ST AN1506 Application note

AN1506
APPLICATION NOTE
A MOTOR DRIVES SYSTEM FOR
WHEELCHAIR APPLICATIONS
G. Belverde - C. Guastella - M. Melito - A. Raciti
1. ABSTRACT
This paper deals with a new conc ept applied in designing low-voltage power MOSFE Ts that are suitable for high-current low-voltage converter application s. The layout of the proposed dev ice famil y overc om es the traditional cell structure by a new strip-based geometry. They present interesting characteristics due to the advanced de sign rules typical of VLS I processes and s trong reduction of the on-state resistance. Further, the technology process allows a significant simplification of the silicon fabrication steps, thus allowing to enhance the device ruggedness. The hig h current handling in switching conditions (up to 150A) with a breakdown voltage in the range betwe en 20-50V in a convenient pac kage solution gi ve the correct answers to the low-voltage range switch applications. This paper starts with the description of the main technology issues in comparison with that of standard devices, particularly focusing on the innovations and the improved performances. Moreover, a detailed characterization of the MOSFET behavior in a traditional test circuit as well as in an actual AC motor drive for wheel chair applications are presented and discussed.
2. INTRODUCTION.
Higher efficiencies are expected nowadays in the field of power converters for battery-powered systems. As industrial and commercial applications of these systems are increasing more and more (laptops, portable equipment, home appliances, electric assisted bikes, electric sc ooters, wheel chairs, mobiles, etc.), higher efficiencies become of major interest in order to meet the user requirem ents of long-lasting behavior with the sam e bat tery cha rge. To do that, researchers have made dra matic efforts in designing new converter structures, in increasing the converter switching freq uency and in conceiving innovative power devices.
Generally speaking, battery powered systems require low-voltage switching devices (<100V). Power MOSFET de vices domina te in thi s voltage range due to t heir attractive c haracteristics of high sw itching speed and easy driving capability. On-state losses of MOSFETs are of major concern on their total power loss balance, esp ecially in case of converters with low or medium sw itching frequency. Since on-state losses depend on the drain-source resistance (R
modern MOSFETs are realized with a cell-based layout, which determines low on-state resistance. The increase of the cell density allows to further reduce th e on-state resistance, thus increasing the current
capability per device area-unit. However, for today’ s state-of-the-art MOSFETs, ulterior reduction of the on-state resistance by this conventional layout is impeded since this approach is reaching its own physical limit [1]. The need of innovative approaches arises in order to overcome the limit of this technology.
), which is strictly related to the structure design, many
on
January 2002
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AN1506 - APPLICATION NOTE
The strip-based layout is a new approach [2], which allows using a simplified process for implant ing the body and isolating the poly silicon gate from the source. The new technology is very effective in eliminating the limit o f the cell-base d layout, which relies on the capability to open smaller and smaller windows on the poly silicon area in order to obtain greater cell-density figures. With the strip-based layout, MOSFET devices show improved performances and a simpler manufacturing process. Moreover, they benefit of the well-established and advanced design rules typical of VLSI processes. On-state resistance values as low as 1.2mcan be reached, but the overall MOSFET design must account for the best trade-off of a merit figure, which is the product of the on-state resistance and the gate charge values (R
on QG
).
In this paper the main issues of the new technology are briefly recalled, and the device structure is described and discussed. The static and dynamic characteristics of devi ces b elonging t o this new f am ily of MOSFETs are presented and compared with those of more traditional ones. Conventional experimental tests have bee n carried out a nd are discussed aiming to de termine the impact of turn on and turn off energy loss [3]. A low-voltage battery-powered converter for wheel chairs is used as a workbench for an application-oriented characterization. Some relevant tests are reported and discussed. A detailed analysis is done on the conduction and switching losses and the thermal behavior in the actual application.
3. MAIN TECHNOLOGY ISSUES OF STRIP-BASED MOSFET.
The structure of a strip-based MOSFET device overcomes the limit of a cell structur e. In figure 1 the geometry of the t wo differently conceived devices are s hown. The m ain differences between a stan dard square-cell layout and the strip imple mentation may be better unders tood by inspecting figure 2. In the conventional cell structure shown, all subsequent contacts and isolation openings must be co nfined a nd aligned inside the large st square windows opene d on the poly silicon layer whose side is L in fig ure 2. That dimension depends on the alignment, the resolution, and the process tolerances and can be expressed as:
Lc2b2t++=1()
where:
c is the contact dimension for the body region imposed by the resolution of the photolithography equipment;
b is the contact dimension for the source re gion which depends on the alignm ent c apability and on the metallization process;
t is the separation (isolation) between the poly and sou rce metal and is controlled by the alignment feature.
Consequently, the standard cell layout depends on three feature sizes.
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Figure 1. Cell-based and strip-based structures of two Power MOSFETs
L
S
source
body
In the strip-based layout process an intermediate dielectric layer is obtained after growing the gate oxide and depositing the poly silicon. In such a sandwich structure parallel strips are opened through an appropriate photo masking process. After implanting the body, the source regions are created by using a sort of small rectangle (patches) masking. The longer sides of the patches are perpendicular to the strips in such a way that they do not need t o be aligned within the strip but only along their spacing, which normally is larger than the opening, thus a voiding any alignment problem. Th e nex t s tep is to isolate the
poly silicon along the stripe’ s pe riphery thanks to the spacer proces s. Etching the dielectric material originally deposited and creating “hills”on the sides of the strips achieve this. Finally, Aluminum deposition is done in order to contact the strips, and the fabrication flow chart is completed.
L
S
source
body
Figure 2. Cell-based and strip-based structures of two Power MOSFETs showing the key parameters of the elemental component of the geometry
a) b)
p
n
bt
c
L cbt
source
body
source
p
n+
p
n+
p-vapox
poly
SiO2
n+
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The source mask d oes not need to be aligned wit hin the strip itself; the only critical parameter is the width of the strip (see figure 1), which depends on the equipm ent res olution. As can be argued from the above description, the process benefits in a reduced number of feature sizes since it is now only dependent on a single feature size, and higher packing dens ities can be obtained in comparison to the conventional cell-geometry process. The new process is also named Extremely High Density (EHD) referring to the possibility of getting devices with very high equivalent cell densities. Figure 3 compares the obtainable channel perimeter density and thus the current density of the two structures.
Figure 3. Channel perimeter density comparison of cell-based and strip-based structures
30
]
2
25
20
Cell-based layout
Strip-based layout
15
Channel perimeter density [cm/mm
10
87654321
Minimum feature size [µm]
4. STATIC AND DYNAMIC BEHAVIOR OF THE NEW DEVICE.
The resulting MOSFET device of the strip-based process shows very interesting characteristics: extremely high packing densit y and low on -state resistance, rugged aval anche charact eristics, and less critical alignment steps. First of all we have selected the device STB8 0NF55, which was the cand idate for the actual application in an AC drive. The drive is described with more details in the next section. The main electrical quantities of the component are summarized in Table 1.
Table 1. STB80NF55 Main Electrical Characteristics
R
on
[m]
6.5 55 180 90 66 80 245 6.4
A preliminary characterization in a dc chopper working on indu ctive load has been done. Looking for the specific application supplied at a dc bus of 24V, several commutation tests (turn on and turn off) have been done at this voltage while the current assumed a variable value. The energy losses in such conditions are reported in figure 4. Linear dependence of the energy versus the switched current is evident both for the turn on and turn off transients.
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BV
DSS
[V]
Q
G
[nC]
Qsw [nC]
Qgd [nC]
trr
[nS]
Qrr
[nC]
Irr
[A]
Package
2
PAK
D
AN1506 - APPLICATION NOTE
Figure 4. Energy losses during turn off and turn on transients versus the drain current at VDS=24V
E [µJ]
60
50
40
E
off
30
20
10
E
on
0
510152025
I [A]
Since the performances of the body-drain diode could be conveniently exploited in bridge topologies, the characteristics of this intrinsic diode have been tested. A favorable characteristic of this internal body­drain diode is its high dv/dt capability; crucial in all bridge topologies such as motor drives or uninterruptible power supply (UPS). For the used device the allowed limit is 10V/ns. Finally in figure 5 the static characteristics of the new MOSFET are reported. In forward conduction (positive drain voltage) the I/V characteristic of the M OSFET is traced . In reverse conduction two static characteristics are reported relative to the MOSFET and the intrinsic diode: at zero source-gate voltage the current will flow exclusively as a diode current; with a gate bias voltage the current will flow through t he MOSFET as in the case of synchronous rectifier applications.
Figure 5. Static characteristics of the new MOSFE T and its body-drain diode at a temperature of
125°C
VDS[V]
150
100
MOS
50
-0
-50 DIODE
-100
-150
1.5 -1 -0.5 0 0.5 1 1.5
[A]
I
D
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