LM4652TF

OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 LM4651 & LM4652 Overture™ Audio Power Amplifier 170W Class D Audio Power Amplifier Solution Check for Samples: LM4651, LM4652 FEATURES DESCRIPTION • • • • • • • The IC combination of the LM4651 driver and the LM4652 power MOSFET provides a high efficiency, Class D subwoofer amplifier solution. 1 23 • Conventional Pulse Width Modulation. Externally Controllable Switching Frequency. 50kHz to 200kHz Switching Frequency Range. Integrated Error Amp and Feedback Amp. Turn−on Soft Start and Under Voltage Lockout. Over Modulation Protection (Soft Clipping). Externally Controllable Output Current Limiting and Thermal Shutdown Protection. Self Checking Protection Diagnostic. APPLICATIONS • • • Powered Subwoofers for Home Theater and PC's Car Booster Amplifier Self-powered Speakers KEY SPECIFICATIONS • • • • Output power into 4Ω with < 10% THD. 170W (Typ) THD at 10W, 4Ω, 10 − 500Hz. < 0.3% THD (Typ) Maximum efficiency at 125W 85% (Typ) Standby attenuation. >100dB (Min) The LM4651 is a fully integrated conventional pulse width modulator driver IC. The IC contains short circuit, under voltage, over modulation, and thermal shut down protection circuitry. The LM4651also contains a standby function which shuts down the pulse width modulation minimizing supply current. The LM4652 is a fully integrated H-bridge power MOSFET IC in a TO-220 power package. The LM4652 has a temperature sensor built in to alert the LM4651 when the die temperature of the LM4652 exceeds the threshold. Together, these two IC's form a simple, compact high power audio amplifier solution complete with protection normally seen only in Class AB amplifiers. Few external components and minimal traces between the IC's keep the PCB area small and aids in EMI control. The near rail-to-rail switching amplifier substantially increases the efficiency compared to Class AB amplifiers. This high efficiency solution significantly reduces the heat sink size compared to a Class AB IC of the same power level. This two-chip solution is optimum for powered subwoofers and self powered speakers. 1 2 3 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. Overture is a trademark of dcl_owner. All other trademarks are the property of their respective owners. PRODUCTION DATA information is current as of publication date. Products conform to specifications per the terms of the Texas Instruments standard warranty. Production processing does not necessarily include testing of all parameters. Copyright © 2000–2013, Texas Instruments Incorporated OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Connection Diagram Figure 1. LM4651 Plastic Package - Top View See Package Number N28B (1) Figure 2. LM4652 Plastic Package (1) Isolated TO-220 Package See Package Number NDB0015B or Non-Isolated TO-220 Package See Package Number NDL0015A The LM4652TA package NDL0015A is a non-isolated package, setting the tab of the device and the heat sink at −V potential when the LM4652 is directly mounted to the heat sink using only thermal compound. If a mica washer is used in addition to thermal compound, θCS (case to sink) is increased, but the heat sink will be isolated from −V. These devices have limited built-in ESD protection. The leads should be shorted together or the device placed in conductive foam during storage or handling to prevent electrostatic damage to the MOS gates. 2 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Absolute Maximum Ratings (1) (2) (3) Supply Voltage ± 22V Output Current (LM4652) 10A Power Dissipation (LM4651) (4) 1.5W Power Dissipation (LM4652) (4) 32W (5) LM4652 (pins 2,6,10,11) 500V 2000V ESD Susceptibility (LM4651) (6) LM4652 (pins 2,6,10,11) 100V 200V ESD Susceptibility (LM4651) Junction Temperature (7) 150°C Soldering Information N, NDL and NDB Package (10 seconds) (1) (2) (3) (4) (5) (6) (7) 260°C −40°C to + 150°C Storage Temperature Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is given, however, the typical value is a good indication of device performance. All voltages are measured with respect to the GND pin unless otherwise specified. If Military/Aerospace specified devices are required, please contact the Texas Instruments Sales Office/ Distributors for availability and specifications. For operating at case temperatures above 25°C, the LM4651 must be de−rated based on a 150°C maximum junction temperature and a thermal resistance of θJA = 62 °C/W (junction to ambient), while the LM4652 must be de−rated based on a 150°C maximum junction temperature and a thermal resistance of θJC = 2.0 °C/W (junction to case) for the isolated package (NDB) or a thermal resistance of θJC = 1.0°C/W (junction to case) for the non-isolated package (NDL). Human body model, 100 pF discharged through a 1.5 kΩ resistor. Machine Model, 220pF-240pF discharge through all pins. The operating junction temperature maximum, Tjmax is 150°C. Operating Ratings (1) (2) −40°C ≤ TA ≤ +85°C Temperature Range Supply Voltage |V+| + |V−| Thermal Resistance 22V to 44V LM4651 N Package LM4652 NDB, TO−220 Package LM4652 NDL, TO−220 Package (1) (2) θJA 52°C/W θJC 22°C/W θJA 43°C/W θJC 2.0°C/W θJA 37°C/W θJC 1.0°C/W Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is given, however, the typical value is a good indication of device performance. All voltages are measured with respect to the GND pin unless otherwise specified. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 3 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com System Electrical Characteristics for LM4651 and LM4652 (1) (2) The following specifications apply for +VCC = +20V, −VEE = −20V, f SW = 125kHz, fIN = 100Hz, RL = 4Ω, unless otherwise specified. Typicals apply for TA = 25°C. For specific circuit values, refer to Figure 3 (Typical Audio Application Circuit). LM4651 & LM4652 Symbol Parameter Conditions Typical Limit See (3) ICQ Total Quiescent Power Supply Current VIN = 0V, IO = 0mA RDLY = 0Ω RDLY = 10kΩ ISTBY Standby Current AM Standby Attenuation PO Output Power (Continuous Average) Units (Limits) 237 124 mA mA VPIN13 = 5V, Stby: On 17 mA VPIN13 = 5V, Stby: On >115 dB RL = 4Ω, 1% THD 125 W RL = 4Ω, 10% THD 155 W RL = 8Ω, 1% THD 75 W RL = 8Ω, 10% THD 90 W fSW = 75kHz, RL = 4Ω, 1% THD 135 W fSW = 75kHz, RL = 4Ω, 10% THD 170 W η Efficiency at PO = 5W PO = 5W, RDLY = 5kΩ 55 % η Efficiency (LM4651 & LM4652) PO = 125W, THD = 1% 85 % Power Dissipation (LM4651 + LM4652) PO = 125W, THD = 1% (max) 22 W Pd fSW = 75kHz, PO = 135W, THD = 1% (max) 22 W THD+N Total Harmonic Distortion Plus Noise 10W, 10Hz ≤ fIN ≤ 500Hz, AV = 18dB 10Hz ≤ BW ≤ 80kHz 0.3 % εOUT Output Noise A Weighted, no signal, RL = 4Ω 550 µV A-Wtg, Pout = 125W, RL = 4Ω 92 dB 22kHz BW, Pout = 125W, RL = 4Ω 89 dB 0.07 V 37 dB SNR Signal-to-Noise Ratio VOS Output Offset Voltage VIN = 0V, IO = 0mA, ROFFSET = 0Ω PSRR Power Supply Rejection Ratio RL = 4Ω, 10Hz ≤ BW ≤ 30kHz +VCCAC = −VEEAC = 1VRMS, fAC = 120Hz (1) (2) (3) Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is given, however, the typical value is a good indication of device performance. All voltages are measured with respect to the GND pin unless otherwise specified. Limits are guaranteed to TI's AOQL (Average Outgoing Quality Level). Electrical Characteristics for LM4651 (1) (2) (3) The following specifications apply for +VCC = +20V, −VEE = −20V, fSW = 125kHz, unless otherwise specified. Limits apply for TA = 25°C. For specific circuit values, refer to Figure 3 (Typical Audio Application Circuit). LM4651 & LM4652 Symbol Parameter Conditions Typical Limit See ICQ (1) (2) (3) 4 Total Quiescent Current LM4652 not connected, IO = 0mA, |VCC+| + |VEE-|, RDLY = 0Ω 36 (3) 15 45 Units (Limits) mA (min) mA (max) Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is given, however, the typical value is a good indication of device performance. All voltages are measured with respect to the GND pin unless otherwise specified. Limits are guaranteed to TI's AOQL (Average Outgoing Quality Level). Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Electrical Characteristics for LM4651(1)(2)(3) (continued) The following specifications apply for +VCC = +20V, −VEE = −20V, fSW = 125kHz, unless otherwise specified. Limits apply for TA = 25°C. For specific circuit values, refer to Figure 3 (Typical Audio Application Circuit). LM4651 & LM4652 Symbol Parameter Conditions Typical Limit See (3) VIL Standby Low Input Voltage Not in Standby Mode VIH Standby High Input Voltage In Standby Mode 2.0 ROSC = 15kΩ 65 ROSC = 0Ω 200 Units (Limits) 0.8 V (max) 2.5 V (min) kHz fSW Switching Frequency Range fSWerror 50% Duty Cycle Error ROSC = 4kΩ, fSW = 125kHz 1 Tdead Dead Time RDLY = 0Ω 27 ns TOverMod Over Modulation Protection Time Pulse Width Measured at 50% 310 ns kHz 3 % (max) Electrical Characteristics for LM4652 (1) (2) (3) The following specifications apply for +VCC = +20V, −VEE = −20V, unless otherwise specified. Limits apply for TA = 25°C. For specific circuit values, refer to Figure 3 (Typical Audio Application Circuit). LM4651 & LM4652 Symbol Parameter Conditions Typical Limit See (3) Units (Limits) V(BR)DSS Drain−to−Source Breakdown Voltage VGS = 0 55 V IDSS Drain−to−Source Leakage Current VDS = 44VDC, VGS = 0V 1.0 mA VGSth Gate Threshold Voltage VDS = VGS, ID = 1mADC 0.85 RDS(ON) Static Drain−to−Source On Resistance VGS = 6VDC, ID = 6ADC 200 tr Rise Time VGD = 6VDC, VDS = 40VDC, RGATE = 0Ω 25 ns tf Fall Time VGD = 6VDC, VDS = 40VDC, RGATE = 0Ω 26 ns ID Maximum Saturation Drain Current VGS = 6VDC, VDS = 10VDC 10 (1) (2) (3) V 300 8 mΩ (max) ADC (min) Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is given, however, the typical value is a good indication of device performance. All voltages are measured with respect to the GND pin unless otherwise specified. Limits are guaranteed to TI's AOQL (Average Outgoing Quality Level). Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 5 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Typical Application Figure 3. Typical Application Circuit and Test Circuit LM4651 PIN DESCRIPTIONS 6 Pin No. Symbol 1 OUT1 The reference pin of the power MOSFET output to the gate drive circuitry. Description 2,27 BS1,BS2 The bootstrap pin provides extra bias to drive the upper gates, HG1,HG2. 3 HG1 High−Gate #1 is the gate drive to a top side MOSFET in the H-Bridge. 4 HG2 High−Gate #2 is the gate drive to a top side MOSFET in the H-Bridge. 5,15 GND The ground pin for all analog circuitry. 6 +6VBYP 7 +VCC 8 −6VBYP The internally regulated negative voltage output for analog circuitry. This pin is available for internal regulator bypassing only. 9 FBKVO The feedback instrumentation amplifier output pin. 10 ERRIN The error amplifier inverting input pin. The input audio signal and the feedback signal are summed at this input pin. 11 ERRVO The error amplifier output pin. 12 TSD 13 STBY Standby function input pin. This pin is CMOS compatible. 14 FBK1 The feedback instrumentation amplifier pin. This must be connected to the feedback filter from VO1 (pin 15 on the LM4652 ). 16 OSC The switching frequency oscillation pin. Adjusting the resistor from 15.5kΩ to 0Ω changes the switching frequency from 75kHz to 225kHz. 17 Delay The dead time setting pin. The internally regulated positive voltage output for analog circuitry. This pin is available for internal regulator bypassing only. The positive supply input for the IC. The thermal shut down input pin for the thermal shut down output of the LM4652. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 LM4651 PIN DESCRIPTIONS (continued) 18 SCKT Short circuit setting pin. Minimum setting is 10A. 19 FBK2 The feedback instrumentation amplifier pin. This must be connected to the feedback filter from VO2 (pin 7 on the LM4652 ). 20,21 −VDDBYP 22,23 −VEE 24 START 25 LG1 Low−Gate #1 is the gate drive to a bottom side MOSFET in the H-Bridge. 26 LG2 Low−Gate #2 is the gate drive to a bottom side MOSFET in the H-Bridge. 28 OUT2 The reference pin of the power MOSFET output to the gate drive circuitry. The regulator output for digital blocks. This pin is for bypassing only. The negative voltage supply pin for the IC. The start up capacitor input pin. This capacitor adjusts the start up time of the diagnostic sequence for the modulator. Refer to Start Up Sequence and Self-Diagnostic Timing in the Application Information section. LM4652 PIN DESCRIPTIONS (1) Pin No. Symbol 1 GND A ground reference for the thermal shut down circuitry. 2 LG1 Low−Gate #1 is the gate input to a bottom side MOSFET in the H-Bridge. 3 −VEE The negative voltage supply input for the power MOSFET H-Bridge. 4 TSD The thermal shut down flag pin. This pin transitions to 6V when the die temperature exceeds 150°C. 5 NC No connection 6 LG2 Low−Gate #2 is the gate input to a bottom side MOSFET in the H-Bridge. 7 VO2 The switching output pin for one side of the H-Bridge. 8 NC No connection. 9 NC No connection. 10 HG2 High−Gate #2 is the gate input to a top side MOSFET in the H-Bridge. 11 NC No connection. 12 NC No connection. 13 +VCC The positive voltage supply input for the power MOSFET H-Bridge. 14 HG1 High−Gate #1 is the gate input to a top side MOSFET in the H-Bridge. 15 VO2 The switching output pin for one side of the H-Bridge. (1) Description Note: NC, no connect pins are floating pins. It is best to connect the pins to GND to minimize any noise from being coupled into the pins. External Components Description (Refer to Figure 3) Components Functional Description 1. R1 Works with R2, Rfl1 and Rfl2 to set the gain of the system. Gain = {[R2/(R1 + 100)] x [(Rfl1 + Rfl2)/Rfl2] − [R2/(R1 + 100)] + 0.5} + [(VCC - 20) * 0.0175] (V/V). 2. R2 See description above for R1. 3. Rf Sets the gain and bandwidth of the system by creating a low pass filter for the Error Amplifier's feedback with Cf. 3dB pole is at fC = 1/(2πRfCf) (Hz). 4. Cf See description above for Rf. 5. RfI1 Provides a reduction in the feedback with RfI2. RfI1should be 10 X RfI2 minimum to reduce effects on the pole created by RfI2 and CfI1. See also note for R1, R2 for effect on System Gain. 6. RfI2 RfI2 and CfI1 creates a low pass filter with a pole at fC = 1/(2πRfI2CfI1) (Hz). See also note for R1, R2 for effect on System Gain. 7. CfI1 See description above for RfI2. 8. RfI3 Establish the second pole for the low pass filter in the feedback path at fC = 1/(2πRfI3CfI2) (Hz). 9. CfI2 See description above for RfI3. 10. L1 Combined with CBYP creates a 2−pole, low pass output filter that has a −3dB pole at fC = 1/{2π[L1(2CBYP + C1)]1/2} (Hz). Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 7 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 8 www.ti.com Filters the commom mode high frequency noise from the amplifier's outputs to GND. Recommended value is 0.1µF to 1µF. 11. C1 12. Cbyp 13. CB1−CB4 14. CBT Provides the bootstrap capacitance for the boot strap pin. 15. RDLY Sets the dead time or break before make time to TDLY = (1.7x10−12)(500 + RDLY) (seconds) or RDLY = [TDLY/(1.7x10−12)] - 500 (Ω). 16. CSTART Controls the startup time with TSTART = (8.5x104) CSTART (seconds) or CSTART = TSTART /(8.5x104) (F). 17. RSCKT Sets the output current limit with ISCKT = (1x105)/(10kΩ ‖ RSCKT) (A) or RSCKT = [(1x109)/ISCKT] / [10k (1x105/ISCKT)] (Ω). 18. ROSC Controls the switching frequency with fSW = 1x109 / (4000 + ROSC) (Hz) or ROSC = (1x109/fSW) - 4000 (Ω). See description for L1. Bypass capacitors for VCC, VEE, analog and digital voltages (VDD, +6V, −6V). See Supply Bypassing and High Frequency PCB Design in the Application Information section for more information. 19. D1 20. CSBY1, CSBY2, CSBY3 Schottky diode to protect the output MOSFETs from fly back voltages. 21. ROFFSET Provides a small DC voltage at the input to minimize the output DC offset seen by the load. This also minimize power on pops and clicks. 22. CIN Blocks DC voltages from being coupled into the input and blocks the DC voltage created by ROFFSET from the source. 23. Rgate Supply de-coupling capacitors. See Supply Bypassing in the Application Information section. Slows the rise and fall time of the gate drive voltages that drive the output FET's. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Typical Performance Characteristics Output Power vs. Supply Voltage Output Power vs. Supply Voltage Figure 4. Figure 5. THD+N vs. Output Power RL = 4Ω THD+N vs. Output Power RL = 8Ω Figure 6. Figure 7. THD+N vs. Output Power RL = 4Ω THD+N vs. Output Power RL = 8Ω Figure 8. Figure 9. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 9 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Typical Performance Characteristics (continued) 10 THD+N vs. Frequency vs. Bandwidth RL = 4Ω THD+N vs. Frequency vs. Bandwidth RL = 8Ω Figure 10. Figure 11. THD+N vs. Frequency vs. Bandwidth RL = 4Ω THD+N vs. Frequency vs. Bandwidth RL = 8Ω Figure 12. Figure 13. Power Dissipation & Efficiency vs. Output Power Clipping Power Point & Efficiency vs. Switching Frequency (fSW) Figure 14. Figure 15. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Typical Performance Characteristics (continued) Frequency Response RL = 4Ω Supply Current vs. Switching Frequency (LM4651 & LM4652) Figure 16. Figure 17. Supply Current vs. Supply Voltage (LM4651 & LM4652) RDS(ON) vs. Temperature Figure 18. Figure 19. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 11 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com APPLICATION INFORMATION GENERAL FEATURES System Functional Information The LM4651 is a conventional pulse width modulator/driver. As Figure 20 shows the incoming audio signal is compared with a triangle waveform with a much higher frequency than the audio signal (not drawn to scale). The comparator creates a variable duty cycle squarewave. The squarewave has a duty cycle proportional to the audio signal level. The squarewave is then properly conditioned to drive the gates of power MOSFETs in an Hbridge configuration, such as the LM4652. The pulse train of the power MOSFETs are then fed into a low pass filter (usually a LC) which removes the high frequency and delivers an amplified replica of the audio input signal to the load. Figure 20. Conventional Pulse Width Modulation Standby Function The standby function of the LM4651 is CMOS compatible, allowing the user to perform a muting of the music by shutting down the pulse width waveform. Standby has the added advantage of minimizing the quiescent current. Because standby shuts down the pulse width waveform, the attenuation of the music is complete (>120dB), EMI is minimized, and any output noise is eliminated since there is no modulation waveform. When in Standby mode, the outputs of the LM4652 will both be at VCC. By placing a logic "1" or 5V at pin 13, the standby function will be enabled. A logic "0" or 0V at pin 13 will disable the standby function allowing modulation by the input signal. Under Voltage Protection The under voltage protection disables the output driver section of the LM4651 while the supply voltage is below ± 10.5V. This condition can occur as power is first applied or when low line, changes in load resistance or power supply sag occurs. The under voltage protection ensures that all power MOSFETs are off, eliminating any shootthrough current and minimizing pops or clicks during turn-on and turn-off. The under voltage protection gives the digital logic time to stabilize into known states providing a popless turn on. Start Up Sequence and Self-Diagnostic Timing The LM4651 has an internal soft start feature (see Figure 21) that ensures reliable and consistent start-up while minimizing turn-on thumps or pops. During the start-up cycle the system is in standby mode. This start-up time is controlled externally by adjusting the capacitance (CSTART) value connected to the START pin. The start-up time can be controlled by the capacitor value connected to the START pin given by Equation 1 or Equation 2: tSTART = (8.4x104)CSTART CSTART = TSTART/(8.5x104) (seconds) (Farads) (1) (2) The value of CSTART sets the time it takes for the IC to go though the start-up sequence and the frequency that the diagnostic circuitry checks to see if an error condition has been corrected. An Error condition occurs if current limit, thermal shut down, under voltage detection, or standby are sensed. The self-diagnostic circuit checks to see if any one of these error flags has been removed at a frequency set by the CSTART capacitor. For example, if the value of CSTART is 10µF then the diagnostic circuitry will check approximately every second to see if an error condition has been corrected. If the error condition is no longer present, the LM4651/52 will return to normal operation. 12 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Figure 21. Startup Timing Diagram Current Limiting and Short Circuit Protection The resistor value connected between the SCKT pin and GND determines the maximum output current. Once the output current is higher than the set limit, the short circuit protection turns all power MOSFETs off. The current limit is set to a minimum of 10A internally but can be increased by adjusting the value of the RSCKT resistor. Equation 3 shows how to find RSCKT. ISCKT = 1X105/(10kΩ‖ RSCKT) (Amps) (3) This feature is designed to protect the MOSFETs by setting the maximum output current limit under short circuit conditions. It is designed to be a fail-safe protection when the output terminals are shorted or a speaker fails and causes a short circuit condition. Thermal Protection The LM4651 has internal circuitry (pin 12) that is activated by the thermal shutdown output signal from the LM4652 (pin 4). The LM4652 has thermal shut down circuitry that monitors the temperature of the die. The voltage on the TSD pin (pin 4 of the LM4652) goes high (6V) once the temperature of the LM4652 die reaches 150°C. This pin should be connected directly to the TSD pin of the LM4651 (pin 12). The LM4651 disables the pulse width waveform when the LM4652 transmits the thermal shutdown flag. The pulse width waveform remains disabled until the TSD flag from the LM4652 goes low, signaling the junction temperature has cooled to a safe level. Dead Time Setting The DELAY pin on the LM4651 allows the user to set the amount of dead time or break before make of the system. This is the amount of time one pair of FETs are off before another pair is switched on. Increased dead time will reduce the shoot through current but has the disadvantage of increasing THD. The dead time should be reduced as the desired bandwidth of operation increases. The dead time can be adjusted with the RDLY resistor by Equation 4: TDLY = 1.7x10−12 (500 + RDLY) (Seconds) (4) Currently, the recommended value is 5kΩ. Oscillator Control The modulation frequency is set by an external resistor, ROSC, connected between pin 16 and GND. The modulation frequency can be set within the range of 50kHz to 225kHz according to the design requirements. The values of ROSC and fOSC can be found by Equation 5 and Equation 6: fOSC = 1x109/ (4000 + ROSC) ROSC = (1x109/ fOSC) − 4000 (Hz) (Ω) (5) (6) Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 13 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Equation 5 and Equation 6 are for RDLY = 0. Using a value of RDLY greater than zero will increase the value needed for ROSC. For RDLY = 5kΩ, ROSC will need to be increased by about 2kΩ. As the graphs show, increasing the switching frequency will reduce the THD but also decreases the efficiency and maximum output power level before clipping. Increasing the switching frequency increases the amount of loss because switching currents lower the efficiency across the output power range. A higher switching frequency also lowers the maximum output power before clipping or the 1% THD point occur. Over-Modulation Protection The over-modulation protection is an internally generated fixed pulse width signal that prevents any side of the Hbridge power MOSFETs from remaining active for an extended period of time. This condition can result when the input signal amplitude is higher than the internal triangle waveform. Lack of an over modulation signal can increase distortion when the amplifier's output is clipping. Figure 22 shows how the over modulation protection works. Figure 22. Over Modulation Protection The over modulation protection also provides a "soft clip" type response on the top of a sine wave. This minimum pulse time is internally set and cannot be adjusted. As the switching frequency increases this minimum time becomes a higher percentage of the period (TPERIOD = 1/fSW). Because the over modulation protection time is a higher percentage of the period, the peak output voltage is lower and, therefore, the output power at clipping is lower for the same given supply rails and load. Feedback Amplifier and Filter The purpose of the feedback amplifier is to differentially sample the output and provide a single-ended feedback signal to the error amplifier to close the feedback loop. The feedback is taken directly from the switching output before the demodulating LC filter to avoid the phase shift caused by the output filter. The signal fed back is first low pass filtered with a single pole or dual pole RC filter to remove the switching frequency and its harmonics. The differential signal, derived from the bridge output, goes into the high input impedance instrumentation amplifier that is used as the feedback amplifier. The instrumentation amplifier has an internally fixed gain of 1. The use of an instrumentation amplifier serves two purposes. First, it's input are high impedance so it doesn't load down the output stage. Secondly, an IA has excellent common-mode rejection when its gain setting resistors are properly matched. This feature allows the IA to derive the true feedback signal from the differential output, which aids in improving the system performance. Figure 23. Feedback instrumentation Amplifier Schematic 14 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Error Amplifier The purpose of the error amplifier is to sum the input audio signal with the feedback signal derived from the output. This inverting amplifier's gain is externally configurable by resistors Rf and R1. The parallel feedback capacitor and resistor form a low pass filter that limits the frequency content of the input audio signal and the feedback signal. The pole of the filter is set by Equation 7. fIP = 1/(2πRfCf) (Hz) (7) On-Board Regulators The LM4651 has its own internal supply regulators for both analog and digital circuits. Separate ±6V regulators exist solely for the analog amplifiers, oscillator and PWM comparators. A separate voltage regulator powers the digital logic that controls the protection, level shifting, and high−/low−side driver circuits. System performance is enhanced by bypassing each regulator's output. The ±6V regulator outputs, labeled +6VBYP (pin 6) and −6VBYP (pin 8) should be bypassed to ground. The digital regulator output, −VDDBYP (pins 20 & 21) should be bypassed to −VEE (pins 22 & 23). The voltage level of −VDDBYP should be always be 6V closer to ground than the negative rail, −VEE. As an example, if −VEE = −20V, then −VDDBYP should equal −14V. Recommended capacitor values and type can be found in Figure 3. APPLICATIONS HINTS Introduction Texas Instruments (TI) is committed to providing application information that assists our customers in obtaining the best performance possible from our products. The following information is provided in order to support this commitment. The reader should be aware that the optimization of performance was done using a reference PCB designed by NSC and shown in Figure 25 through Figure 29. Variations in performance can occur because of physical changes in the printed circuit board and the application. Therefore, the designer should know that component value changes may be required in order to optimize performance in a given application. The values shown in this data sheet can be used as a starting point for evaluation purposes. When working with high frequency circuits, good layout practices are also critical to achieving maximum performance. Input Pre-Amplifier with Subwoofer Filter The LM4651 and LM4652 Class D solution is designed for low frequency audio applications where low gain is required. This necessitates a pre−amplifier stage with gain and a low pass audio filter. An inexpensive input stage can be designed using TI's LM833 audio operational amplifier and a minimum number of external components. A gain of 10 (20dB) is recommended for the pre−amplifier stage. For a subwoofer application, the pole of the low pass filter is normally set within the range of 60Hz − 180Hz. For a clean sounding subwoofer the filter should be at least a second-order filter to sharply roll off the high frequency audio signals. A higher order filter is recommended for stand-alone self-powered subwoofer applications. Figure 6 shows a simple input stage with a gain of 10 and a second-order low pass filter. Figure 24. Pre−amplifier Stage with Low Pass Filter Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 15 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Supply Bypassing Correct supply bypassing has two important goals. The first is to ensure that noise on the supply lines does not enter the circuit and become audible in the output. The second is to help stabilize an unregulated power supply and provide current under heavy current conditions. Because of the two different goals multiple capacitors of various types and values are recommended for supply bypassing. For noise de-coupling, generally small ceramic capacitors (.001µF to .1µF) along with slightly larger tantalum or electrolytic capacitors (1µF to 10µF) in parallel will do an adequate job of removing most noise from the supply rails. These capacitors should be placed as close as possible to each IC's supply pin(s) using leads as short as possible. For supply stabilizing, large electrolytic capacitors (3,300µF to 15,000µF) are needed. The value used is design and cost dependent. High Frequency PCB Design A double-sided PCB is recommended when designing a class D amplifier system. One side should contain a ground plane with the power traces on the other side directly over the ground plane. The advantage is the parasitic capacitance created between the ground plane and the power planes. This parasitic capacitance is very small (pF) but is the value needed for coupling high frequency noise to ground. At high frequencies, capacitors begin to act more like inductors because of lead and parasitic inductance in the capacitor. For this reason, bypassing capacitors should be surface mount because of their low parasitic inductance. Equation 8 shows how to determine the amount of power to ground plane capacitance. C = εoεrA/d (Farads) where • here εo = 0.22479pF/in and εr = 4.1 (8) A is the common PCB area and d is the distance between the planes. The designer should target a value of 100pF or greater for both the positive supply to ground capacitance and negative supply to ground capacitance. Signal traces that cross over each other should be laid out at 90° to minimized any coupling. Output Offset Voltage Minimization The amount of DC offset voltage seen at the output with no input signal present is already quite good with the LM4651/52. With no input signal present the system should be at 50% duty cycle. Any deviation from 50% duty cycle creates a DC offset voltage seen by the load. To completely eliminate the DC offset, a DC voltage divider can be used at the input to set the DC offset to near zero. This is accomplished by a simple resistor divider that applies a small DC voltage to the input. This forces the duty cycle to 50% when there is no input signal. The result is a LM4651 and LM4652 system with near zero DC offset. The divider should be a 1.8MΩ from the +6V output (pin 6) to the input (other side of 25k, R1). R1 acts like the second resistor in the divider. Also use a 1µF input capacitor before R1 to block the DC voltage from the source. R1 and the 1µF capacitor create a high pass filter with a 3dB point at 6.35Hz. The value of ROFFSET is set according to the application. Variations in switching frequency and supply voltage will change the amount of offset voltage requiring a different value than stated above. The value above (1.8MΩ) is for ±20V and a switching frequency of 125kHz. Output Stage Filtering As common with Class D amplifier design, there are many trade-offs associated with different circuit values. The output stage is not an exception. Texas Insturments has found good results with a 50µF inductor and a 5µF Mylar capacitor (see Figure 3) used as the output LC filter. The two-pole filter contains three components; L1 and CBYP because the LM4651 and LM4652 have a bridged output. The design formula for a bridge output filter is fC = 1/{2π[L1(2CBYP + C1)]½} (Hz). A common mistake is to connect a large capacitor between ground and each output. This applies only to singleended applications. In bridge operation, each output sees CBYP. This causes the extra factor of 2 in the formula. The alternative to CBYP is a capacitor connected between each output, VO, and VO2, and ground. This alternative is, however, not size or cost efficient because each capacitor must be twice CBYP's value to achieve the same filter cutoff frequency. The additional small value capacitors connected between each output and ground (C1) help filter the high frequency from the output to ground . The recommended value for C1 is 0.1µF to 1µF or 2% to 20% of CBYP." 16 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Modulation Frequency Optimization Setting the modulation frequency depends largely on the application requirements. To maximize efficiency and output power a lower modulation frequency should be used. The lower modulation frequency will lower the amount of loss caused by switching the output MOSFETs increasing the efficiency a few percent. A lower switching frequency will also increase the peak output power before clipping because the over modulation protection time is a smaller percentage of the total period. Unfortunately, the lower modulation frequency has worse THD+N performance when the output power is below 10 watts. The recommended switching frequency to balance the THD+N performance, efficiency and output power is 125kHz to 145kHz. THD+N Measurements and Out of Audio Band Noise THD+N (Total Harmonic Distortion plus Noise) is a very important parameter by which all audio amplifiers are measured. Often it is shown as a graph where either the output power or frequency is changed over the operating range. A very important variable in the measurement of THD+N is the bandwidth limiting filter at the input of the test equipment. Class D amplifiers, by design, switch their output power devices at a much higher frequency than the accepted audio range (20Hz - 20kHz). Switching the outputs makes the amplifier much more efficient than a traditional Class A/B amplifier. Switching the outputs at high frequency also increases the out-of-band noise. Under normal circumstances this out-of-band noise is significantly reduced by the output low pass filter. If the low pass filter is not optimized for a given switching frequency, there can be significant increase in out-of-band noise. THD+N measurements can be significantly affected by out-of-band noise, resulting in a higher than expected THD+N measurement. To achieve a more accurate measurement of THD, the bandwidth at the input of the test equipment must be limited. Some common upper filter points are 22kHz, 30kHz, and 80kHz. The input filter limits the noise component of the THD+N measurement to a smaller bandwidth resulting in a more real-world THD+N value. The output low pass filter does not remove all of the switching fundamental and harmonics. If the switching frequency fundamental is in the measurement range of the test equipment, the THD+N measurement will include switching frequency energy not removed by the output filter. Whereas the switching frequency energy is not audible, it's presence degrades the THD+N measurement. Reducing the bandwidth to 30kHz and 22kHz reveals the true THD performance of the Class D amplifier. Increasing the switching frequency or reducing the cutoff frequency of the output filter will also reduce the level of the switching frequency fundamental and it's harmonics present at the output. This is caused by a switching frequency that is higher than the output filter cutoff frequency and, therefore, more attenuation of the switching frequency. In-band noise is higher in switching amplifiers than in linear amplifiers because of increased noise from the switching waveform. The majority of noise is out of band (as discussed above), but there is also an increase of audible noise. The output filter design (order and location of poles) has a large effect on the audible noise level. Power supply voltage also has an effect on noise level. The output filter removes a certain amount of the switching noise. As the supply increases, the attenuation by the output fiter is constant. However, the switching waveform is now much larger resulting in higher noise levels. THERMAL CONSIDERATIONS Heat Sinking The choice of a heat sink for the output FETs in a Class D audio amplifier is made such that the die temperature does not exceed TJMAX and activate the thermal protection circuitry under normal operating conditions. The heat sink should be chosen to dissipate the maximum IC power which occurs at maximum output power for a given load. Knowing the maximum output power, the ambient temperature surrounding the device, the load and the switching frequency, the maximum power dissipation can be calculated. The additional parameters needed are the maximum junction temperature and the thermal resistance of the IC package (θJC, junction to case), both of which are provided in the Absolute Maximum Ratings and Operating Ratings sections above. It should be noted that the idea behind dissipating the power within the IC is to provide the device with a low resistance to convection heat transfer such as a heat sink. Convection cooling heat sinks are available commercially and their manufacturers should be consulted for ratings. It is always safer to be conservative in thermal design. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 17 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Proper IC mounting is required to minimize the thermal drop between the package and the heat sink. The heat sink must also have enough metal under the package to conduct heat from the center of the package bottom to the fins without excessive temperature drop. A thermal grease such as Wakefield type 120 or Thermalloy Thermacote should be used when mounting the package to the heat sink. Without some thermal grease, the thermal resistance θCS (case to sink) will be no better than 0.5°C/W, and probably much worse. With the thermal grease, the thermal resistance will be 0.2°C/W or less. It is important to properly torque the mounting screw. Over tightening the mounting screw will cause the package to warp and reduce the contact area with the heat sink. It can also crack the die and cause failure of the IC. The recommended maximum torque applied to the mounting screw is 40 inch-lbs. or 3.3 foot-lbs. Determining Maximum Power Dissipation Power dissipation within the integrated circuit package is a very important parameter. An incorrect maximum power dissipation (PD) calculation may result in inadequate heat sinking, causing thermal shutdown circuitry to operate intermittently. There are two components of power dissipation in a class D amplifier. One component of power dissipation in the LM4652 is the RDS(ON) of the FET times the RMS output current when operating at maximum output power. The other component of power dissipation in the LM4652 is the switching loss. If the output power is high enough and the DC resistance of the filter coils is not minimized then significant loss can occur in the output filter. This will not affect the power dissipation in the LM4652 but should be checked to be sure that the filter coils with not over heat. The first step in determining the maximum power dissipation is finding the maximum output power with a given voltage and load. Refer to the graph Output Power verses Supply Voltage to determine the output power for the given load and supply voltage. From this power, the RMS output current can be calculated as IOUTRMS = SQRT(POUT/RL). The power dissipation caused by the output current is PDOUT = (IOUTRMS)2 * (2 * RDS(ON)). The value for RDS(ON) can be found from the Electrical Characteristics for LM4652 table above. The percentage of loss due to the switching is calculated by Equation 9: %LOSSSWITCH = (tr+ tf + TOVERMOD) * fSW (9) tr, tf and TOVERMOD can be found in the Electrical Characteristics for LM4651 and Electrical Characteristics for LM4652 sections above. The system designer determines the value for fSW (switching frequency). Power dissipation caused by switching loss is found by Equation 10. POUTMAX is the 1% output power for the given supply voltage and the load impedance being used in the application. POUTMAX can be determined from the graph Output Power vs. Supply Voltage in the Typical Performance Characteristics section above. PDSWITCH = (%LOSSSWITCH * POUTMAX) / (1−%LOSSSWITCH) (Watts) (10) PDMAX for the LM4652 is found by adding the two components (PDSWITCH + PDOUT) of power dissipation together. Determining the Correct Heat Sink Once the LM4652's power dissipation known, the maximum thermal resistance (in °C/W) of a heat sink can be calculated. This calculation is made using Equation 11 and is based on the fact that thermal heat flow parameters are analogous to electrical current flow properties. PDMAX = (TJMAX − TAMBIENTMAX) / θJA (Watts) where • θJA = θJC + θCS + θSA (11) Since we know θJC, θCS, and TJMAX from the Absolute Maximum Ratings and Operating Ratings sections above (taking care to use the correct θJC for the LM4652 depending on which package type is being used in the application) and have calculated PDMAX and TAMBIENTMAX, we only need θSA, the heat sink's thermal resistance. The following equation is derived from Equation 11: θSA = [(TJMAX − TAMBIENTMAX) / PDMAX] − θJC − θCS (12) Again, it must be noted that the value of θSA is dependent upon the system designer's application and its corresponding parameters as described previously. If the ambient temperature surrounding the audio amplifier is higher than TAMBIENTMAX, then the thermal resistance for the heat sink, given all other parameters are equal, will need to be lower. 18 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Example Design of a Class D Amplifier The following is an example of how to design a class D amplifier system for a power subwoofer application utilizing the LM4651 and LM4652 to meet the design requirements listed below: • Output Power, 1% THD 125W • Load Impedance 4Ω • Input Signal level 3V RMS (max) • Input Signal Bandwidth 10Hz − 150Hz • Ambient Temperature 50°C (max) Determine the Supply Voltage From the graph Output Power verses Supply voltage at 1% THD the supply voltage needed for a 125 watt, 4Ω application is found to be ±20V. Determine the Value for ROSC(Modulation Frequency) The oscillation frequency is chosen to obtain a satisfactory efficiency level while also maintaining a reasonable THD performance. The modulation frequency can be chosen using the Clipping Power Point and Efficiency verses Switching Frequency graph. A modulation frequency of 125kHz is found to be a good middle ground for THD performance and efficiency. The value of the resistor for ROSC is found from Equation 6 to be 3.9 kΩ. Determine the Value for RSCKT (Circuit Limit) The current limit is internally set as a failsafe to 10 amps. The inductor ripple current and the peak output current must be lower than 10 amps or current limit protection will turn on. A typical 4Ω load driven by a filter using 50µH inductors does not require more than 10A. The current limit will have to be increased when loads less than 4Ω are used to acheive higher output power. With RSCKT equal to 100kΩ, the current limit is 10A. Determine the Value for RDLY (Dead Time Control) The delay time or dead time is set to the recommended value so RDLY equals 5kΩ. If a higher bandwidth of operation is desired, RDLY should be a lower value resistor. If a zero value for RDLY is desired, connect the LM4651's pin 17 to GND. Determine the Value of L1, CBYP, C1, Rfl1 Rfl2, Cfl1 Cfl2, Rf, Cf (the Output and Feedback Filters) All component values show in Figure 3, are optimized for a subwoofer application. Use the following guidelines when changing any component values from those shown. The frequency response of the output filter is controlled by L1 and CBYP. Refer to the Application Information section titled Output Stage Filtering for a detailed explanation on calculating the correct values for L1 and CBYP. C1 should be in the range of 0.1µF to 1µF or 2 - 20% of CBYP. Rfl1 and Rfl2 are found by the ratio Rfl1 = 10Rfl2. A lower ratio can be used if the application is for lower output voltages than the 125Watt, 4Ω solution show here. The feedback RC filter's pole location should be higher than the output filter pole. The reason for two capacitors in parallel instead of one larger capacitor is to reduce the possible EMI from the feedback traces. Cfl1 is placed close as possible to the output of the LM4652 so that an audio signal is present on the feedback trace instead of a high frequency square wave. Cfl2 is then placed as close as possible to the feedback inputs (pins 14, 19) of the LM4651 to filter off any noise picked up by the feedback traces. The combination lowers EMI and provides a cleaner audio feedback signal to the LM4651. Rf should be in range of 100kΩ to1MΩ. Cf controls the bandwidth of the error signal and should be in the range of 100pF to 470pF. Determine the Value for CSTART (Start Up Delay) The start-up delay is chosen to be 1 second to ensure minimum pops or clicks when the amplifier is powered up. Using Equation 2, the value of CSTART is 11.7µF. A standard value of 10µF is used. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 19 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Determine the Value of Gain, R1, and R2 The gain is set to produce a 125W output at no more than 1% distortion with a 3VRMS input. A dissipation of 125W in a 4Ω load requires a 22.4VRMS signal. To produce this output signal, the LM4651/LM4652 amplifier needs an overall closed-loop gain of 22.4VRMS/3VRMS, or 7.5V/V (17.5db). Equation 13 shows all the variables that affect the system gain. Gain = {[R2/(R1 + 100)] x [(Rfl1 + Rfl2)/Rfl2] − [R2/(R1 + 100)] + 0.5} + [(VCC - 20) * 0.0175] (V/V) (13) The values for RfI1, RfI2, and Rf were found in the Determine the Value of the Filters section above and shown in Figure 1. Therefore, RfI1 = 620kΩ, RfI2 = 62kΩ and Rf = 390kΩ. The value of VCC was also found as the first step in this example to be ±20V. Inserting these values into Equation 13 and reducing gives the equation below: R2 = 0.7(R1 + 100) (14) The input resistance is desired to be 20kΩ so R1 is set to 20kΩ. R2 is then found to require a value of 14.1kΩ. Standard resistor values are 14.0kΩ giving a gain of 7.43V/V or 14.3kΩ giving a gain of 7.58V/V. Lowering R2 direcly affects the noise of the system. Changing R1 to increase gain with the lower value for R2 has very little affect on the noise level. The percent change in noise is about what whould be expected with a higher gain. The drawback to a lower R1 value is a larger CIN value, necessary to properly couple the lowest desired signal frequencies. If a 20kΩ input impedance is not required, then the recommended values shown in Figure 3 should be used: with R1's value set to 4.7kΩ and then using a value of 3.4kΩ for R2 for a gain of 7.5V/V. Determine the Needed Heat Sink The only remaining design requirement is a thermal design that prevents activating the thermal protection circuitry. Use Equation 9, Equation 10, and Equation 11 to calculate the amount of power dissipation for the LM4652. The appropriate heat sink size, or thermal resistance in °C/W, will then be determined. Equation 9 determines the percentage of loss caused by the switching. Use the typical values given in the Electrical Characteristics for LM4651 and Electrical Characteristics for LM4652 tables for the rise time, fall time and over modulation time: %Loss = (25ns+26ns+350ns) * 125kHz where • %Loss = 5.0% (15) This switching loss causes a maximum power dissipation, using Equation 10, of: PDSWITCH = (5.0% * 125W) / (1−5.0%) where • PDSWITCH = 6.6W (16) Next the power dissipation caused by the RDS(ON) of the output FETs is found by multiplying the output current times the RDS(ON). Again, the value for RDS(ON) is found from the Electrical Characteristics for LM4652 table above. The value for RDS(ON) at 100°C is used since we are calculating the maximum power dissipation. IOUTRMS = SQRT(125watts/4Ω) = 5.59 amps where • • PRDS(ON) = (5.59A)2 * (0.230Ω*2) PRDS(ON) = 14.4W (17) The total power dissipation in the LM4652 is the sum of these two power losses giving: PDTOTAL = 6.6W + 14.4W = 21W (18) The value for Maximum Power Dissipation given in the System Electrical Characteristics for LM4651 and LM4652 is 22 watts. The difference is due to approximately 1 watt of power loss in the LM4651. The above calculations are for the power loss in the LM4652. 20 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Lastly, use Equation 11 to determine the thermal resistance of the LM4652's heat sink. The values for θJC and TJMAX are found in the Operating Ratings and the Absolute Maximum Ratings section above for the LM4652. The value of θJC is 2°C/W for the isolated (NDB) package or 1°C/W for the non-isolated (NDL) package. The value for TJMAX is 150°C. The value for θCS is set to 0.2°C/W since this is a reasonable value when thermal grease is used. The maximum ambient temperature from the design requirements is 50°. The value of θSA for the isolated (NDB) package is: θSA = [(150°C − 50°C)/21W] − 2°C/W − 0.2°C/W where • θSA = 2.5°C/W (19) and for the non-isolated (NDL) package without a mica washer to isolate the heat sink from the package: θSA = [(150°C − 50°C)/21W] − 1°C/W − 0.2°C/W where • θSA = 3.5°C/W (20) To account for the use of a mica washer simply subtract the thermal resistance of the mica washer from θSA calculated above. Table 1. RECOMMENDATIONS FOR CRITICAL EXTERNAL COMPONENTS Circuit Symbol Suggested Value Suggested Type CfI1 330pF Ceramic Disc CfI2 100pF Ceramic Disc Cf 470pF Ceramic Disc Supplier/Contact Information Supplier Part # CB2 1.0µF - 10µF Resin Dipped Solid Tantalum CB1 & CBT 0.1µF Monolithic Ceramic CB3 0.001µF - 0.1µF Monolithic Ceramic C2 0.1µF - 1.0µF Metallized Polypropylene or Polyester Film CBYP 1.0µF - 10µF Metallized Polypropylene or Polyester Film Bishop Electronics Corp. (562) 695 - 0446 http://www.bishopelectronics.com/ BEC-9950 A11A-50V CBYP 1.0µF - 10µF Metallized Polypropylene or Polyester Film Nichicon Corp. (847) 843-7500 http://www.nichicon-us.com/ QAF2Exx or QAS2Exx D1 1A, 50V Fast Schottky Diode L1 25µH, 5A High Current Toroid Inductor (with header) J.W. Miller (310) 515-1720 http://www.jwmiller.com/ 6702 L1 47µH, 5A High Saturation Open Core (Vertical Mount Power Chokes) CoilCraft (847) 639-6400 http://www.coilcraft.com/ PCV-0473-05 L1 50µH, 5.6A High Saturation Flux Density Ferrite Rod J.W. Miller (310) 515-1720 http://www.jwmiller.com/ 5504 L1 68µH, 7.3A High Saturation Flux Density Ferrite Rod J.W. Miller (310) 515-1720 http://www.jwmiller.com/ 5512 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 21 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Figure 25. Reference PCB Schematic Figure 26. Reference PCB Silk Screen Layer 22 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Figure 27. Reference PCB Silk Screen and Solder Mask Layers Figure 28. Reference PCB Top Layer Figure 29. Reference PCB Bottom Layer Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 23 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Table 2. BILL OF MATERIALS FOR REFERENCE PCB Symbol Value Tolerance Type # per Board RFL1 620kΩ 1% 1/8 - 1/4 watt 2 RFL2 62kΩ 1% 1/8 - 1/4 watt 2 RFL3 0Ω 1% 1/8 - 1/4 watt 2 RF 1MΩ 1% 1/8 - 1/4 watt 1 R1 4.7kΩ 1% 1/8 - 1/4 watt 1 R2 4.7kΩ 1% 1/8 - 1/4 watt 1 RLP 2.2kΩ 1% 1/8 - 1/4 watt 1 ROFFSET 0 1% 1/8 - 1/4 watt 0 RDLY 5.1kΩ 10% 1/8 - 1/4 watt 1 RSCKT 39kΩ 10% 1/8 - 1/4 watt 1 ROSC 6.8kΩ 10% 1/8 - 1/4 watt 1 Supplier/Comment Part # Shorting Jumper ** NOT USED ** Can also use as a 5.6kΩ resistor All Caps. are Radial lead except CBYP, C1. Symbol Value Tolerance Type Voltage # per Board Supplier/Comment Part # CIN 1µF 10% Metal Polyester 100V 1 Digi-Key (800) 344-4539 EF1105-ND CLP 0.47µF 10% Metal Polyester 25V 1 Digi-Key (800) 344-4539 EF1474-ND CF 470pF 5% Ceramic Disc 25V 1 Digi-Key (800) 344-4539 1321PH-ND CFL1 0 5% Ceramic Disc 25V 0 ** NOT USED ** 1319PH-ND CFL2 100pF 5% Ceramic Disc 25V 2 Digi-Key (800) 344-4539 1313PH-ND CBT 0.1µF 10% - 20% Monolithic Ceramic 100V 2 Digi-Key (800) 344-4539 P4924-ND CB1 0.1µF 10% - 20% Monolithic Ceramic 100V 6 Digi-Key (800) 344-4539 P4924-ND CB2 1µF 10% Tantalum Radial lead 35V 6 Digi-Key (800) 344-4539 P2059-ND CB3 0.001µF 10% - 20% Monolithic Ceramic 100V 3 Digi-Key (800) 344-4539 P4898-ND CB4 47µF 10% - 20% Electrolytic Radial 16V 1 Digi-Key (800) 344-4539 P914-ND 1.5µF 10% Tantalum Radial lead 25V 1 Digi-Key (800) 344-4539 P2044-ND C1 0 10% Metal Polyester 25V 0 ** NOT USED ** C2 1µF 10% Metal Polyester 25V 2 Digi-Key (800) 344-4539 EF1105-ND CBYP 4.7µF 10% - 20% Metal Polyester 50V 1 Digi-Key (800) 344-4539 EF1475-ND CSBY1 4,700µF 20% Electrolytic Radial 25V 2 Digi-Key (800) 344-4539 P5637A-ND CSBY2 0.1µF 20% Ceramic Disc 25V 2 Digi-Key (800) 344-4539 P4201-ND CSBY3 0 10% - 20% Mylar Axial lead 50V 0 ** NOT USED ** CStart One or more pairs of coils from the list below is included with the reference PCB. Symbol Value Tolerance Type Voltage # per Board Supplier/Comment Part # L1 25µH 15% High Current Toroid with Header 5.5 amp 2 J.W. Miller (310) 515-1720 6702 L1 47µH 10% Ferrite Bobbin Core 5.0 amp 2 CoilCraft (847) 639-6400 http://www.coilcraft.com PVC-2-473-05 L1 50µH 10% Ferrite Core 5.6 amp 2 J.W. Miller (310) 515-1720 5504 # per Board Supplier/Comment Part # Symbol S1 Standoffs 24 Description (SPDT) on-on, switch for STBY 1 Mouser (800) 346-6873 1055-TA2130 Plastic Round, 0.875", 4-40 4 Newark (800) 463-9275 92N4905 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Table 2. BILL OF MATERIALS FOR REFERENCE PCB (continued) RCA Input PCB Mount Banana Jack Banana jack BLACK Heat sink D1 1 Mouser (800) 346-6873 16PJ097 5 Mouser (800) 346-6873 164-6218 Wakefield 603K, 2” high X 2” wide, ~ 7°C/W 1 Newark (800) 463-9275 58F537 (603K) 1A, 50Volt Schottky (40A surge current, 8.3mS) 4 Digi-Key (800) 344-4539 SR105CT-ND Additional Formulas for Reference PCB: Pole due to CIN: f3dB = 1/[2π(R1 + RLP)CIN] or CIN = 1/[2π(R1 + RLP)f3dB] Pole due to RLP and CLP: f3dB = 1/[2π(R1 // RLP)CLP] or CLP = 1/[2π(R1 // RLP)f3dB] where: (R1 // RLP) = 1/[1/R1 + 1/RLP] Gain for Reference PCB: Gain = {[R2/(R1 + 100 + Rlp)] x [(Rfl1 + Rfl2)/Rfl2] − [R2/(R1 + 100 + Rlp)] + 0.5} + [(VCC - 20) * 0.0175] FULL AUDIO BANDWIDTH OPERATION There is nothing in the design of the LM4651/52 class D chipset that prevents full audio bandwidth (20 – 20kHz) operation. For full bandwidth operation there are several external circuit changes required. Additional external circuitry is helpful to achieve a complete solution with the best performance possible with the LM4651/52 class D chipset. The additional sections and figures below detail the changes needed for either a 60W / 8Ω or 100W / 4Ω (10% THD+N) complete solution using a +/-17V supply. FILTERS To achieve full bandwidth operation there are several filter points that must be modified. They are the output filter, the feedback filters, the error amplifier filter and the input filter. If any of the filter points are too low there will be large phase shifts in the upper audio frequencies reducing the resolution and clarity of the highs. For this reason the frequency response of the system should be flat out to 20kHz. The mistake is often made to set the –3dB point near 20kHz resulting in good bench performance but poor quality in listening test. The output filter is made up of L1, L2, CBYP, CF1, CF2 (see Figure 31). The output filter design is determined by the load impedance along with the frequency response. The filter must have a 3dB point beyond 20kHz and a Q factor close to 0.707 for best performance. The output filter is the only filter that changes with the load impedance (See Table 2 for values). Standard inductor values were used for both 4Ω and 8Ω filters. The feedback filters and error amplifier filters will interact with the output filter if the individual pole locations of each are too close together. The feedback filter point is moved by reducing the value of CFL1, CFL3 to 50pF putting the feedback filter points approximately 5kHz higher than the output filter point. The error amplifier filter point is determined by Equation 7. Reducing the value of CF to 390pF gave the best results. The input filter in the typical application is a simple passive, single pole RC filter. For improved performance an active two pole filter was added as discussed below. Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 25 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com PRE-AMPLIFIER AND INPUT FILTER For a complete solution and best performance a pre-amplifier is required. With the addition of a pre-amplifier the gain of the class D stage can be greatly reduced to improve performance. The pre-amplifier gain is set to 10V/V allowing for low gain on the class D stage with total system gain high enough to be a complete solution from line level (1VRMS) sources. Without the pre-amplifier stage the class D stage must have much higher gain and will result in decreased performance in the form of much higher THD. With an extra op. amp. available on the other side of the LM833N the passive RC input filter is changed to an active two pole filter. The input filter does not noticeable increase THD performance but will help maintain a flat frequency response as the Q of the output filter changes with load impedance. A real speaker load impedance varies with frequency changing the Q of the output filter. The input filter is recommended to maintain flat response. For the pre-amplifier and input filter stage the circuit in Figure 6 was used with the complete input stage shown in Figure 12. SWITCHING FREQUENCY A switching frequency from 75kHz to 125kHz is adequate for subwoofer applications. A lower switching frequency has higher efficiency and higher output power at the start of clipping. For a full audio bandwidth application a higher switching frequency is needed. The switching frequency must be increased not only for waveform resolution for the higher audio frequencies but also to decrease the noise floor. A switching frequency of 175kHz was used for the performance graphs shown below. The Audio Precision AUX-0025 Switching Amplifier Measurement Filter was placed before the input to the Audio Precision unit for the THD+N graphs below. TYPICAL PERFORMANCE FOR FULL RANGE APPLICATION 26 Frequency Response ±17V, fSW = 175kHz, POUT = 5W = 0dB RL = 8Ω, No Filters THD+N vs Frequency ±17V, fSW = 175kHz, POUT = 1W & 25W RL = 8Ω, 30kHz BW THD+N vs Output Power ±17V, fSW = 175kHz RL = 8Ω, 30kHz BW Frequency Response ±17V, fSW = 175kHz, POUT = 5W = 0dB RL = 4Ω, No Filters Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 THD+N vs Frequency ±17V, fSW = 175kHz, POUT = 1W & 50W RL = 4Ω, 30kHz BW THD+N vs Output Power ±17V, fSW = 175kHz RL = 4Ω, 30kHz BW Figure 30. Input Pre-Amplifier And Filter Schematic Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 27 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Figure 31. Full Audio Bandwidth Schematic 28 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 FULL AUDIO BANDWIDTH REFERENCE BOARD ARTWORK Figure 32. Composite Top View Figure 33. Composite Bottom View Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 29 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Figure 34. Silk Screen Layer Figure 35. Top Layer 30 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 Figure 36. Bottom Layer Table 3. BILL OF MATERIALS FOR FULL AUDIO BANDWIDTH REFERENCE PCB Symbol Value Tolerance Type RFL1, RFL2 620kΩ 1% 1/8 – 1/4 Watt RFL3, RFL4 62kΩ 1% 1/8 – 1/4 Watt RF 1MΩ 1% 1/8 – 1/4 Watt R1 10kΩ 1% 1/8 – 1/4 Watt R2 3.3kΩ 1% 1/8 – 1/4 Watt Supplier/ Comment ROFFSET Part # ** NOT USED ** RDLY 5.1kΩ 5% RSCKT 39kΩ 5% 1/8 – 1/4 Watt 1/8 – 1/4 Watt ROSC 20kΩ 20% Trim Potentiometer RG1, RG2, RG3, RG4 3.3Ω 5% 1/8 – 1/4 Watt RTSD 100kΩ 5% 1/8 – 1/4 Watt RPA 10kΩ 1% 1/8 – 1/4 Watt Ri 1kΩ 1% 1/8 – 1/4 Watt RLP1, RLP2 2.7kΩ 1% 1/8 – 1/4 Watt RIN 47kΩ 5% 1/8 – 1/4 Watt RV1, RV2 750kΩ 5% Mouser (800) 346–6873 323–409H-20K 1/4 Watt All Capacitors are Radial lead Symbol Value Tolerance Type Voltage Supplier/Comment Part # CIN 1µF 10% Metal Polyester 100V Digi-Key (800) 344–4539 EF1105–ND CLP1 0.0022µF 10% Ceramic Disc 25V Digi-Key (800) 344–4539 P4053A-ND CLP2 0.001µF 10% Ceramic Disc 25V Digi-Key (800) 344–4539 P4049A-ND CBT1, CBT2 0.1µF 20% Monolithic Ceramic 100V Digi-Key (800) 344–4539 P4924–ND CF 390pF 10% Metal Polyester 25V Digi-Key (800) 344–4539 P4932–ND Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 31 OBSOLETE LM4651, LM4652 SNOS507H – MAY 2000 – REVISED APRIL 2013 www.ti.com Table 3. BILL OF MATERIALS FOR FULL AUDIO BANDWIDTH REFERENCE PCB (continued) CFL1, CFL3 47pF 10% Metal Polyester 50V CFL2 P4845–ND ** NOT USED ** CSTART 1.5μF 10% Tantalum Radial lead 25V Digi-Key (800) 344–4539 P2044–ND CB1, CB2 0.001μF 20% Monoilthic Ceramic 100V Digi-Key (800) 344–4539 P4898–ND CB3 – CB12 0.1μF 20% Monolithic Ceramic 100V Digi-Key (800) 344–4539 P4924–ND CS1 – CS5 1μF 10% Tantalum Radial lead 35V Digi-Key (800) 344–4539 P2059–ND CVD1 0.001μF 20% Monolithic Ceramic 100V Digi-Key (800) 344–4539 P4898–ND CVD2 47μF 20% Electrolytic Radial 16V Digi-Key (800) 344–4539 P914–ND CF1, CF2 0.1μF 10% Metal Polyester 25V Digi-Key (800) 344–4539 EF1104–ND CBYP (4Ω) 0.47μF 10% Metal Polyester 50V Digi-Key (800) 344–4539 EF1474–ND CBYP (8Ω) 0.22μF 10% Metal Polyester 50V Digi-Key (800) 344–4539 EF1224–ND CSBY1 , CSBY2 4,700μF 20% Electrolytic Radial 25V Digi-Key (800) 344–4539 P10289-ND CSBY3 , CSBY4 1,000μF 20% Electrolytic Radial 25V Digi-Key (800) 344–4539 P10279–ND CSBY5 , CSBY6 0.1μF Ceramic Disc 25V Digi-Key (800) 344–4539 P4201–ND CSBY7, CSBY8 47μF 20% Electrolytic Radial 16V Digi-Key (800) 344–4539 P914–ND Symbol Value Tolerance Type Rating Supplier/Comment Part # PVC–2–103–05 20% L1, L2 (4Ω) 10μH 10% Ferrite Bobbin Core 5.0 amp CoilCraft (847) 639–6400 http://www.coilcraft.com L1, L2 (8Ω) 22μH 10% Ferrite Bobbin Core 5.0 amp CoilCraft (847) 639–6400 http://www.coilcraft.com PVC–2–223–05 Symbol Description Supplier/Comment Part # S1 (SPDT) on-on, switch for STBY Mouser (800) 346–6873 1055–TA2130 D1 – D4 1A, 50V Schottky (40A surge current, 8.3ms) Digi-Key (800) 344–4539 SR105CT-ND ZDV1, ZDV2 12V, 500mW Zener diode Digi-Key (800) 344–4539 1N5242 Standoffs J1, J2, J3, J4 32 Digi-Key (800) 344–4539 Plastic Round, 0.875”, 4–40 Newark (800) 463–9275 92N4905 Banana jack RED Mouser (800) 346–6873 164–6219 J5 Banana jack BLACK Mouser (800) 346–6873 164–6218 J6 RCA jack, PCB mount Mouser (800) 346–6873 16PJ097 U1 Dual audio Op. Amp. Texas Instruments LM833N U2 Integrated Class D controller and amplifier Texas Instruments LM4651N U3 H-Bridge Power MOSFET Texas Instruments LM4652 Heat sink Wakefield 603K, 2” high x 2” wide, ∼7°C/W Newark (800) 463–9275 58F537 (603K) Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 OBSOLETE LM4651, LM4652 www.ti.com SNOS507H – MAY 2000 – REVISED APRIL 2013 REVISION HISTORY Changes from Revision G (April 2013) to Revision H • Page Changed layout of National Data Sheet to TI format .......................................................................................................... 31 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4651 LM4652 33 IMPORTANT NOTICE Texas Instruments Incorporated and its subsidiaries (TI) reserve the right to make corrections, enhancements, improvements and other changes to its semiconductor products and services per JESD46, latest issue, and to discontinue any product or service per JESD48, latest issue. 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