " L " material is characterized by a large resistance
|
OCR Scan
|
FP111
Q65111-L100-D
FP111L100
Q65111-L100-D
FP111L100
L100
|
PDF
|
FP110L60
Abstract: TESLA 1 tesla potentiometer D155 FP110 FP110D155 Q65110-D155-D Q65110-L60-D
Text: F P 110D 155 FP110L60 Center-tap magneto resistors The center-tap magneto resistors F P 1 1 0 D 1 5 5 and F P 1 1 0 L 6 0 are magnetically controllable resistors made of InSb/NiSb and having an intrinsic resistance R 0 of 2 x 1 5 5 f i and 2 x 6 0 f2 , respectively. They are mounted on an insulated iron sub
|
OCR Scan
|
FP110D155
FP110L60
FP110L60
FP110
Q65110-D155-D
Q65110-L60-D
TESLA 1
tesla potentiometer
D155
Q65110-D155-D
Q65110-L60-D
|
PDF
|
Untitled
Abstract: No abstract text available
Text: SIEMENS Double Differential Magneto Resistor FP 420 L 90 1.6 pin connection 2 6 fingers on both sides free of lacquer 3) Center-distance between the Diff.-Systems. Approx, weight 0.2 g GPX06896 Dimensions in mm Features Typical applications • • •
|
OCR Scan
|
GPX06896
|
PDF
|
