ogy, for driving inductive or resistive loads. An internal Clamping Diode enables the fast demagnetizationof inductive loads.
Diagnostic for CPU feedback and extensive use
of electrical protections make this device inherently indistructible and suitable for general purpose industrial applications.
October 1995
1/12
Page 2
TDE1897C- TDE1898C
PIN CONNECTIONS (Top view)
SIP9
Minidip
SO20
ABSOLUTE MAXIMUM RATINGS (Minidippin reference)
SymbolParameterValueUnit
V
V
S–VO
V
V
I
E
P
T
T
S
I
i
O
tot
op
stg
Supply Voltage (Pins 3 - 1) (TW< 10ms)50V
Supply to OutputDifferential Voltage. SeealsoVCl3-2(Pins3 - 2)internally limitedV
Input Voltage (Pins 7/8)-10 to VS +10V
i
Differential Input Voltage (Pins 7 - 8)43V
i
Input Current (Pins 7/8)20mA
Output Current (Pins 2 - 1). See also ISCinternally limitedA
Energy from Inductive Load(TJ=85°C)200mJ
l
Power Dissipation. See alsoTHERMAL CHARACTERISTICS.internally limitedW
Operating Temperature Range (T
Turn on Delay Time100µs
Turn off Delay Time20µs
Input Switching to Diagnostic
100µs
Valid
Note Vil < 0.8V, Vih > 2V @ (V+In > V–In); Minidip pin reference.(*) Not tested.
Figure1
DIAGNOSTICTRUTH TABLE
Diagnostic ConditionsInputOutputDiag1Diag2
Normal OperationL
H
Open Load Condition (I
)L
o<Iold
H
Short to V
S
L
H
Short Circuit to Ground (I
) (**)TDE1897C
O=ISC
TDE1898C
H<H (*)HL
HH
Output DMOS OpenL
H
OvertemperatureL
H
SupplyUndervoltage (V
supplyvoltage;V
S<Vsth2
S<Vsth1
in the fallingphase of the
inthe rising phaseof the supply
L
H
voltage)
(*) According to the intervention of the current limiting block.
(**) A cold lampfilament,or a capacitive load may activatethe current limiting circuit of the IPS,when theIPS is initially turned on.TDE1897
uses Diag2 to signal such condition, TDE1898 does not.
4/12
L
H
L
H
H
H
H
H
H
L
L
L
H
L
L
L
L
L
L
L
H
H
L
H
H
L
L
H
H
H
H
H
H
H
H
H
H
L
L
L
L
Page 5
TDE1897C - TDE1898C
APPLICATION INFORMATION
DEMAGNETIZATIONOF INDUCTIVE LOADS
An internal zener diode, limiting the voltage
across the Power MOS to between 45 and 55V
(V
), provides safe and fast demagnetization of
cl
inductiveloads without external clamping devices.
The maximum energy that can be absorbed from
an inductive load is specified as 200mJ (at
=85°C).
T
j
To define the maximumswitching frequencythree
pointshave to be considered:
1) The total power dissipation is the sum of the
On State Power and of the Demagnetization
Energy multipliedby the frequency.
2) The total energy W dissipated in the device
during a demagnetizationcycle (figg. 2, 3) is:
W = V
L
Io–
V
cl–Vs
R
L
L
cl
R
log
1 +
Vcl–V
V
s
s
Where:
V
= clamp voltage;
cl
L =inductive load;
= resistiveload;
R
L
Vs =supply voltage;
I
O=ILOAD
3) In normal conditions the operating Junction
temperatureshould remain below 125°C.
Figure 3: DemagnetizationCycle Waveforms
Figure2: InductiveLoad Equivalent Circuit
Figure 4: Normalized R
Temperature
α
1.8
RDSON (Tj)
α=
1.6
1.4
1.2
1.0
0.8
0.6
-250255075100 125Tj (°C)
RDSON (Tj=25°C)
DSON
vs. Junction
D93IN018
5/12
Page 6
TDE1897C- TDE1898C
WORST CONDITION POWER DISSIPATION IN
THEON-STATE
In IPS applications the maximum average power
dissipation occurs when the device stays for a
long time in the ON state. In such a situation the
internal temperature depends on delivered current (and related power), thermal characteristics
of the packageand ambient temperature.
At ambient temperature close to upper limit
(+85°C)and in theworst operating conditions,it is
possible that the chip temperature could increase
so much to make the thermal shutdown procedureuntimely intervene.
Our aim is to find the maximum current the IPS
can withstand in the ON state without thermal
shutdown intervention, related to ambient temperature.To this end, we should consider the followingpoints:
1) The ON resistance R
DSON
of the output
NDMOS (the real switch) of the device increases with its temperature.
Experimentalresults show that silicon resistivity increases with temperature at a constant
rate, rising of 60% from 25°Cto 125°C.
The relationship between R
DSON
and tem-
peratureis therefore:
R
DSON
= R
DSON0
( 1 + k )
( Tj± 25 )
where:
T
is the silicon temperature in °C
j
R
k is the constant rate (k = 4.711 ⋅
DSON0
isR
DSON
at Tj=25°C
10
±3
)
(see fig.4).
the third element are constant, while the first
one increases with temperature because
R
increasesas well.
DSON
3) The chip temperature must not exceed ΘLim
in order do not lose the control of the device.
The heat dissipation path is represented by
the thermal resistance of the system deviceboard-ambient (R
). In steady state condi-
th
tions, this parameter relates the power dissipated P
the ambient temperatureT
T
j
to the silicon temperature Tjand
± T
on
amb
= Pon⋅ R
th
amb
:
(2)
From this relationship, the maximum power
P
which can be dissipated without exceed-
on
ing ΘLim at a given ambient temperature
is:
T
amb
P
on
=
ΘLim ± T
amb
R
th
Replacing the expression (1) in this equation
and solvingfor I
, we can find the maximum
out
current versus ambient temperature relationship:
ΘLim ± T
I
= √
outx
amb
R
DSONx
± Pq± P
R
th
os
2)In the ON state the power dissipatedin the
device is dueto three contributes:
a) power lost in the switch:
P
out
= I
out
2
⋅ R
DSON(Iout
is theoutput cur-
rent);
b) power due to quiescent current in the ON
state Iq,sunk by thedevice in additionto
I
out:Pq=Iq⋅Vs(Vs
isthe supplyvoltage);
c) an external LED could be used to visualize
the switchstate (OUTPUT STATUS pin).
Such a LEDis driven by aninternal current
source (deliveringI
) and therefore,if Vosis
os
the voltagedrop across the LED, thedissipated power is: P
= I
⋅( V
± V
os
os
s
).
os
Thus the total ON state power consumptionis
given by:
= P
P
on
+ Pq+ P
out
os
(1)
In theright side of equation 1, the secondand
6/12
where R
course, I
maximum operative current I
xisR
DSON
values are top limited by the
outx
at Tj=ΘLim. Of
DSON
outx
(500mA
nominal).
From the expression (2) we can also find the
maximum ambient temperature T
a given power P
T
amb
=ΘLim ±
( I
out
canbe dissipated:
on
=ΘLim± Pon⋅ Rth=
2
⋅ R
+ Pq+ Pos) ⋅ R
DSONx
amb
at which
th
In particular, this relation is useful to find the
maximum ambient temperature T
which I
T
ambx
+ P
canbe delivered:
outx
=ΘLim ±(I
+ Pos) ⋅ R
q
th
outx
2
⋅ R
DSONx
+
(4)
ambx
at
Referring to application circuit in fig. 5, let us consider the worstcase:
- The supply voltage is at maximumvalue of industrial bus (30V instead of the 24V nominal
value).This means also that I
risesof 25%
outx
Page 7
TDE1897C - TDE1898C
(625mAinstead of 500mA).
- All electrical parameters of the device, concerning the calculation, are at maximum values.
- Thermal shutdown threshold is at minimum
value.
- No heat sink nor air circulation (R
R
thj-amb
).
equal to
th
Therefore:
V
= 30V, R
s
=2.5V, ΘLim = 135°C
V
os
R
thj-amb
= 100°C/W (Minidip); 90°C/W (SO20);
= 0.6Ω,Iq= 6mA, Ios= 4mA @
DSON0
70°C/W(SIP9)
It follows:
I
= 0.625mA, R
outx
P
=110mW
os
= 1.006Ω,Pq= 180mW,
DSONx
Figure5: Application Circuit.
From equation 4, we can find:
= 66.7°C(Minidip);
T
ambx
73.5°C(SO20);
87.2°C(SIP9).
Therefore, the IPS TDE1897/1898, although
guaranteed to operate up to 85°C ambient temperature,if used in the worstconditions,can meet
some limitations.
SIP9 package, which has the lowest R
thj-amb
, can
work at maximum operative current over the entire ambient temperature range in theworst conditions too. For other packages, it is necessary to
consider some reductions.
With the aid of equation 3, we can draw a derating curve giving the maximum current allowable
versus ambienttemperature. The diagrams, computed using parameter values above given, are
depicted in figg. 6 to 8.
If an increase of the operating area is needed,
heat dissipation must be improved (R
Information furnished is believed to be accurate and reliable. However, SGS-THOMSON Microelectronics assumes no responsibility for the
consequences of use of such information nor for any infringement of patents or other rights of third parties which mayresult from its use. No
license is granted by implication or otherwise under any patent or patent rights of SGS-THOMSON Microelectronics. Specification mentioned
in this publication are subject to change without notice. This publication supersedes and replaces all information previously supplied. SGSTHOMSON Microelectronics products are not authorized for use as critical components in life support devices or systems without express
written approval of SGS-THOMSON Microelectronics.
1995 SGS-THOMSON Microelectronics – Printed in Italy – All Rights Reserved
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