NTD25P03L Power MOSFET −25 A, −30 V, Logic Level P−Channel DPAK Designed for low voltage, high speed switching applications and to withstand high energy in the avalanche and commutation modes. The source−to−drain diode recovery time is comparable to a discrete fast recovery diode. Typical Applications • • • • • PWM Motor Controls Power Supplies Converters Bridge Circuits Pb−Free Package is Available http://onsemi.com V(BR)DSS RDS(on) TYP ID MAX −30 V 51 m @ 5.0 V −25 A D P−Channel G MAXIMUM RATINGS (TJ = 25°C unless otherwise noted) Unit Drain−to−Source Voltage VDSS −30 V Gate−to−Source Voltage − Continuous − Non−Repetitive (tp ≤ 10 ms) VGS VGSM 15 20 V Vpk Drain Current − Continuous @ TA = 25°C − Single Pulse (tp ≤ 10 s) ID IDM −25 −75 A Apk Total Power Dissipation @ TA = 25°C PD 75 Watts Operating and Storage Temperature Range TJ, Tstg −55 to +150 °C EAS 200 mJ Single Pulse Drain−to−Source Avalanche Energy − Starting TJ = 25°C (VDD = 25 Vdc, VGS = 5.0 Vdc, Peak IL = 20 Apk, L = 1.0 mH, RG = 25 ) Thermal Resistance − Junction−to−Case − Junction−to−Ambient (Note 1) − Junction−to−Ambient (Note 2) Maximum Lead Temperature for Soldering Purposes, (1/8″ from case for 10 s) S 4 RJC RJA RJA 1.65 67 120 TL 260 °C Maximum ratings are those values beyond which device damage can occur. Maximum ratings applied to the device are individual stress limit values (not normal operating conditions) and are not valid simultaneously. If these limits are exceeded, device functional operation is not implied, damage may occur and reliability may be affected. 1. When surface mounted to an FR4 board using 0.5 sq in pad size. 2. When surface mounted to an FR4 board using the minimum recommended pad size. 4 Drain 1 2 3 DPAK CASE 369C (Surface Mount) Style 2 2 1 3 Drain Gate Source 4 4 Drain 1 °C/W MARKING DIAGRAMS YWW 25P 03L Value YWW 25P 03L Symbol Rating 2 3 DPAK CASE 369D (Straight Lead) Style 2 25P03L Device Code Y = Year WW = Work Week 1 2 3 Gate Drain Source ORDERING INFORMATION Package Shipping† DPAK 75 Units/Rail NTD25P03LG DPAK (Pb−Free) 75 Units/Rail NTD25P03L1 DPAK Straight Lead 75 Units/Rail NTD25P03LT4 DPAK 2500/Tape & Reel Device NTD25P03L †For information on tape and reel specifications, including part orientation and tape sizes, please refer to our Tape and Reel Packaging Specification Brochure, BRD8011/D. Semiconductor Components Industries, LLC, 2004 August, 2004 − Rev. 1 1 Publication Order Number: NTD25P03L/D NTD25P03L ELECTRICAL CHARACTERISTICS (TC = 25°C unless otherwise noted) Symbol Characteristic Min Typ Max Unit OFF CHARACTERISTICS Drain−to−Source Breakdown Voltage (Note 3) (VGS = 0 Vdc, ID = −250 A) Temperature Coefficient (Positive) V(BR)DSS Zero Gate Voltage Drain Current (VDS = −30 Vdc, VGS = 0 Vdc, TJ = 25°C) (VDS = −30 Vdc, VGS = 0 Vdc, TJ = 125°C) IDSS Gate−Body Leakage Current (VGS = ±15 Vdc, VDS = 0 Vdc) IGSS V −30 mV/°C −24 A −1.0 −100 nA −100 ON CHARACTERISTICS (Note 3) Gate Threshold Voltage (VDS = VGS, ID = −250 Adc) Temperature Coefficient (Negative) VGS(th) Static Drain−to−Source On−State Resistance (VGS = −5.0 Vdc, ID = −12.5 Adc) (VGS = −5.0 Vdc, ID = −25 Adc) (VGS = −4.0 Vdc, ID = −10 Adc) RDS(on) V −1.0 Forward Transconductance (VDS = −8.0 Vdc, ID = −12.5 Adc) −1.6 4.0 −2.0 0.051 0.056 0.065 0.072 0.080 0.090 mV/°C gFS Mhos 13 DYNAMIC CHARACTERISTICS Input Capacitance Output Capacitance (VDS = −25 Vdc, VGS = 0 Vdc, f = 1.0 MHz) Reverse Transfer Capacitance pF Ciss 900 1260 Coss 290 410 Crss 105 210 td(on) 9.0 20 tr 37 75 td(off) 15 30 tf 16 55 QT 15 20 nC Q1 3.0 Q2 9.0 Q3 7.0 VSD −1.0 −0.9 −1.5 V trr 35 ta 20 tb 14 QRR 0.035 SWITCHING CHARACTERISTICS (Notes 3 & 4) Turn−On Delay Time Rise Time Turn−Off Delay Time (VDD = −15 Vdc, ID = −25 A, VGS = −5.0 50V V, RG = 1.3 )) Fall Time Gate Charge (VDS = −24 Vdc, VGS = −5.0 5 0 Vdc Vdc, ID = −25 A)) ns BODY−DRAIN DIODE RATINGS (Note 3) Diode Forward On−Voltage (IS = −25 Adc, VGS = 0 V) (IS = −25 Adc, VGS = 0 V, TJ = 125°C) Reverse Recovery Time (IS = −25 A, VGS = 0 V, dIS/dt = 100 A/s) Reverse Recovery Stored Charge 3. Pulse Test: Pulse Width ≤ 300 s, Duty Cycle ≤ 2%. 4. Switching characteristics are independent of operating junction temperature. http://onsemi.com 2 ns C NTD25P03L TYPICAL MOSFET ELECTRICAL CHARACTERISTICS 50 8V 7V 30 4.5 V 4V 20 3.5 V 10 3V 2.5 V 0 0 1 3 2 TJ = 25°C 40 TJ = 125°C 30 20 10 0 1 2 4 3 5 6 −VDS, DRAIN−TO−SOURCE VOLTAGE (VOLTS) −VGS, GATE−TO−SOURCE VOLTAGE (VOLTS) Figure 1. On−Region Characteristics Figure 2. Transfer Characteristics VGS = −5 V 0.25 0.2 0.15 T = 125°C 0.1 T = 25°C 0.05 T = −40°C 0 TJ = −40°C VDS ≥ −5 V 5 4 0.3 0 10 5 15 20 25 30 35 40 45 50 0.01 TJ = 25°C 0.075 VGS = −5 V 0.05 VGS = −10 V 0.025 0 0 5 10 15 20 25 30 35 40 45 50 −ID, DRAIN CURRENT (AMPS) −ID, DRAIN CURRENT (AMPS) Figure 3. On−Resistance versus Drain Current and Temperature Figure 4. On−Resistance versus Drain Current and Gate Voltage 10,000 1.6 1.4 VGS = 0 V ID = −12.5 VGS = −5 V −IDSS, LEAKAGE (nA) RDS(on), DRAIN−TO−SOURCE RESISTANCE (NORMALIZED) RDS(on), DRAIN−TO−SOURCE RESISTANCE () −ID, DRAIN CURRENT (AMPS) 5V 6V RDS(on), DRAIN−TO−SOURCE RESISTANCE () −ID, DRAIN CURRENT (AMPS) 9V 40 50 TJ = 25°C VGS = 10 V 1.2 1 TJ = 150°C 1000 TJ = 125°C 100 0.8 0.6 −50 10 −25 0 25 50 75 100 125 150 0 5 10 15 20 25 TJ, JUNCTION TEMPERATURE (°C) −VDS, DRAIN−TO−SOURCE VOLTAGE (VOLTS) Figure 5. On−Resistance Variation with Temperature Figure 6. Drain−to−Source Leakage Current versus Voltage http://onsemi.com 3 30 NTD25P03L POWER MOSFET SWITCHING Switching behavior is most easily modeled and predicted by recognizing that the power MOSFET is charge controlled. The lengths of various switching intervals (t) are determined by how fast the FET input capacitance can be charged by current from the generator. The published capacitance data is difficult to use for calculating rise and fall because drain−gate capacitance varies greatly with applied voltage. Accordingly, gate charge data is used. In most cases, a satisfactory estimate of average input current (IG(AV)) can be made from a rudimentary analysis of the drive circuit so that t = Q/IG(AV) The capacitance (Ciss) is read from the capacitance curve at a voltage corresponding to the off−state condition when calculating td(on) and is read at a voltage corresponding to the on−state when calculating td(off). At high switching speeds, parasitic circuit elements complicate the analysis. The inductance of the MOSFET source lead, inside the package and in the circuit wiring which is common to both the drain and gate current paths, produces a voltage at the source which reduces the gate drive current. The voltage is determined by Ldi/dt, but since di/dt is a function of drain current, the mathematical solution is complex. The MOSFET output capacitance also complicates the mathematics. And finally, MOSFETs have finite internal gate resistance which effectively adds to the resistance of the driving source, but the internal resistance is difficult to measure and, consequently, is not specified. The resistive switching time variation versus gate resistance (Figure 9) shows how typical switching performance is affected by the parasitic circuit elements. If the parasitics were not present, the slope of the curves would maintain a value of unity regardless of the switching speed. The circuit used to obtain the data is constructed to minimize common inductance in the drain and gate circuit loops and is believed readily achievable with board mounted components. Most power electronic loads are inductive; the data in the figure is taken with a resistive load, which approximates an optimally snubbed inductive load. Power MOSFETs may be safely operated into an inductive load; however, snubbing reduces switching losses. During the rise and fall time interval when switching a resistive load, VGS remains virtually constant at a level known as the plateau voltage, VSGP. Therefore, rise and fall times may be approximated by the following: tr = Q2 x RG/(VGG − VGSP) tf = Q2 x RG/VGSP where VGG = the gate drive voltage, which varies from zero to VGG RG = the gate drive resistance and Q2 and VGSP are read from the gate charge curve. During the turn−on and turn−off delay times, gate current is not constant. The simplest calculation uses appropriate values from the capacitance curves in a standard equation for voltage change in an RC network. The equations are: td(on) = RG Ciss In [VGG/(VGG − VGSP)] td(off) = RG Ciss In (VGG/VGSP) 2200 Ciss C, CAPACITANCE (pF) 2000 TJ = 25°C 1800 1600 1400 1200 Crss Ciss 1000 800 600 Coss 400 200 0 VDS = 0 V 10 Crss VGS = 0 V 5 0 5 10 15 20 −VGS −VDS GATE−TO−SOURCE OR DRAIN−TO−SOURCE VOLTAGE (VOLTS) Figure 7. Capacitance Variation http://onsemi.com 4 25 QT −VDS 8 25 20 6 −VGS Q2 Q1 4 15 10 2 0 ID = −25 A TJ = 25°C 5 Q3 0 2.5 0 5 7.5 10 12.5 15 Qg, TOTAL GATE CHARGE (nC) 1000 VDD = −15 V ID = −25 A VGS = −5.0 V TJ = 25°C t, TIME (ns) 30 10 −VDS, DRAIN−TO−SOURCE VOLTAGE (VOLTS) −VGS, GATE−TO−SOURCE VOLTAGE (VOLTS) NTD25P03L tr 100 tf td(off) td(on) 10 1 1 10 100 RG, GATE RESISTANCE () Figure 8. Gate−to−Source and Drain−to−Source Voltage versus Total Charge Figure 9. Resistive Switching Time Variation versus Gate Resistance DRAIN−TO−SOURCE DIODE CHARACTERISTICS high di/dts. The diode’s negative di/dt during ta is directly controlled by the device clearing the stored charge. However, the positive di/dt during tb is an uncontrollable diode characteristic and is usually the culprit that induces current ringing. Therefore, when comparing diodes, the ratio of tb/ta serves as a good indicator of recovery abruptness and thus gives a comparative estimate of probable noise generated. A ratio of 1 is considered ideal and values less than 0.5 are considered snappy. Compared to ON Semiconductor standard cell density low voltage MOSFETs, high cell density MOSFET diodes are faster (shorter trr), have less stored charge and a softer reverse recovery characteristic. The softness advantage of the high cell density diode means they can be forced through reverse recovery at a higher di/dt than a standard cell MOSFET diode without increasing the current ringing or the noise generated. In addition, power dissipation incurred from switching the diode will be less due to the shorter recovery time and lower switching losses. The switching characteristics of a MOSFET body diode are very important in systems using it as a freewheeling or commutating diode. Of particular interest are the reverse recovery characteristics which play a major role in determining switching losses, radiated noise, EMI and RFI. System switching losses are largely due to the nature of the body diode itself. The body diode is a minority carrier device, therefore it has a finite reverse recovery time, trr, due to the storage of minority carrier charge, QRR, as shown in the typical reverse recovery wave form of Figure 14. It is this stored charge that, when cleared from the diode, passes through a potential and defines an energy loss. Obviously, repeatedly forcing the diode through reverse recovery further increases switching losses. Therefore, one would like a diode with short trr and low QRR specifications to minimize these losses. The abruptness of diode reverse recovery effects the amount of radiated noise, voltage spikes, and current ringing. The mechanisms at work are finite irremovable circuit parasitic inductances and capacitances acted upon by −IS, SOURCE CURRENT (AMPS) 25 VGS = 0 V TJ = 25°C 20 15 10 5 0 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 −VSD, SOURCE−TO−DRAIN VOLTAGE (VOLTS) 1.1 Figure 10. Diode Forward Voltage versus Current http://onsemi.com 5 NTD25P03L SAFE OPERATING AREA The Forward Biased Safe Operating Area curves define the maximum simultaneous drain−to−source voltage and drain current that a transistor can handle safely when it is forward biased. Curves are based upon maximum peak junction temperature and a case temperature (TC) of 25°C. Peak repetitive pulsed power limits are determined by using the thermal response data in conjunction with the procedures discussed in AN569, “Transient Thermal Resistance − General Data and Its Use.” Switching between the off−state and the on−state may traverse any load line provided neither rated peak current (IDM) nor rated voltage (VDSS) is exceeded, and that the transition time (tr, tf) does not exceed 10 s. In addition the total power averaged over a complete switching cycle must not exceed (TJ(MAX) − TC)/(RJC). A power MOSFET designated E−FET can be safely used in switching circuits with unclamped inductive loads. For VGS = −20 V SINGLE PULSE TC = 25°C 100 s 10 1 ms 10 ms dc 1 RDS(on) LIMIT THERMAL LIMIT PACKAGE LIMIT 0.1 0.1 1 10 100 EAS, SINGLE PULSE DRAIN−TO−SOURCE AVALANCHE ENERGY (mJ) −ID, DRAIN CURRENT (AMPS) 100 reliable operation, the stored energy from circuit inductance dissipated in the transistor while in avalanche must be less than the rated limit and must be adjusted for operating conditions differing from those specified. Although industry practice is to rate in terms of energy, avalanche energy capability is not a constant. The energy rating decreases non−linearly with an increase of peak current in avalanche and peak junction temperature. Although many E−FETs can withstand the stress of drain−to−source avalanche at currents up to rated pulsed current (IDM), the energy rating is specified at rated continuous current (ID), in accordance with industry custom. The energy rating must be derated for temperature as shown in the accompanying graph (Figure 12). Maximum energy at currents below rated continuous ID can safely be assumed to equal the values indicated. 200 180 ID = −20 A 160 140 120 100 80 60 40 20 0 25 50 75 100 125 150 −VDS, DRAIN−TO−SOURCE VOLTAGE (VOLTS) TJ, STARTING JUNCTION TEMPERATURE (°C) Figure 11. Maximum Rated Forward Biased Safe Operating Area Figure 12. Maximum Avalanche Energy versus Starting Junction Temperature http://onsemi.com 6 NTD25P03L r(t), EFFECTIVE TRANSIENT THERMAL RESISTANCE (NORMALIZED) TYPICAL ELECTRICAL CHARACTERISTICS 1 D = 0.5 0.2 0.1 0.1 P(pk) 0.05 RJC(t) = r(t) RJC D CURVES APPLY FOR POWER PULSE TRAIN SHOWN READ TIME AT t1 TJ(pk) − TC = P(pk) RJC(t) 0.02 0.01 t1 t2 DUTY CYCLE, D = t1/t2 SINGLE PULSE 0.01 1.0E−05 1.0E−04 1.0E−03 1.0E−02 1.0E−01 t, TIME (s) Figure 13. Thermal Response di/dt IS trr ta tb TIME 0.25 IS tp IS Figure 14. Diode Reverse Recovery Waveform http://onsemi.com 7 1.0E+00 1.0E+01 NTD25P03L PACKAGE DIMENSIONS DPAK CASE 369C−01 ISSUE O −T− NOTES: 1. DIMENSIONING AND TOLERANCING PER ANSI Y14.5M, 1982. 2. CONTROLLING DIMENSION: INCH. C B V SEATING PLANE E R 4 Z A S 1 2 DIM A B C D E F G H J K L R S U V Z 3 U K F J L H D G 2 PL 0.13 (0.005) M T INCHES MIN MAX 0.235 0.245 0.250 0.265 0.086 0.094 0.027 0.035 0.018 0.023 0.037 0.045 0.180 BSC 0.034 0.040 0.018 0.023 0.102 0.114 0.090 BSC 0.180 0.215 0.025 0.040 0.020 −−− 0.035 0.050 0.155 −−− STYLE 2: PIN 1. GATE 2. DRAIN 3. SOURCE 4. DRAIN SOLDERING FOOTPRINT* 6.20 0.244 3.0 0.118 2.58 0.101 5.80 0.228 1.6 0.063 6.172 0.243 SCALE 3:1 mm inches *For additional information on our Pb−Free strategy and soldering details, please download the ON Semiconductor Soldering and Mounting Techniques Reference Manual, SOLDERRM/D. http://onsemi.com 8 MILLIMETERS MIN MAX 5.97 6.22 6.35 6.73 2.19 2.38 0.69 0.88 0.46 0.58 0.94 1.14 4.58 BSC 0.87 1.01 0.46 0.58 2.60 2.89 2.29 BSC 4.57 5.45 0.63 1.01 0.51 −−− 0.89 1.27 3.93 −−− NTD25P03L PACKAGE DIMENSIONS DPAK CASE 369D−01 ISSUE O C B V NOTES: 1. DIMENSIONING AND TOLERANCING PER ANSI Y14.5M, 1982. 2. CONTROLLING DIMENSION: INCH. E R 4 Z A S 1 2 3 −T− SEATING PLANE K J F H D G 3 PL 0.13 (0.005) M DIM A B C D E F G H J K R S V Z INCHES MIN MAX 0.235 0.245 0.250 0.265 0.086 0.094 0.027 0.035 0.018 0.023 0.037 0.045 0.090 BSC 0.034 0.040 0.018 0.023 0.350 0.380 0.180 0.215 0.025 0.040 0.035 0.050 0.155 −−− STYLE 2: PIN 1. GATE 2. DRAIN 3. SOURCE 4. DRAIN T http://onsemi.com 9 MILLIMETERS MIN MAX 5.97 6.35 6.35 6.73 2.19 2.38 0.69 0.88 0.46 0.58 0.94 1.14 2.29 BSC 0.87 1.01 0.46 0.58 8.89 9.65 4.45 5.45 0.63 1.01 0.89 1.27 3.93 −−− NTD25P03L ON Semiconductor and are registered trademarks of Semiconductor Components Industries, LLC (SCILLC). SCILLC reserves the right to make changes without further notice to any products herein. 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