SUM50N03-13LC [VISHAY]

Current-Sensing Power MOSFETs; 电流检测功率MOSFET
SUM50N03-13LC
型号: SUM50N03-13LC
厂家: VISHAY    VISHAY
描述:

Current-Sensing Power MOSFETs
电流检测功率MOSFET

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AN606  
Vishay Siliconix  
Current-Sensing Power MOSFETs  
Kandarp Pandya  
INTRODUCTION  
Vishay Siliconix current-sensing power MOSFETs offer a  
simple means of incorporating a protection feature into an  
electronic control circuit and avoiding catastrophic failures  
resulting from overcurrent (overload) and/or short-circuit  
conditions. The device package is a modified D2PAK with five  
pins. The MOSFET termination retains the standard D2PAK  
footprint for a three-pin device. The additional two pins provide  
termination for a current-sense output and an internal Kelvin  
connection to the source. For current sensing, the MOSFET  
design employs a small number of the total number of  
MOSFET cells in a known ratio. The latter define the  
current-sense parameters. A typical control interface uses a  
simple circuit with an op-amp or a comparator. This approach  
offers the freedom of control-level setting and facilitates its  
incorporation into the main control system.  
between gate and drain-stub and between drain-stub and source,  
respectively. See Application Note 826, Recommended Minimum  
Pad Patterns With Outline Access for Vishay Siliconix  
MOSFETs  
(http://www.vishay.com/doc?72286),  
for  
the  
recommended PCB layout dimensional details of the pad pattern.  
Modified-part library symbols for schematic symbol and PCB  
layout are available on the “Protel” (PCB design software)  
platform. For soft copy, please contact Vishay Siliconix in Santa  
Clara, Calif., in the United States, by phoning 1-408-567-8927.  
The Principle Behind the Current-Sensing Feature  
The most efficient way to sense the drain-source current is to  
use the ratio-metric measurement. In a power MOSFET, it is  
possible to implement this method easily.  
DEVICE DESCRIPTION AND PRINCIPLE OF  
OPERATION  
The cell density, a favored term within the power MOSFET  
industry, conveys that the power MOSFET structure consists  
of many cells connected in parallel. In principle, these cells  
constitute a resistive path for drain-source current. Electrically,  
these cells are parallel connected resistors, rDS(on)s. Each cell  
- being identical in structure and electrical characteristics -  
shares the current equally when the device is on. This property  
enables design of a MOSFET with a current-sensing feature.  
D (Tab, 3)  
2
D PAK-5  
(1)  
(2)  
(4)  
Dividing the MOSFET cells in a known ratio creates two paths  
that share the drain-source current. The path with the smaller  
number of cells constitutes the sense current, which is much  
smaller than the current conducting through the rest of the  
cells. A very simple, low-power, external circuit can measure  
this current. Multiplying this value with the cell ratio gives the  
total drain-source current.  
KELVIN  
G
1 2 3 4 5  
SENSE  
S (5)  
N-Channel MOSFET  
G
D
S
SENSE  
KELVIN  
The classic Kelvin termination for the return of sense current  
to the main source connection insures the measurement  
accuracy. This terminal not only eliminates the ground loop,  
but also minimizes the imbalance of internal structures with  
two current paths.  
FIGURE 1. Package Information and Schematic Symbol  
Package Information and Schematic Symbol, Figure 1, shows a  
partial reproduction of a datasheet for a current-sensing  
MOSFET, SUM50N03-13C. Gate, drain-stub/tab, and source  
(pins 1, 2, and 3) are in the same position as in a standard D2PAK  
(TO-263) MOSFET. However, pin-out modification is required to  
incorporate current-sense (pin 2) and Kelvin-to-source (pin 4)  
The Current-Sensing Parameters, Table 1, and the  
Current-Sense Die Characteristics and Schematic, Figure 2,  
help to demonstrate the current-sensing operation and circuit  
implementation.  
TABLE 1: Current Sense Characteristics  
Current Sensing Ratio  
r
I
D
= 1 A, V  
= 10 V, R = 1.1 W  
SENSE  
420  
520  
3.5  
620  
GSS  
Mirror Active Resistance  
r
V
GS  
= 10 V, I = 10 mA  
W
m(on)  
D
Document Number: 71991  
17-Dec-03  
www.vishay.com  
1
AN606  
Vishay Siliconix  
TYPICAL CHARACTERISTICS (25_C UNLESS NOTED)  
SENSE DIE  
On-Resistancevs. Sense Current  
On-Resistance vs. Gate-Source Voltage  
10  
10  
8
8
I
D
= 10 mA  
6
4
2
0
V
GS  
= 4.5 V  
6
V
GS  
= 10 V  
4
2
0
0.00  
0.02  
0.04  
0.06  
(A)  
0.08  
0.10  
0
2
4
6
8
10  
I
V
GS  
Gate-to-Source Voltage (V)  
SENSE  
Current Ratio (I  
)
(MAIN)/IS  
vs. Gate-Source Voltage (Figure 1)  
1200  
1000  
800  
600  
400  
200  
0
R
S
= 6.6 W  
R
= 4.7 W  
S
G
R
R
= 2.2 W  
= 1.1 W  
S
SENSE  
S
KELVIN  
V
G
S
R
S
R
S
= 0.5 W  
0
4
8
12  
16  
20  
V
GS  
Gate-to-Source Voltage (V)  
FIGURE 2. Current-Sensing Die Characteristics and Schematic  
Definition of Current-Sensing Parameters  
ISENSE is the current flowing out of the sense terminal and into  
the sense resistor, RSENSE  
The current-sense ratio, r, is the quotient of the number of cells  
terminated on the sense terminal to the total number of cells on  
the MOSFET die.  
Mirror active resistance, rm(on), is the resistance of parallel  
connected cells used in the sense chain when the device is on.  
Being rDS(on) as in any other MOSFET, the value depends on  
the gate drive, drain current, and junction temperature.  
Accordingly, rm(on) is defined at given values of VGS, IDRAIN  
and TJ junction.  
,
To derive the value of r using the above definition requires  
detailed die design. However, the quotient of drain current to  
the sense current provides the same value because these  
current values are the sum of cell current in each path.  
By definition, for the sense die, refer to Figure 2. Mirror active  
resistance rm(on) is specified at the gate-source voltages, VGS  
at 4.5 V and 10 V, corresponding drain-source current ISENSE  
up to 0.1 A, and junction temperature TJ at 25 _C. The  
Mathematically:  
temperature coefficient of rm(on) is the same as that of rDS(on)  
Refer to the on-resistance vs. junction temperature curve in  
.
r = ID/ISENSE  
ID is drain current  
Figure 3.  
Document Number: 71991  
17-Dec-03  
www.vishay.com  
2
AN606  
Vishay Siliconix  
On-Resistance vs. Junction Temperature  
2. use a minimum value of the ISENSE signal at the maximum  
value of ID; and  
2.0  
1.8  
1.6  
1.4  
1.2  
1.0  
0.8  
0.6  
V
I
= 10 V  
GS  
= 25 A  
D
3. use a fast comparator with hysterisis to control and protect  
the MOSFET.  
Typical schematic configurations for implementing the current  
sense are shown in Figure 4 and Figure 5.  
The Virtual Earth Sensing Scheme, Figure 4, is suitable for  
applications aiming at higher noise immunity and speed. This  
approach also improves measurement accuracy by  
eliminating the sense resistor. However, a dual power supply  
and inverted (negative) output signal are the price designers  
pay for deriving these benefits.  
50 25  
0
25  
50  
75 100 125 150 175  
T
J
Junction Temperature (_C)  
The Resistor Sensing Scheme shown in Figure 5 is a quite  
simple and economical approach. The accuracy of current  
measurement is affected by the introduction of an external  
sense resistor RS. However, the latter aids in lowering the  
temperature sensitivity of the current-sense signal.  
FIGURE 3. Normalized r  
for the Sense Die  
m(on)  
DESIGN EQUATIONS  
V
DD  
The following three equations enable circuit design and  
analysis.  
Load  
I
L
D
ISENSE = x ID/r  
Kelvin  
VDS = ISENSE x [rm(on) + RSENSE] or  
G
VDS = ID x rDS(on)/(rm(on) + RSENSE)  
+V  
Sense  
VSENSE = ISENSE x RSENSE or  
VSENSE = VDS x RSENSE/(rm(on) + RSENSE  
+
V
1
)
Where ISENSE  
Current flowing out of sense terminal  
Current-sensing ratio  
Drain-source current  
V  
r
ID  
S
VDS  
rm(on)  
Drain-source voltage  
Mirror active resistance  
FIGURE 4. Virtual Earth Sensing Scheme  
RSENSE External current-sense resistor  
V
DD  
Load  
Application Aspects and Design Examples  
I
L
D
The current-sense ratio r, even though fixed by design, is  
R3  
dependent  
on  
manufacturing  
process  
variations.  
Kelvin  
R2  
Furthermore, mirror active resistance rm(on) depends on circuit  
parameters VGS and ID and junction temperature TJ. As a  
result, a practical design can realize an accuracy of 15% —  
20% for current sensing. Accordingly, the current-sensing  
MOSFET is most suitable for supervisory functions such as  
overcurrent and/or short-circuit protection.  
G
R1  
V
1
+
Sense  
S
Stray  
Resistance  
Three keys to a successful design are to:  
1. have an adequate margin between the normal  
operating-current value and the trip-current value;  
FIGURE 5. Resistor Sensing Scheme  
Document Number: 71991  
17-Dec-03  
www.vishay.com  
3
AN606  
Vishay Siliconix  
TABLE 2: Current Product Range  
Part #  
Channel Type  
VDS (VDC)  
rDS (W)  
IDS (A)  
PD (W)  
Package  
N
N
20  
30  
0.026/4.5 V  
0.015/10 V  
6.6  
1.8  
3.6  
TSSOP-8*  
SO-8*  
Si6862DQ  
Si4730EY  
11.7  
N
N
30  
75  
0.013/10 V  
0.007/10 V  
50  
60  
83  
SUM50N03-13LC  
SUM60N08-07C  
2
D PAK-5  
300  
Recommended minimum pads for current-sensing MOSFETs in TSSOP-8 and SOIC-8 packages see application note AN826  
(http://www.vishay.com/doc?72286).  
CONCLUSION  
Vishay Siliconix current-sensing power MOSFETs enable  
implementation of  
a simple solution for incorporating  
supervisory protection features such as overcurrent and/or  
short circuit. This approach offers the freedom and flexibility of  
control-circuit design, though the accuracy of measurement is  
not suitable for current-control applications. Virtually any  
power MOSFET from the Vishay Siliconix product range can  
be supplied with a current-sensing feature.  
Document Number: 71991  
17-Dec-03  
www.vishay.com  
4

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