The TDE1890/1891 is a monolithic Intelligent
Power Switch in Multipower BCD Technology, for
BLOCK DIAGRAM
- 50VFOR FASTDEMAGNETIZATION
S
TDE1891
2A HIGH-SIDE DRIVER
MULTIPOWER BCD TECHNOLOGY
MULTIWATT11 MULTIWATT11V PowerSO20
(In line)
ORDERING NUMBERS:
TDE1891LTDE1890VTDE1890D
TDE1891V
driving inductive or resistive loads. An internal
ClampingDiode enablesthe fast demagnetization
of inductiveloads.
Diagnostic for CPU feedback and extensive use
of electrical protections make this device extremely rugged and specially suitable for industrial automationapplications.
July 1998
1/12
Page 2
TDE1890 - TDE1891
PIN CONNECTION (Topview)
11
10
9
8
7
6
5
4
3
2
1
D93IN022
OUTPUT
SUPPLY VOLTAGE
OUTPUT
N.C.
N.C.
GND
OUTPUT STATUS
INPUT INPUT +
DIAGNOSTIC 2
DIAGNOSTIC 1
Note: Output pins mustbe must be connectedexternally to the package touse allleadsfor the outputcurrent (Pin9 and 11 for Multiwatt
package, Pin 2, 3, 8 and 9 for PowerSO20package).
ABSOLUTE MAXIMUM RATINGS
SymbolParameterValueUnit
V
V
S–VO
V
V
I
P
T
T
E
S
I
O
tot
op
stg
Supply Voltage (Pin 10) (TW< 10ms)50V
Supply toOutputDifferential Voltage. Seealso VCl(Pins10 - 9)internally limitedV
Input Voltage (Pins 3/4)-10 to VS +10V
i
Differential Input Voltage (Pins 3 - 4)43V
i
Input Current (Pins 3/4)20mA
i
Output Current(Pin 9). See also ISC (Pin 9)internally limitedA
Power Dissipation.See also THERMAL CHARACTERISTICS.internally limitedW
Operating Temperature Range (T
)-25 to +85°C
amb
Storage Temperature-55 to 150°C
Energy Induct.Load TJ=85°C1J
Turn on Delay Time200µs
Turn off Delay Time40µs
Input Switchingto Diagnostic
200µs
Valid
Note Vil < 0.8V, Vih > 2V@ (V+In> V–In)
Figure 1
TRUE
FALSE
HIGH
LOW
DIAGNOSTICTRUTHTABLE
Diagnostic ConditionsInputOutputDiag1Diag2
Normal OperationL
H
Open Load Condition (I
)L
o<Iold
H
Short to V
S
L
H
Short Circuit to Ground (I
) (**)TDE1891
O=ISC
TDE1890
H<H (*)HL
HH
Output DMOS OpenL
H
OvertemperatureL
H
Supply Undervoltage (V
S<Vsth2
)L
H
(*) According to theintervention of the current limitingblock.
(**) A cold lampfilament,or a capacitiveload may activate the current limiting circuit of the IPS, when the IPSis initially turned on. TDE1891
uses Diag2 to signal such condition, TDE1890 does not.
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
TDE1890 - TDE1891
APPLICATIONINFORMATION
DEMAGNETIZATION OF INDUCTIVE LOADS
An internal zener diode, limiting the voltage
across the Power MOS to between 50 and 60V
(V
), provides safe and fast demagnetization of
cl
inductiveloads without externalclamping devices.
The maximum energy that can be absorbed from
an inductive load is specified as 1J (at
T
=85°C).
j
To define the maximumswitching frequencythree
points haveto 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 demagnetizationcycle(figg.2, 3) is:
W=V
L
[Io–
V
cl–Vs
R
log
L
L
cl
R
1
+
Vcl–V
V
s
]
s
Where:
= clampvoltage;
V
cl
L = inductiveload;
=resistiveload;
R
L
Vs = supply voltage;
I
O=ILOAD
3) In normal conditions the operating Junction
temperatureshouldremain below 125°C.
If the demagnetization energy exceeds the rated
value, an externalclamp between output and +V
must be externallyconnected(see fig. 5).
The external zener will be chosen with V
zener
value lower than the internal Vclminimum rated
value and significantly (at least 10V) higher than
the voltage that is externally supplied to pin 10,
i.e. than the supplyvoltage.
Alternative circuit solutions can be implemented
to divert the demagnetization stress from the
TDE1890/1, if it exceeds 1J. In all cases it is recommended that at least 10V are available to demagnetizethe loadin the turn-offphase.
A clampingcircuitconnected between ground and
the output pin is not recommended. An interruption of the connection between the ground of the
load and the ground of the TDE1890/1 would
leave the TDE1890/1 alone to absorb the full
amountof the demagnetizationenergy.
S
Figure 2: InductiveLoad EquivalentCircuit
5/12
Page 6
TDE1890 - TDE1891
Figure 3: DemagnetizationCycle Waveforms
Figure4: NormalizedR
Temperature
α
1.8
RDSON (Tj)
α=
1.6
1.4
1.2
1.0
0.8
0.6
-250255075 100 125Tj (°C)
RDSON (Tj=25°C)
DSON
vs. Junction
D93IN018
Figure 5.
6/12
Page 7
TDE1890 - TDE1891
WORST CONDITION POWER DISSIPATION IN
THE ON-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 packageandambient temperature.
At ambient temperature close to upper limit
(+85°C) and in the worstoperating conditions, it is
possible that the chip temperature could increase
so much to make the thermal shutdown procedure untimelyintervene.
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
DSON
of the output
NDMOS (the real switch) of the device increaseswithits temperature.
Experimentalresults 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-
peratureis therefore:
R
DSON
=
R
DSON0
( 1 +k)
( Tj− 25 )
where:
T
isthe silicon temperaturein °C
j
DSON0
is R
R
k isthe constantrate (k=4.711
DSON
atTj=25°C
−3
⋅
10
)
(seefig. 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 deviceambient (R
parameter relates the power dissipated P
the silicon temperature T
temperatureT
− T
T
j
). In steady state conditions, this
th
and the ambient
j
th
amb
:
amb
= Pon⋅ R
on
(2)
From this relationship, the maximum power
which can be dissipated without exceed-
P
on
ing ΘLim at a given ambient temperature
T
is:
amb
Θ
Lim−T
=
P
on
amb
R
th
Replacing the expression (1) in this equation
and solving for I
, we can find the maximum
out
current versus ambient temperature relationship:
Θ
I
Lim−T
√
=
outx
amb
R
− Pq−P
DSONx
R
th
os
to
2)In the ON state the power dissipated in the
deviceis due to three contributes:
a) power lost in the switch:
P
out
2
=
⋅
out
R
I
DSON
(I
is the outputcur-
out
rent);
b) power due to quiescentcurrentin the ON
state Iq, sunk by the devicein addition to
=
:P
I
out
⋅
I
q
(Vsisthe supplyvoltage);
V
q
s
c) an external LED could be usedto visualize
the switch state (OUTPUT STATUSpin).
Such a LED is drivenby an internalcurrent
source(deliveringI
) and therefore, if Vosis
os
the voltage drop across the LED, the dissi-
=
⋅(
−
)
pated power is: P
I
os
V
s
os
.
V
os
Thus the total ON state power consumptionis
given by:
P
on
= P
+ Pq+ P
out
os
(1)
In the right sideof equation1, the second and
where R
course, I
maximumoperativecurrent I
xisR
DSON
values are top limited by the
outx
at Tj=ΘLim. Of
DSON
outx
(2Anominal).
From the expression (2) we can also find the
maximum ambient temperature T
a givenpower 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
whichI
T
ambx
+ P
can be delivered:
outx
=ΘLim −(I
+ Pos) ⋅ R
q
th
outx
2
⋅ R
DSONx
+
(4)
ambx
at
Referring to application circuit in fig. 6, 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
risesof 25%
outx
(2.5A instead of 2A).
7/12
Page 8
TDE1890 - TDE1891
- All electricalparametersof the device, concerningthe calculation,areat maximumvalues.
- Thermal shutdownthresholdis at minimum
value.
Therefore:
V
= 30V, R
s
@V
R
thj-amb
= 2.5V, ΘLim = 135°C
os
=35°C/W
= 0.23Ω,Iq= 8mA, Ios= 4mA
DSON0
Figure 6: ApplicationCircuit
DC BUS 24V +/-25%
+IN
-IN
µP POLLING
D1
D2
It follows:
I
outx
P
= 110mW
os
= 2.5A,R
= 0.386Ω,Pq= 240mW,
DSONx
From equation 4 we can see that, without any
heatsink, it is not possible to operate in the ON
steady state at the maximum current value. A
derating curve for this case is reported in fig. 7.
Usingan external heatsink,in order to obtain a total R
(1) ”D and F” do not include mold flash or protrusions.
- Moldflash or protrusionsshall not exceed 0.15mm (0.006”).
- Criticaldimensions: ”E”, ”G” and ”a3”
NN
a2
b
E2
hx45°
DETAIL A
e3
H
D
T
110
e
1120
A
E1
DETAIL B
PSO20MEC
R
lead
a3
Gage Plane
BOTTOM VIEW
E
DETAIL B
0.35
S
D1
a1
L
DETAIL A
slug
(COPLANARITY)
E3
c
-C-
SEATING PLANE
GC
11/12
Page 12
TDE1890 - TDE1891
Information furnished is believed to be accurate and reliable. However, STMicroelectronics assumes no responsibility for the consequences
of use of such information nor for any infringement of patents or other rights of third parties which may result from its use. No license is
granted by implication or otherwise under any patent or patent rights of STMicroelectronics. Specification mentioned in this publication are
subject to change without notice. This publication supersedes and replaces all information previously supplied. STMicroelectronics products
are not authorized for use as criticalcomponents in life support devices or systems without express written approval of STMicroelectronics.
The ST logo is a registered trademark of STMicroelectronics
MULTIWATTis a RegisteredTrademark of STMicroelectronics
PowerSO20 is a Trademark of STMicroelectronics
1998 STMicroelectronics – Printed in Italy – AllRights Reserved
STMicroelectronics GROUP OF COMPANIES
Australia - Brazil - Canada - China - France - Germany - Italy - Japan - Korea - Malaysia - Malta- Mexico - Morocco -The Netherlands -
Singapore - Spain - Sweden - Switzerland- Taiwan - Thailand - United Kingdom - U.S.A.
12/12
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