0.5A OUTPUT CURRENT
18V TO 35V SUPPLY VOLTAGE RANGE
INTERNAL CURRENT LIMITING
THERMAL SHUTDOWN
OPEN GROUND PROTECTION
INTERNAL NEGATIVE VOLTAGE CLAMPING
TO V
- 45V FOR FAST DEMAGNETIZATION
S
DIFFERENTIAL INP UTS WITH LARGE COMMON MODE RANGE AND THRESHOLD
HYSTERESIS
UNDERVOLTAGE LOCKOUT WITH HYSTERESIS
OPEN LOAD DETECTION
TWO DIAGNOSTIC OUTPUTS
OUTPUT STATUS LED DRIVER
DESCRIPTION
The TDE1897C/TDE1898C is a monolithic Intelligent Power Switch in Multipower BCD Technol-
BLOCK DIAGRAM
TDE1898C
0.5A HIGH-SIDE DRIVER
MULTIPOWER BCD TECHNOLOGY
Minidip SIP9 SO20
ORDERING NUMBERS:
TDE1897CDP TDE1898CSP TDE1897CFP
TDE1898CDP TDE1898CFP
ogy, for driving inductive or resistive loads. An internal Clamping Diode enables the fast demagnetization of inductive loads.
Diagnostic for CPU feedback and extensive use
of electrical protections make this device inherently indistructible and suitable for general purpose industrial applications.
September 2003
1/12
Page 2
TDE1897C - TDE1898C
PIN CONNECTIONS
SIP9
(Top view)
Minidip
SO20
ABSOLUTE MAXIMUM RATINGS
(Minidip pin reference)
SymbolParameterValueUnit
Supply Voltage (Pins 3 - 1) (TW < 10ms)50V
V
S
VS – V
V
V
I
I
O
E
P
tot
T
op
T
stg
Supply to Output Differential Voltage. See also VCl 3-2 (P i ns 3 - 2)internally limitedV
O
Input Voltage (Pins 7/8)-10 to VS +10V
i
Differential Input Voltage (Pins 7 - 8)43V
i
Input Current (Pins 7/8)20mA
i
Output Current (Pins 2 - 1). See also ISCinternally limitedA
Energy from Inductive Load (TJ = 85°C)200mJ
l
Power Dissipation. See also THERMAL 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.
Figure 1
DIAGNOSTIC TRUTH TABLE
Diagnostic ConditionsInputOutputDiag1Diag2
Normal OperationL
H
< I
Open Load Condition (I
)L
o
old
H
Short to V
L
S
H
Short Circuit to Ground (I
TDE1898C
= ISC) (**) TDE1897C
O
H<H (*)HL
HH
Output DMOS OpenL
H
OvertemperatureL
H
Supply Undervoltage (V
ply voltage; V
(*) According to the intervention of the current limiting block.
(**) A cold lamp filament, or a capacitive load may activate the current limiting circuit of the IPS, when the IPS is initially turned on. TDE1897
uses Diag2 to signal such condition, TDE1898 does not.
S
< V
< V
S
in the rising phase of the supply voltage)
sth2
in the falling phase of the sup-
sth1
L
H
L
H
L
H
H
H
L
L
L
L
L
L
L
H
H
H
L
L
L
H
H
H
L
H
H
L
L
H
H
H
H
H
H
H
H
H
H
L
L
L
L
4/12
Page 5
TDE1897C - TDE1898C
APPLICATION IN FOR MATION
DEMAGNETIZATION OF INDUCTIVE LOADS
An internal zener diode, limiting the voltage
across the Power MOS to between 45 and 55V
), provides safe and fast demagnetization of
(V
cl
inductive loads 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 maximum switching frequency three
points have to be considered:
1) The total power dissipation is the sum of the
On State Power and of the Demagnetization
Energy multiplied by the frequency.
2) The total energy W dissipated in the device
during a demagnetization cycle (figg. 2, 3) is:
W = V
V
L
[Io –
cl
R
L
cl
R
– V
L
s
log
1 +
V
s
Vcl – V
]
s
Where:
V
= clamp voltage;
cl
L = inductive load;
= resistive load;
R
L
Vs = supply voltage;
= I
I
O
LOAD
3) In normal conditions the operating Junction
temperature should remain below 125°C.
Figure 3:
Demagnetization Cycle Waveforms
Figure 2:
Inductive Load Equivalent Circuit
Figure 4:
α
1.8
1.6
1.4
1.2
1.0
0.8
0.6
Normalized R
vs. Junction
DSON
Temperature
D93IN018
RDSON (Tj)
α=
RDSON (Tj=25˚C)
-250255075100 125Tj (˚C)
5/12
Page 6
TDE1897C - TDE1898C
WORST CONDITION POWER DISSIPATION IN
THE ON-S TA T E
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 package and ambient temperature.
At ambient temperature close to upper limit
(+85°C) and in the worst operating conditions, it is
possible that the chip temperature could increase
so much to make the thermal shutdown procedure untimely 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 following points:
1) The ON resistance R
of the output
DSON
NDMOS (the real switch) of the device increases with its temperature.
Experimental results show that silicon resistivity increases with temperature at a constant
rate, rising of 60% from 25°C to 125°C.
The relationship between R
DSON
and tem-
perature is therefore:
R
DSON
= R
DSON0
( 1
+ k )
(
T
− 25
j
)
where:
Tj is the silicon temperature in °C
DSON0
is R
R
k is the constant rate (k = 4.711 ⋅
DSON
at Tj=25°C
10
−
3
)
(see fig. 4).
the third element are constant, while the first
one increases with temperature because
increases as well.
R
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 temperature T
T
to the silicon temperature Tj and
− T
j
on
= P on ⋅ R
amb
th
:
amb
(2)
From this relationship, the maximum power
which can be dissipated without exceed-
P
on
ing ΘLim at a given ambient temperature
is:
T
amb
Θ
P
on
=
Lim − T
R
amb
th
Replacing the expression (1) in this equation
and solving for I
, we can find the maximum
out
current versus ambient temperature relationship:
Θ
−
Lim
T
I
R
√
outx
=
th
amb
R
DSONx
− P q − P
os
2) In the ON state the power dissipated in the
device is due to three contributes:
a) power lost in the switch:
= I
P
out
out
2 ⋅ R
DSON
(I
is the output cur-
out
rent);
b) power due to quiescent current in the ON
state Iq, sunk by the device in addition to
: P q = I q ⋅ V
I
out
(Vs is the supply voltage);
s
c) an external LED could be used to visualize
the switch state (OUTPUT STATUS pin).
Such a LED is driven by an internal current
source (delivering I
) and therefore, if Vos is
os
the voltage drop across the LED, the dissi-
)
pated power is: P
= I os ⋅ ( V s − V
os
.
os
Thus the total ON state power consumption is
given by:
P
on
= P
+ P q + P os (1)
out
In the right side of equation 1, the second and
6/12
where R
course, I
maximum operative current I
x is R
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
Lim −
(
I
out
= Θ
can be dissipated:
on
= ΘLim − P
2 ⋅ R
DSONx
⋅
R th
on
+
P q + P os ) ⋅ R
at which
amb
=
th
In particular, this relation is useful to find the
maximum ambient temperature T
which I
T
ambx
+
can be delivered:
outx
= ΘLim − ( I
P
+ P
q
os
2 ⋅ R
outx
) ⋅
R
(4)
th
DSONx
+
ambx
at
Referring to application circuit in fig. 5, let us consider the worst case:
- The supply voltage is at maximum value of industrial bus (30V instead of the 24V nominal
value). This means also that I
rises of 25%
outx
Page 7
TDE1897C - TDE1898C
(625mA instead 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
thj-amb
).
R
equal to
th
Therefore:
V
= 30V, R
s
= 2.5V, ΘLim = 135°C
V
os
R
= 100°C/W (Minidip); 90°C/W (SO20);
thj-amb
= 0.6Ω, Iq = 6mA, I
DSON0
= 4mA @
os
70°C/W (SIP9)
It follows:
I
= 0.625mA, R
outx
= 1.006Ω, Pq = 180mW,
DSONx
Pos = 110mW
Figure 5:
Application Circuit.
From equation 4, we can find:
T
= 66.7°C (Minidip);
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 worst conditions, 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 the worst 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 ambient temperature. 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
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