DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 1.2-A HIGH-EFFICIENCY PWM POWER DRIVER FEATURES D 1.22-A DC (82% Duty Cycle) Output Current D D D D D D DESCRIPTION The DRV590 is a high-efficiency power amplifier ideal for driving a wide variety of thermoelectric cooler elements in systems powered from 2.7 V to 5.5 V. PWM operation and low output stage on-resistance significantly decrease power dissipation in the amplifier. (TJ ≤ 89°C) 1-A DC (100% Duty Cycle) Output Current (TJ ≤ 89°C) Low Supply Voltage Operation from 2.7 V to 5.5 V High Efficiency Generates Less Heat Over-Temperature Protection Short-Circuit Protection PowerPADt SOIC and 4 × 4 mm MicroStar Junior Packages The DRV590 is internally protected against over temperature conditions and current overloads due to short circuits. The over temperature protection activates at a junction temperature of 190°C and will deactivate once the temperature is less than 130°C. If the overcurrent circuitry is tripped, the amplifier will automatically reset after 3–5 ms. APPLICATIONS D Thermoelectric Cooler (TEC) Driver D Laser Diode Biasing J5 IN– (VCOM) The gain of the DRV590 is controlled by two input terminals, GAIN1 and GAIN0. The amplifier may be configured for a gain of 6, 12, 18, and 23.5 dB. J4 IN+ C4 1 µF R1 1 kΩ J1 R2 1 kΩ R3 120 kΩ J8 VDD R4 120 kΩ J2 R5 120 kΩ C3 1 µF J3 NC IN+ IN– SHUTDOWN GAIN0 GAIN1 PVDD OUT+ NC PGND L1 10 µH J7 OUT+ C5 10 µF C6 10 µF C9 220 pF NC AREF AGND COSC ROSC VDD PVDD OUT– NC PGND R6 120 kΩ J8 VDD C1 1 µF C2 1 µF C8 10 µF J9 GND L2 10 µH C7 10 µF J6 OUT– Typical Circuit Schematic for Driving a Thermoelectric Cooler Element Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet. PowerPAD and MicroStar Junior are trademarks of Texas Instruments. Copyright 2002, Texas Instruments Incorporated This document contains information on products in more than one phase of development. The status of each device is indicated on the page(s) specifying its electrical characteristics. www.ti.com 1 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 AVAILABLE OPTIONS PACKAGED DEVICES TA SOIC (DWP)† GQC‡ – 40°C to 85°C DRV590DWP DRV590GQCR † The PW package is available taped and reeled. To order a taped and reeled part, add the suffix R to the part number (e.g., DRV590PWR). ‡ The GQC package is only available taped and reeled. MicroStar Juniort (GQC) Package (TOP VIEW) DWP PACKAGE (TOP VIEW) IN+ NC IN+ IN– SHUTDOWN GAIN0 GAIN1 PVDD OUT+ NC PGND 1 2 3 4 5 6 7 8 9 10 20 19 18 17 16 15 14 13 12 11 NC AREF AGND COSC ROSC VDD PVDD OUT– NC PGND NC – No internal connection IN– SHUTDOWN GAIN0 GAIN1 PVDD PVDD OUT+ A2 AGND AREF A6 A1 B1 A7 B7 NC C1 C7 D1 D7 E1 F1 E7 F7 G1 G7 COSC ROSC VDD PVDD PVDD OUT– PGND (SIDE VIEW) NC – No internal connection NOTE: The shaded terminals are used for thermal connections to the ground plane. Terminal Functions TERMINAL NAME I/O DESCRIPTION GQC NO. DWP NO. AGND A3–A5, B2–B6 C2–C6, D2–D4 18 I Analog ground AREF A6 19 O Connect capacitor to ground for AREF voltage filtering (1 µF). COSC B7 17 I Connect capacitor to ground to set oscillation frequency (220 pF). GAIN0 C1 5 I Bit 0 of gain control (TTL logic level) GAIN1 D1 6 I Bit 1 of gain control (TTL logic level) IN– A1 3 I Negative differential input IN+ A2 2 I Positive differential input NC A7 1, 9, 12, 20 OUT– G7 13 O Negative BTL output OUT+ G1 8 O Positive BTL output PGND D5–D6, E2–E6 F2–F6, G2–G6 10, 11 I High-current grounds (2) E1, E7, F1, F7 7, 14 I High-current power supplies (2) C7 16 I Connect resistor to ground to set oscillation frequency (120 kΩ). SHUTDOWN B1 4 I Places the amplifier in shutdown mode if a TTL logic low is placed on this terminal, and normal operation if a TTL logic high is placed on this terminal. VDD D7 15 I Analog power supply PVDD ROSC 2 Not connected www.ti.com DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 absolute maximum ratings over operating free-air temperature range (unless otherwise noted)‡ Supply voltage, VDD, PVDD . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . –0.3 V to 5.5 V Input voltage, VI . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . –0.3 V to VDD + 0.3 V Continuous total power dissipation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . See Dissipation Rating Table Operating free-air temperature range, TA . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 40°C to 85°C Operating junction temperature range, TJ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 40°C to 150°C Storage temperature range, Tstg . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . –65°C to 150°C Lead temperature 1,6 mm (1/16 inch) from case for 10 seconds . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 260°C ‡ Stresses beyond those listed under “absolute maximum ratings” may cause permanent damage to the device. These are stress ratings only, and functional operation of the device at these or any other conditions beyond those indicated under “recommended operating conditions” is not implied. Exposure to absolute-maximum-rated conditions for extended periods may affect device reliability. DISSIPATION RATING TABLE TA ≤ 25°C 2.61 W DERATING FACTOR GQC 20.9 mW/°C TA = 70°C 1.67 W TA = 85°C 1.36 W DWP 3.66 W 29.3 mW/°C 2.34 W 1.9 W PACKAGE recommended operating conditions ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ Supply voltage, VDD, PVDD High-level input voltage, VIH GAIN0, GAIN1, SHUTDOWN Low-level input voltage, VIL GAIN0, GAIN1, SHUTDOWN MIN MAX 2.7 5.5 2 Operating free-air temperature, TA – 40 Load impedance UNIT V V 0.7 V 85 °C Ω 1 electrical characteristics at specified free-air temperature, TA = 25°C (unless otherwise noted) ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁ ÁÁÁÁÁÁÁÁÁ ÁÁÁ ÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁ ÁÁÁÁ ÁÁÁÁÁÁÁÁ PARAMETER |VOS| Output offset voltage (measured differentially) PSRR Power supply rejection ratio |IIH| High-level input current |IIL| Low-level input current IDD IDD(SD) Supply current, no filter TEST CONDITIONS VI = 0 V, TYP AV = any gain mV dB 61 1 µA 1 µA 4.5 6.5 mA 0.05 5 µA GAIN0 = low, GAIN1 = low 5.1 6 6.5 GAIN0 = high, GAIN1 = low 11 12 12.5 GAIN0 = low, GAIN1 = high 17 18 19 GAIN0 = high, GAIN1 = high 23 23.5 24 Single ended UNIT 77 GAIN0, GAIN1, SHUTDOWN = 0 V Differential MAX 25 VI = 3.3 V VI = 0 V Supply current, shutdown mode Switching frequency MIN PVDD = 4.9 V to 5.1 V PVDD = 3.2 V to 3.4 V Gain fs ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁ ÁÁÁÁÁÁ ÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁ ÁÁÁ ÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁ dB 250 Rosc = 120 kΩ, kΩ Cosc = 220 pF www.ti.com 500 kHz 3 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 operating characteristics, TA = 25°C, RL = 2 Ω, gain = 6 dB (unless otherwise noted) ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ ÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁÁ PARAMETER TEST CONDITIONS IO PSRR Maximum output current Duty cycle = 82% Power supply rejection ratio f = 1 kHz, ZI Input impedance VICR Common mode input voltage range Common-mode PVDD = 5 V PVDD = 3.3 V rds(on) Output on-resistance on resistance PVDD = 5 V PVDD = 3.3 V η Efficiency PVDD = 5 V PVDD = 3.3 V Vn Integrated noise floor f = 10 Hz to 5 kHz, Gain = 6 dB MIN TYP MAX 1.22 C(AREF) = 1 µF UNIT A 70 dB >15 kΩ 1.2 3.8 1.2 2.1 0.5 0.65 V Ω 64% 60% 23 µV rms functional block diagram VDD AGND VDD PVDD Gain Adjust IN– _ + _ Deglitch Logic Gate Drive OUT– + _ + Gain Adjust IN+ PGND + _ PVDD + _ _ + Deglitch Logic Gate Drive OUT+ PGND SHUTDOWN SD GAIN1 GAIN0 2 Gain Biases and References Ramp Generator COSC ROSC AREF 4 Start-Up Protection Logic Thermal www.ti.com VDD ok OC Detect DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 TYPICAL CHARACTERISTICS Table of Graphs FIGURE Gain and phase vs Frequency Efficiency vs Load resistance 1 PSRR Power supply rejection ratio vs Frequency rds(on) Small signal drain-source drain source on-state on state resistance Small-signal IO Maximum output current 2, 3 4 vs Supply voltage 5, 6 vs Ambient temperature 7, 8 vs Differential output voltage 9 GAIN AND PHASE vs FREQUENCY 100 10 72 8 Gain 44 6 16 4 2 –12 0 –40 –2 –68 –4 –6 –8 –10 10 Phase – ° Gain – dBV Phase –96 VI = 1.17 Vrms VDD = 5 V RL = 2 Ω 100 –124 –152 1k 10k f – Frequency – Hz –180 100k Figure 1 www.ti.com 5 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 TYPICAL CHARACTERISTICS EFFICIENCY vs LOAD RESISTANCE EFFICIENCY vs LOAD RESISTANCE 90 90 VDD = 3.3 V 85 VDD = 5 V PO = 2 W 85 PO = 0.25 W 80 PO = 1 W Efficiency – % Efficiency – % 80 75 PO = 0.5 W 70 65 PO = 0.5 W 75 70 60 65 55 50 60 2 3 4 5 6 7 8 9 2 10 3 RL – Load Resistance – Ω 4 POWER SUPPLY REJECTION RATIO vs FREQUENCY PSRR – Power Supply Rejection Ratio – dB –40 –45 –50 –55 –60 –65 –70 –75 –80 10 100 f – Frequency – Hz 1k 10k Figure 4 6 6 7 8 9 10 Figure 3 rds(on) – Small-Signal Drain-Source On-State Resistance – Ω Figure 2 1 5 RL – Load Resistance – Ω SMALL-SIGNAL DRAIN-SOURCE ON-STATE RESISTANCE vs SUPPLY VOLTAGE 0.8 IO = 0.5 A 0.7 0.6 rds(on) Low Side 0.5 0.4 0.3 2.7 rds(on) High Side 3.1 3.5 3.9 Figure 5 www.ti.com 4.3 4.7 VDD – Supply Voltage – V 5.1 5.5 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 SMALL-SIGNAL DRAIN-SOURCE ON-STATE RESISTANCE vs SUPPLY VOLTAGE 0.9 IO = 1 A 0.8 0.7 0.6 rds(on) Low Side 0.5 rds(on) High Side 0.4 0.3 2.7 3.1 3.5 3.9 4.3 4.7 5.1 5.5 rds(on) – Small-Signal Drain-Source On-State Resistance – Ω rds(on) – Small-Signal Drain-Source On-State Resistance – Ω TYPICAL CHARACTERISTICS SMALL-SIGNAL DRAIN-SOURCE ON-STATE RESISTANCE vs AMBIENT TEMPERATURE 0.62 IO = 0.5 A VDD = 5 V DWP Package 0.58 rds(on) Low Side 0.54 0.50 0.46 rds(on) High Side 0.42 0.38 25 35 45 VDD – Supply Voltage – V Figure 6 65 75 85 Figure 7 SMALL-SIGNAL DRAIN-SOURCE ON-STATE RESISTANCE vs AMBIENT TEMPERATURE MAXIMUM OUTPUT CURRENT vs DIFFERENTIAL OUTPUT VOLTAGE 1.4 0.62 VDD = 5 V IO = 1 A VDD = 3.3 V DWP Package 0.58 rds(on) Low Side 0.54 0.50 0.46 rds(on) High Side 0.42 0.38 25 35 45 TJ = 89°C 1.2 IO – Maximum Output Current – A rds(on) – Small-Signal Drain-Source On-State Resistance – Ω 55 TA – Ambient Temperature – °C 55 65 75 85 TA – Ambient Temperature – °C 1.0 TJ = 102°C 0.8 0.6 TJ = 124°C 0.4 0.2 0.0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 VOD – Differential Output Voltage – V Figure 8 Figure 9 www.ti.com 7 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 APPLICATION INFORMATION driving TEC elements Below is a typical application schematic. J5 IN– (VCOM) J4 IN+ C4 1 µF R1 1 kΩ J1 R2 1 kΩ R3 120 kΩ J8 VDD R4 120 kΩ J2 R5 120 kΩ C3 1 µF J3 NC IN+ IN– SHUTDOWN GAIN0 GAIN1 PVDD OUT+ NC PGND L1 10 µH J7 OUT+ C5 10 µF C6 10 µF C9 220 pF NC AREF AGND COSC ROSC VDD PVDD OUT– NC PGND R6 120 kΩ J8 VDD C1 1 µF C2 1 µF C8 10 µF J9 GND L2 10 µH C7 10 µF J6 OUT– output filter considerations TEC element manufacturers provide electrical specifications for maximum dc current and maximum output voltage for each particular element. The maximum ripple current, however, is typically only recommended to be less than 10%. The maximum temperature differential across the element decreases as ripple current increases and can be calculated using equation 1. DT + ( 1 ) N 2) 1 (1) DT max ∆T = actual temperature differential ∆Tmax = maximum temperature differential (specified by manufacturer) N = ratio of ripple current to dc current According to this relationship, a 10% ripple current reduces the maximum temperature differential by 1%. A LC network may be used to filter the current flowing to the TEC to reduce the amount of ripple and, more importantly, protect the rest of the system from any electromagnetic interference (EMI). 8 www.ti.com DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 APPLICATION INFORMATION driving TEC elements (continued) filter component selection The LC filter may be designed from a couple of different perspectives, both of which may help estimate the overall performance of the system. The filter should be designed for the worst-case conditions during operation, which is typically when the differential output is at 50% duty cycle. The following section serves as a starting point for the design, and any calculations should be confirmed with a prototype circuit. To simplify the design, half-circuit analysis may also be used. This should only be done if the TEC element is close to the output of the filter. Any filter should always be placed as close to the DRV590 as possible to reduce EMI. L OUT+ C C TEC R L OUT+ or OUT– OUT– L 2C C TEC R 2 C Figure 10. LC Output Filter Figure 11. LC Half-Circuit Equivalent LC filter in the frequency domain The transfer function for the second order low-pass filter in Figure 10 and Figure 11 is shown in equation 2. H (jw) + LP (2) 1 ǒ Ǔ ) Q1 wjw0 ) 1 – ww 0 2 1 ǸL 3C Q = quality factor ω = DRV590 differential switching frequency w0 + For the DRV590, the differential output switching frequency is 500 kHz. The resonant frequency for the filter should be chosen to be at least one order of magnitude lower than the switching frequency. Equation 2 may then be simplified to give the following magnitude equation 3. These equations assume the use of the filter in Figure 10, which effectively triples the capacitance. ǒǓ ŤHLPŤdB + –40 log fo + (3) fs fo 1 Ǹ 2p L 3C fs = 500 kHz (DRV590 differential switching frequency) www.ti.com 9 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 APPLICATION INFORMATION LC filter in the frequency domain (continued) If L = 10 µH and C = 10 µF, the resonant frequency is 9.2 kHz, which corresponds to –69 dB of attenuation at the 500-kHz switching frequency. For VDD = 5 V, the amount of ripple voltage at the TEC element will be approximately 1.7 mV. The average TEC element has a resistance of 1.5 Ω, so the ripple current through the TEC is approximately 1.13 mA. At the 1-A maximum output current of the DRV590, this 1.13 mA corresponds to 0.113% ripple current, causing less than 0.0001% reduction of the maximum temperature differential of the TEC element (see equation 1). LC filter in the time domain The ripple current of an inductor can be calculated using equation 4. DI + L ǒVDD * VTECǓDTs (4) L D = duty cycle (0.5 worst case) Ts = 1/fs = 1/500 kHz For VDD = 5 V, VTEC = 2.5 V, and L = 10 µH, the inductor ripple current is 250 mA. To calculate how much of that ripple current will flow through the TEC element, however, the properties of the filter capacitor must be considered. For relatively small capacitors (less than 10 µF) with very low equivalent series resistance (ESR, less than 10 mΩ), such as ceramic capacitors, equation 5 may be used to estimate the ripple voltage on the capacitor due to the change in charge. ǒǓ f 2 DV + p (1–D) o C 2 fs (5) 2 V TEC D = duty cycle fs = 500 kHz 1 fo + 2p ǸL 3C For L = 10 µH and C = 10 µF, the cutoff frequency fo = 9.2 kHz. For a worst case duty cycle of 0.5 and VTEC = 2.5, the ripple voltage on the capacitors is 2 mV. The ripple current may be simply calculated by dividing the ripple voltage by the TEC resistance of 1.5 Ω, resulting in a ripple current through the TEC element of 1.33 mA. Note that this is similar to the value calculated using the frequency domain approach. For larger capacitors (greater than 10 µF) with relatively high ESR (greater than 100 mΩ), such as electrolytic capacitors, the ESR drop dominates over the charging-discharging of the capacitor. Equation 6 can be used to estimate the ripple voltage. DV C + DI L R (6) ESR ∆L = inductor ripple current RESR = filter capacitor ESR For a 100-µF electrolytic capacitor, an ESR of 0.1 Ω is common. If the 10-µH inductor is used, delivering 250 mA of ripple current to the capacitor (as calculated above), then the ripple voltage is 25 mV. This is over ten times that of the 10-µF ceramic capacitor, as ceramic capacitors typically have negligible ESR. 10 www.ti.com DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 APPLICATION INFORMATION LC filter in the time domain (continued) For worst case conditions, the on-resistance of the output transistors has been ignored to give the maximum theoretical ripple current. In reality, the voltage drop across the output transistors will decrease the maximum VO as the output current increases. It can be shown using equation 4 that this will decrease the inductor ripple current, and therefore the TEC ripple current. general operation oscillator components ROSC and COSC The onboard ramp generator requires an external resistor and capacitor to set the oscillation frequency. For proper operation, the resistor ROSC should be 120 kΩ with 1% tolerance. The capacitor COSC should be a ceramic 220 pF with 10% tolerance. Both components should be grounded to AGND, which should be connected to PGND at a single point, typically where the power and ground physically connect to the printed circuit board. AREF capacitor The AREF terminal is the output of an internal mid-rail voltage regulator used for the on-board oscillator and ramp generator. The regulator may not be used to provide power to any additional circuitry. A 1-µF ceramic capacitor must be connected from AREF to AGND for stability (see the oscillator components ROSC and COSC section for AGND connection information). gain settings The differential output voltage may be calculated using equation 7. V O +V ǒ Ǔ –V –V + Av V IN) IN– OUT) OUT– (7) Av is the voltage gain, which may be selected by configuring GAIN0 and GAIN1 according to the table below. The input resistance also varies with the gain setting, as shown by the typical values in Table 1. Though these values may vary by up to 30% due to process variations, the gain settings themselves vary little, as they are determined by resistor ratios. Table 1. Gain Settings GAIN0 GAIN1 AMPLIFIER GAIN (dB, TYPICAL) INPUT RESISTANCE (kΩ, TYPICAL) 0 0 0 6 104 1 12 74 1 1 0 18 44 1 23.5 24 www.ti.com 11 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 APPLICATION INFORMATION general operation (continued) input configuration—differential and single-ended If a differential input is used, it should be biased around the mid-rail of the DRV590 and must not exceed the common-mode input range of the input stage (see the operating characteristics at the beginning of the data sheet). The most common configuration employs a single-ended input. The unused input should be tied to the mid-rail, which may be simply accomplished with a resistive voltage divider. For the best performance, the resistor values chosen should be at least an order of magnitude lower than the input resistance of the DRV590 at the selected gain setting. This prevents the bias voltage at the unused input from shifting when the signal input is applied. A small ceramic capacitor should also be placed from the input to ground to filter noise and keep the voltage stable. power supply decoupling To reduce the effects of high-frequency transients or spikes, a small ceramic capacitor, typically 0.1 µF to 1 µF, should be placed as close to each PVDD pin of the DRV590 as possible. For bulk decoupling, a 10-µF to 100-µF tantalum or aluminum electrolytic capacitor should be placed relatively close to the DRV590. SHUTDOWN operation The DRV590 includes a shutdown mode that disables the outputs and places the device in a low supply current state. The SHUTDOWN pin may be controlled with a TTL logic signal. When SHUTDOWN is held high, the device operates normally. When SHUTDOWN is held low, the device is placed in shutdown. The SHUTDOWN pin must not be left floating. If the shutdown feature is unused, the pin may simply be connected to VDD. power dissipation and maximum ambient temperature Though the DRV590 is much more efficient than traditional linear solutions, the IR drop across the on-resistance of the output transistors generates some heat in the package, which may be calculated using equation 8. P DISS ǒ OUTǓ + I 2 r ds(on), total (8) For example, at the maximum output current of 1.2 A through a total on-resistance of 1 Ω, the power dissipated in the package is 1.44 W. The maximum ambient temperature can be calculated using equation 9. ǒ T +T q A J JA P Ǔ DISS (9) Continuing the example above, the maximum ambient temperature driving 1.2 A without exceeding 89°C junction temperature for a DRV590 in the DWP package (see the maximum output current vs duty cycle section) is 39°C. maximum output current vs duty cycle At 100% duty cycle across the load, the reliability of the DRV590 is degraded if more than 1 A is driven through the outputs. Furthermore, the junction temperature must not exceed 89°C at the maximum output current levels to prevent further degradation. However, as the duty cycle across the load decreases, the maximum allowable output current increases. Table 2 shows the typical maximum output current, voltage across the load, and junction temperature versus duty cycle. The dissipation and junction temperatures were calculated using equations 8 and 9. The total on-resistance was assumed to be 1 Ω, the ambient temperature to be 25°C, and the θJA to be 34.1°C/W. 12 www.ti.com DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 APPLICATION INFORMATION maximum output current vs duty cycle (continued) Table 2. Typical Maximum Output Specifications vs Duty Cycle (VDD = 5 V) DUTY CYCLE MAX IO (A) MAX VLOAD (V) 100% 1 4 PDISS (W) 1 TJ (°C) 67.6 95% 1.05 90% 1.11 3.69 1.11 72.2 3.38 1.24 77.6 85% 84% 1.17 3.07 1.39 83.9 1.19 3.01 1.42 85.3 83% 1.2 2.94 1.45 86.8 82% 1.22 2.88 1.49 88.3 At duty cycles less than 82%, the power dissipated from the theoretical maximum current flowing through the on-resistance causes the junction temperature to exceed 89°C. See Figure 9 for more details. www.ti.com 13 DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 MECHANICAL DATA DWP (R-PDSO-G20) PowerPad PLASTIC SMALL-OUTLINE PACKAGE 0.020 (0,51) 0.014 (0,35) 0.050 (1,27) 20 0.010 (0,25) M 11 Thermal Pad 0.150 (3,81) 0.170 (4,31) NOM (see Note C) 0.299 (7,59) 0.293 (7,45) 0.430 (10,92) 0.411 (10,44) 0.010 (0,25) NOM 1 10 0.510 (12,95) 0.500 (12,70) Gage Plane 0.010 (0,25) +2°–ā8° 0.050 (1,27) 0.016 (0,40) Seating Plane 0.096 (2,43) MAX 0.004 (0,10) 0.000 (0,00) 0.004 (0,10) 4073226/B 01/96 NOTES: A. All linear dimensions are in inches (millimeters). B. This drawing is subject to change without notice. C. The thermal performance may be enhanced by bonding the thermal pad to an external thermal plane. This solderable pad is electrically and thermally connected to the backside of the die and leads 1, 10, 11 and 20. PowerPad is a trademark of Texas Instruments. 14 www.ti.com DRV590 SLOS365A – AUGUST 2001 – REVISED AUGUST 2002 MECHANICAL DATA GQC (S-PBGA-N48) PLASTIC BALL GRID ARRAY 4,10 3,90 SQ 3,00 TYP 0,50 0,50 G F E D C B A 1 2 3 4 5 6 7 (BOTTOM VIEW) 0,68 0,62 1,00 MAX Seating Plane 0,35 0,25 0,05 M 0,08 0,21 0,11 4200460/C 10/00 NOTES: A. B. C. D. All linear dimensions are in millimeters. This drawing is subject to change without notice. MicroStar Junior BGA configuration Falls within JEDEC MO-225 MicroStar Junior BGA is a trademark of Texas Instruments. www.ti.com 15 IMPORTANT NOTICE Texas Instruments Incorporated and its subsidiaries (TI) reserve the right to make corrections, modifications, enhancements, improvements, and other changes to its products and services at any time and to discontinue any product or service without notice. Customers should obtain the latest relevant information before placing orders and should verify that such information is current and complete. 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