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Document Number: 28335

240

Revision: 09-May-08

119 AHT-DIN

Vishay BCcomponents

Aluminum Capacitors

Axial High Temperature, DIN-Based

EQUIVALENT SERIES RESISTANCE (ESR)

IMPEDANCE (Z)

Fig.7 Typical multiplier of ESR as a function of

ambient temperature

0150

50

100

1

10

- 50

- 100

ESR

0

ESR

10

2

10

-1

1

2

1

2

Case Ø D x L = 6.5 x 18 to 15 x 30 mm

ESR

Curve 1: 25 to 200 V

Curve 2: 10 V; 16 V

Fig.8 Typical multiplier of ESR as a function of

ambient temperature

0150

50

100

1

10

- 50

- 100

ESR

0

ESR

10

2

10

-1

Case Ø D x L = 18 x 30 to 21 x 38 mm

ESR

1

2

1

2

Curve 1: 25 to 100 V

Curve 2: 10 V; 16 V

Fig.9 Typical multiplier of ESR as a function

of frequency

ESR

0

ESR

Case Ø D x L = 6.5 x 18 to 10 x 25 mm

ESR

0

10

5

10

4

10

3

10

2

10

f (Hz)

0.4

0.8

1.2

1.6

2.0

4

3

2

1

1

2

4

3

Curve 1: 63 V (< 10 µF) and 200 V

Curve 2: 63 V (< 10 µF) and 100 V

Curve 3: 25 V; 40 V

Curve 4: 10 V; 16 V

Fig.10 Typical multiplier of ESR as a function

of frequency

Case Ø D x L = 10 x 30 to 21 x 38 mm

ESR

10

5

10

4

10

3

10

2

10

f (Hz)

0

0.2

0.4

0.6

0.8

1.4

ESR

1.2

1.0

1

2

3

2

1

3

Curve 1: 10 V

Curve 2: 16 V; 25 V

Curve 3: 40 V to100 V

Fig.11 Typical impedance as a function of frequency

f (Hz)

10

6

10

5

10

4

10

3

10

2

10

10

7

10

10

10

1

Z

( )

Ω

1

2

3

10

-1

Case Ø D x L = 8 x 18 mm

Curve 1: 22 µF

Curve 2: 47 µF

Curve 3: 100 µF

T

Fig.12 Typical impedance as a function of frequency

f (Hz)

10

6

10

5

10

4

10

3

10

2

10

10

7

10

3

10

2

10

1

Z

( )

Ω

10

-1

Case Ø D x L = 8 x 18 mm

1

2

3

Curve 1: 100 µF

Curve 2: 220 µF

Curve 3:470 µF