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ACPL-K43T-000E Datasheet(PDF) 10 Page - AVAGO TECHNOLOGIES LIMITED

Part # ACPL-K43T-000E
Description  Automotive R2CouplerTM Wide Operating Temperature
Download  11 Pages
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Manufacturer  AVAGO [AVAGO TECHNOLOGIES LIMITED]
Direct Link  http://www.avagotech.com
Logo AVAGO - AVAGO TECHNOLOGIES LIMITED

ACPL-K43T-000E Datasheet(HTML) 10 Page - AVAGO TECHNOLOGIES LIMITED

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10
1
2
3
4
8
7
6
5
Die1:
LED
Die2:
Detector
Figure 15. Diagram of ACPL-K43T for measurement
Thermal Resistance Model for ACPL-K43T
The diagram of ACPL-K43T for measurement is shown in Figure 15. Here, one die is heated first and the temperatures of
all the dice are recorded after thermal equilibrium is reached. Then, the 2nd die is heated and all the dice temperatures
are recorded. With the known ambient temperature, the die junction temperature and power dissipation, the thermal
resistance can be calculated. The thermal resistance calculation can be cast in matrix form. This yields a 2 by 2 matrix for
our case of two heat sources.
R11
R12
X
P1
=
T1
R21
R22
P2
T2
R11 : Thermal Resistance of Die1 due to heating of Die1 (˚C/W)
R12 : Thermal Resistance of Die1 due to heating of Die2 (˚C/W)
R21 : Thermal Resistance of Die2 due to heating of Die1 (˚C/W)
R22 : Thermal Resistance of Die2 due to heating of Die2 (˚C/W)
P1 : Power dissipation of Die1 (W)
P2 : Power dissipation of Die2 (W)
T1 : Junction temperature of Die1 due to heat from all dice (˚C)
T2 : Junction temperature of Die2 due to heat from all dice (˚C)
Ta : Ambient temperature (˚C)
T1 : Temperature difference between Die1 junction and ambient (˚C)
T2 : Temperature deference between Die2 junction and ambient (˚C)
T1 = (R11 x P1 + R12 x P2) + Ta
T2 = (R21 x P1 + R22 x P2) + Ta
Measurement data on a low K board:
R11 = 160 °C/W, R12= R21 = 74 °C/W, R22 = 115 °C/W
Figure 16. Diagram of ACPL-K44T for measurement
Thermal Resistance Model for ACPL-K44T
The diagram of ACPL-K44T for measurement is shown in Figure 16. Here, one die is heated first and the temperatures of
all the dice are recorded after thermal equilibrium is reached. Then, the 2nd ,3rd and 4th die is heated and all the dice
temperatures are recorded. With the known ambient temperature, the die junction temperature and power dissipation,
the thermal resistance can be calculated. The thermal resistance calculation can be cast in matrix form. This yields a 4 by
4 matrix for our case of two heat sources.
R11
R12
R13
R14
X
P1
=
T1
R21
R22
R23
R24
P2
T2
R31
R32
R33
R34
P3
T3
R41
R42
R43
R44
P4
T4
R11 : Thermal Resistance of Die1 due to heating of Die1 (˚C/W)
R12 : Thermal Resistance of Die1 due to heating of Die2 (˚C/W)
R13 : Thermal Resistance of Die1 due to heating of Die3 (˚C/W)
R14 : Thermal Resistance of Die1 due to heating of Die4 (˚C/W)
R21 : Thermal Resistance of Die2 due to heating of Die1 (˚C/W)
R22 : Thermal Resistance of Die2 due to heating of Die2 (˚C/W)
R23 : Thermal Resistance of Die2 due to heating of Die3 (˚C/W)
R24 : Thermal Resistance of Die2 due to heating of Die4 (˚C/W)
1
2
3
4
8
7
6
5
Die1:
LED 1
Die2:
Detector 1
Die3:
LED 1
Die4:
Detector 2


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