THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 D D D D D D D D AND DGN PACKAGE (TOP VIEW) ADSL Differential Receiver Low 1.6 nV/√Hz Voltage Noise High Speed – 100 MHz Bandwidth [–3 dB, G = 2 (–1)] – 100 V/µs Slew Rate 90 mA Output Drive (Typ) Very Low Distortion – THD = –72 dBc (f = 1 MHz, RL = 150 Ω) – THD = –90 dBc (f = 1 MHz, RL = 1 kΩ) 5 V, ±5 V to ±15 V Typical Operation Available in Standard SOIC or MSOP PowerPAD Package 1OUT 1IN – 1IN + –VCC 1 8 2 7 3 6 4 5 VCC+ 2OUT 2IN– 2IN+ Cross Section View Showing PowerPAD description The THS6062 is a high-speed differential receiver designed for ADSL data communication systems. Its very low 1.6 nV/√Hz voltage noise provides the high signal-to-noise ratios necessary for the long transmission lengths of ADSL systems over copper telephone lines. In addition, this receiver operates with a very low distortion of –90 dBc (f = 1 MHz, RL = 1 kΩ), exceeding the distortion requirements of ADSL CODECs. The THS6062 is a voltage feedback amplifier offering a high 100-MHz bandwidth and 100-V/µs slew rate and is stable at gains of 2(–1) or greater. It operates over a wide range of power supply voltages including 5 V and ±5 V to ±15 V. This device is available in standard SOIC or MSOP PowerPAD package. The small, surface-mount, thermally-enhanced MSOP PowerPAD package is fully compatible with automated surface-mount assembly procedures. THS6022 Driver 1 VI+ 50 Ω + _ 1:1 100 Ω To Telephone Line 1 kΩ 1 kΩ 2 kΩ Driver 2 VI– 50 Ω + _ THS6062 1 kΩ 1 kΩ – + Receiver 1 VO+ 2 kΩ 1 kΩ 1 kΩ 1 kΩ 1 kΩ – + VO– Receiver 2 Figure 1. Typical Client-Side ADSL Application CAUTION: The THS6062 provides ESD protection circuitry. However, permanent damage can still occur if this device is subjected to high-energy electrostatic discharges. Proper ESD precautions are recommended to avoid any performance degradation or loss of functionality. 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 is a trademark of Texas Instruments Incorporated. Copyright 1999, Texas Instruments Incorporated PRODUCTION DATA information is current as of publication date. Products conform to specifications per the terms of Texas Instruments standard warranty. Production processing does not necessarily include testing of all parameters. POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 1 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 HIGH-SPEED xDSL LINE DRIVER/RECEIVER FAMILY DEVICE DRIVER RECEIVER • • • • THS6002 THS6012 THS6022 5V • • THS6062 THS7002 ±5 V ±15 V • • • • • • • • • • • BW (MHz) SR (V/µs) THD f = 1 MHz (dB) IO (mA) Vn (nV/√Hz) 140 1000 –62 500 1.7 140 1300 –65 500 1.7 210 1900 –66 250 1.7 100 100 –72 90 1.6 70 100 –84 25 2.0 AVAILABLE OPTIONS PACKAGED DEVICES TA PLASTIC SMALL OUTLINE† (D) PowerPAD PLASTIC MSOP† (DGN) MSOP SYMBOL EVALUATION MODULE 0°C to 70°C THS6062CD THS6062CDGN TIABE THS6062EVM – 40°C to 85°C THS6062ID THS6062IDGN TIABH — † The D and DGN packages are available taped and reeled. Add an R suffix to the device type (i.e., THS6062CDGNR). functional block diagram VCC+ 8 1IN– 2 – 1 1IN+ 2IN– 3 6 + – 7 2IN+ 5 1OUT 2OUT + 4 VCC– 2 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 absolute maximum ratings over operating free-air temperature (unless otherwise noted)† Supply voltage, VCC+ to VCC– . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33V Input voltage, VI . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±VCC Output current, IO . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 150 mA Differential input voltage, VIO . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±4 V Continuous total power dissipation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . See Dissipation Rating Table Operating free-air temperature, TA: C–suffix . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0°C to 70°C I-suffix . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 40°C to 85°C Maximum junction temperature, TJ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 150°C Storage temperature, Tstg . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 65°C to 150°C Lead temperature, 1,6 mm (1/16 inch) from case for 10 seconds . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 300°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 PACKAGE θJA (°C/W) θJC (°C/W) TA = 25°C POWER RATING D 167† 38.3 740 mW DGN‡ 58.4 4.7 2.14 W † This data was taken using the JEDEC standard Low-K test PCB. For the JEDEC Proposed High-K test PCB, the θJA is 95°C/W with a power rating at TA = 25°C of 1.32 W. ‡ This data was taken using 2 oz. trace and copper pad that is soldered directly to a 3 in. × 3 in. PC. For further information, refer to Application Information section of this data sheet. recommended operating conditions MIN Supply voltage voltage, VCC+ CC and VCC– CC Operating free-air free air temperature, temperature TA NOM MAX ±2.5 ±16 Single supply 5 32 C-suffix 0 70 –40 85 Dual supply I-suffix POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 UNIT V °C 3 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 electrical characteristics at TA = 25°C, VCC = ±15 V, RL = 150 Ω (unless otherwise noted) PARAMETER VCC ICC Supply voltage operating range Supply current (per amplifier) TEST CONDITIONS Single supply Output voltage swing ISC VIO VCC = ±5 V 7.5 VCC = ±2.5 ±2 5 V TA = 25°C TA = full range 7.3 RL = 1 kΩ RL = 250 Ω Output current (see Note 1) VCC = ±15 V VCC = ±5 V Short-circuit current (see Note 1) VCC = ±2.5 V VCC = ±15 V RL = 150 Ω RL = 20 Ω Input offset voltage VCC = ±5 V or ±15 V Offset drift VCC = ±5 V or ±15 V VCC = ±5 V or ±15 V IOS Input offset current VCC = ±5 V or ±15 V Offset current drift VCC = ±5 V or ±15 V Power supply rejection ratio 9 10.5 mA 9 10.5 ±13 ±13.6 ±3.4 ±3.8 ±1 ±1.3 ±12 ±12.9 ±3 ±3.5 ±0.9 ±1.2 60 90 50 70 40 55 TA = 25°C TA = full range 1.5 V mA TA = full range TA = 25°C 20 mA 6 8 3 TA = full range TA = 25°C 30 TA = full range TA = full range 250 400 0.3 85 VICR = ±12 V VCC = ±5 V, V VICR = ±2.5 ±2 5 V TA = 25°C TA = full range 90 TA = 25°C TA = full range 85 mV µV/°C 6 8 V VCC = ±15 V, VCC = ±5 V or ±15 V V 11 TA = 25°C TA = full range Common mode rejection ratio UNIT 10 150 Input bias current PSRR 33 TA = 25°C TA = full range IIB CMRR 4.5 8.5 VCC = ±2.5 V VCC = ±15 V MAX ±16.5 TA = 25°C TA = full range VCC = ±5 V VCC = ±2.5 V IO TYP ± 2.25 VCC = ±15 V VCC = ±15 V VCC = ±5 V VO MIN Dual supply µA nA nA/°C 95 80 100 dB 85 80 95 dB † Full range = 0°C to 70°C for the THS6062C and –40°C to 85°C for the THS6062I. NOTE 1: Observe power dissipation ratings to keep the junction temperature below absolute maximum ratings when the output is heavily loaded or shorted. See the absolute maximum ratings section for more information. 4 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 electrical characteristics at TA = 25°C, VCC = ±15 V, RL = 150 Ω (unless otherwise noted) (continued) PARAMETER VICR Common-mode input voltage range RI Input resistance Ci Input capacitance RO Output resistance Open loop gain MIN TYP VCC = ±15 V VCC = ±5 V TEST CONDITIONS ±13.5 ±14.3 ±3.8 ±4.3 VCC = ±2.5 V ±1.4 ±1.8 Open loop VCC = ±15 V,, RL = 1 kΩ VO = ±10 V,, VCC = ±5 V,, RL = 1 kΩ VO = ±2.5 V,, TA = 25°C TA = full range 40 TA = 25°C TA = full range 35 MAX UNIT V 2 MΩ 1.5 pF 13 Ω 70 V/mV 35 50 V/mV 30 † Full range = 0°C to 70°C for the THS6062C and –40°C to 85°C for the THS6062I. operating characteristics at TA = 25°C, VCC = ±15 V, RL = 150 Ω (unless otherwise noted) TEST CONDITIONS† PARAMETER SR Slew rate (see Note 2) VCC = ±15 V VCC = ±5 V VCC = ±2.5 V VCC = ±15 V, Settling time to 0.1% ts Settling time to 0.01% THD Vn In BW Total harmonic distortion MIN TYP MAX UNIT 100 Gain = –1 80 V/µs 70 5-V step VCC = ±5 V, VCC = ±2.5 V, 2.5-V step VCC = ±15 V, VCC = ±5 V, 5-V step VCC = ±2.5 V, 1-V step 60 Gain = –1 1-V step 2.5-V step VCC = ±5 V or ±15 V, VO( V, f = 1 MHz MHz, O(pp)) = 2 V Gain = 2 45 ns 35 90 Gain = –1 80 ns 75 RL = 150 Ω –72 RL = 1 kΩ –90 dBc 1.6 nV/√Hz Input current noise VCC = ±5 V or ±15 V, f = 10 kHz VCC = ±5 V or ±15 V, f = 10 kHz 1.2 pA/√Hz 100 Dynamic D i performance f small-signal ll i l bandwidth (–3 dB) VCC = ±15 V VCC = ±5 V Input voltage noise Bandwidth for 0.1 dB flatness Full power bandwidth (see Note 3) Channel-to-channel crosstalk VO(pp) = 0.4 0 4 V, V Gain = 2 2, –1 VCC = ±2.5 V VCC = ±15 V 90 85 50 VO(pp) = 0.4 0 4 V, V Gain = 2 2, –1 VCC = ±5 V VCC = ±2.5 V MHz 45 40 VO(pp) = 20 V, VCC = ±15 V 1.6 RL = 1 kΩ VO(pp) = 5 V, VCC = ±5 V MHz 5 VCC = ±5 V or ±15 V, f = 1 MHz, Gain = 2 –61 dBc † Full range = 0°C to 70°C for the THS6062C and –40°C to 85°C for the THS6062I. NOTES: 2. Slew rate is measured from an output level range of 25% to 75%. 3. Full power bandwidth = slew rate /2 π V(peak) POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 5 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 PARAMETER MEASUREMENT INFORMATION 330 Ω 330 Ω 330 Ω _ VI1 330 Ω _ VO1 + CH1 50 Ω VO2 150 Ω + CH2 150 Ω 50 Ω Figure 2. THS6062 Crosstalk Test Circuit Rg Rf _ VI VO + RL 50 Ω Figure 3. Step Response Test Circuit Rg Rf VI 50 Ω _ VO + RL Figure 4. Step Response Test Circuit 6 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 VI2 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS Table of Graphs FIGURE VIO IIB Input offset voltage vs Free-air temperature 5 Input bias current vs Free-air temperature 6 VO Output voltage vs Supply voltage 7 Maximum output voltage swing vs Free-air temperature 8 IO ICC Maximum output current vs Free-air temperature 9 Supply current vs Free-air temperature 10 VIC ZO Common-mode input voltage vs Supply voltage 11 Closed-loop output impedance vs Frequency 12 Open-loop gain 13 Phase response 13 PSRR Power-supply rejection ratio vs Frequency 14 CMRR Common-mode rejection ratio vs Frequency 15 Crosstalk vs Frequency 16 Harmonic distortion vs Frequency 17, 18 Harmonic distortion vs Peak-to-peak output voltage 19, 20 Slew rate vs Free-air temperature 0.1% settling time vs Output voltage step size Output amplitude vs Frequency SR 21 22 23–29 Small and large frequency response 30–33 1-V step response 34, 35 4-V step response 36 20-V step response 37 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 7 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS INPUT OFFSET VOLTAGE vs FREE-AIR TEMPERATURE INPUT BIAS CURRENT vs FREE-AIR TEMPERATURE 3.10 3.05 –1.3 I IB – Input Bias Current – mA V IO – Input Offset Voltage – mV –1.2 VCC = ± 5 V –1.4 –1.5 VCC = ± 15 V –1.6 –1.7 VCC = ± 15 V 3 2.95 2.90 2.85 VCC = ± 5 V 2.80 2.75 –1.8 –40 –20 60 0 20 40 80 TA – Free-Air Temperature – °C 2.70 –40 100 –20 60 80 0 20 40 TA – Free-Air Temperature – °C Figure 5 Figure 6 OUTPUT VOLTAGE vs SUPPLY VOLTAGE MAXIMUM OUTPUT VOLTAGE SWING vs FREE–AIR TEMPERATURE 14 14 Maximum Output Voltage Swing – ± V TA = 25°C 12 |VO | – Output Voltage Swing – V 100 10 RL = 1 kΩ 8 RL = 150 Ω 6 4 2 13.5 VCC = ± 15 V RL = 1 kΩ 13 VCC = ± 15 V RL = 250 Ω 12.5 12 4.5 VCC = ± 5 V RL = 1 kΩ 4 3.5 VCC = ± 5 V RL = 150 Ω 3 2.5 2 1.5 VCC = ± 2.5 V RL = 1 kΩ VCC = ± 2.5 V RL = 150 Ω 0 2 4 6 8 10 12 ± VCC – Supply Voltage – ± V 14 16 1 –40 –20 Figure 7 8 60 80 0 20 40 TA – Free-Air Temperature – °C Figure 8 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 100 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS MAXIMUM OUTPUT CURRENT vs FREE-AIR TEMPERATURE SUPPLY CURRENT vs FREE-AIR TEMPERATURE 110 11 VCC = ± 15 V Sink Current 100 10 I CC – Supply Current – mA I O – Maximum Output Current – mA RL = 20 Ω 90 80 VCC = ± 15 V Source Current VCC = ± 5 V Sink Current VCC = ± 5 V Source Current 70 60 VCC = ± 2.5 V Sink Current 50 –40 –20 VCC = ± 2.5 V Source Current 60 80 0 20 40 TA – Free-Air Temperature – °C 100 9 VCC = ± 15 V 8 VCC = ± 2.5 V 7 6 VCC = ± 10 V 5 –40 –20 0 20 40 60 80 TA – Free-Air Temperature – °C Figure 9 100 Figure 10 COMMON-MODE INPUT VOLTAGE vs SUPPLY VOLTAGE CLOSED-LOOP OUTPUT IMPEDANCE vs FREQUENCY 15 100 TA = 25°C Z O– Closed-Loop Output Impedance – Ω VIC – Common-Mode Input Voltage – ± V VCC = ± 5 V 12.5 10 7.5 5 2.5 0 0 2.5 5 7.5 10 12.5 ± VCC – Supply Voltage – ± V 15 Gain = 1 RF = 1 kΩ PI = + 3 dBm 10 1 VO 1 kΩ 1 kΩ – 0.1 + 50 Ω VI THS6062 1000 VO Zo = –1 VI ( 0.01 100 k 1M 10 M 100 M ) 500 M f – Frequency – Hz Figure 11 Figure 12 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 9 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS OPEN-LOOP GAIN AND PHASE RESPONSE 100 45° VCC = ± 15 V RL = 150 Ω 80 0° 60 –45° Phase 40 –90° 20 –135° 0 –180° –20 100 Phase Response Open-Loop Gain – dB Gain –225° 1k 10 k 100 k 1M 10 M 100 M 1 G f – Frequency – Hz Figure 13 POWER-SUPPLY REJECTION RATIO vs FREQUENCY COMMON-MODE REJECTION RATIO vs FREQUENCY 120 CMRR – Common-Mode Rejection Ratio – dB PSRR – Power-Supply Rejection Ratio – dB 120 100 VCC+ 80 60 VCC– 40 20 VCC = ± 15 V and ± 5 V 0 10 10 100 1k 10 k 100 k 1M 10 M 100 M VCC = ± 5 V 100 VCC = ± 15 V 80 60 1 kΩ 1 kΩ 40 _ VI VO + 20 1 kΩ 1 kΩ RL 150 Ω 0 10 100 1k 10 k 100 k 1M f – Frequency – Hz f – Frequency – Hz Figure 14 Figure 15 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 10 M 100 M THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS CROSSTALK vs FREQUENCY 0 –10 VCC = ± 15 V PI = 0 dBm See Figure 1 Crosstalk – dB –20 –30 –40 –50 Input = CH 2 Output = CH 1 –60 –70 Input = CH 1 Output = CH 2 –80 –90 100 k 1M 10 M 100 M 500 M f – Frequency – Hz Figure 16 HARMONIC DISTORTION vs FREQUENCY Harmonic Distortion – dBc –50 –60 –40 VCC = ± 15 V and ± 5 V Gain = 2 RF = 300 Ω RL = 1 kΩ VO(PP) = 2 V –50 Harmonic Distortion – dBc –40 HARMONIC DISTORTION vs FREQUENCY Third Harmonic –70 –80 Second Harmonic –90 –100 –110 100 k –60 –70 VCC = ± 15 V and ± 5 V Gain = 2 RF = 300 Ω RL = 150 Ω VO(PP) = 2 V Second Harmonic –80 –90 –100 1M 10 M –110 100 k Third Harmonic 1M f – Frequency – Hz f – Frequency – Hz Figure 17 Figure 18 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 10 M 11 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS HARMONIC DISTORTION vs PEAK-TO-PEAK OUTPUT VOLTAGE HARMONIC DISTORTION vs PEAK-TO-PEAK OUTPUT VOLTAGE –50 –10 Third Harmonic VCC = ± 15 V Gain = 5 RF = 300 Ω RL = 150 Ω f = 1 MHz –20 –30 Second Harmonic Harmonic Distortion – dBc Harmonic Distortion – dBc –60 –70 –80 –90 VCC = ± 15 V Gain = 5 RF = 300 Ω RL = 1 kΩ f = 1 MHz –100 –110 0 2 4 6 8 10 12 14 16 18 VO(PP) – Peak-to-Peak Output Voltage – V –40 –50 Second Harmonic –60 –70 –80 –90 Third Harmonic –100 –110 20 0 2 4 6 8 10 12 14 16 18 VO(PP) – Peak-to-Peak Output Voltage – V Figure 19 Figure 20 SLEW RATE vs FREE-AIR TEMPERATURE 0.1% SETTLING TIME vs OUTPUT VOLTAGE STEP SIZE 120 80 VCC = ± 15 V Step = 20 V 100 90 80 70 VCC = ± 5 V Step = 4 V 60 VCC = ± 2.5 V Step = 2 V 50 40 –40 –20 Gain = –1 RF = 430 Ω 70 t s – 0.1% Settling Time – ns SR – Slew Rate – V/ µ s 110 Gain = –1 RL = 150 Ω VCC = ± 2.5 V 60 VCC = ± 5 V 50 VCC = ± 15 V 40 30 20 10 0 20 40 60 80 TA – Free-Air Temperature – °C 100 0 1 Figure 21 12 20 4 2 3 VO – Output Voltage Step Size – V Figure 22 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 5 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS OUTPUT AMPLITUDE vs FREQUENCY OUTPUT AMPLITUDE vs FREQUENCY 8 8 7 RF = 1 kΩ 7 5 Output Amplitude – dB Output Amplitude – dB 6 RF = 300 Ω RF = 100 Ω 4 3 2 VCC = ± 15 V Gain = 2 RL = 150 Ω VO(PP) = 0.4 V 1 0 –1 100 k 1M 6 5 RF = 100 Ω 3 2 0 100 M RF = 300 Ω 4 1 10 M RF = 1 kΩ VCC = ± 5 V Gain = 2 RL = 150 Ω VO(PP) = 0.4 V –1 100 k 500 M Figure 23 Figure 24 500 M 100 M 500 M 2 7 1 RF = 1 kΩ 6 5 Output Amplitude – dB Output Amplitude – dB 100 M OUTPUT AMPLITUDE vs FREQUENCY 8 RF = 300 Ω RF = 100 Ω 4 3 2 0 10 M f – Frequency – Hz OUTPUT AMPLITUDE vs FREQUENCY 1 1M f – Frequency – Hz VCC = ± 2.5 V Gain = 2 RL = 150 Ω VO(PP) = 0.4 V –1 100 k 1M 0 –1 500 M RF = 100 Ω –3 –4 –6 100 M RF = 360 Ω –2 –5 10 M RF = 1 kΩ VCC = ± 15 V Gain = –1 RL = 150 Ω VO(PP) = 0.4 V –7 100 k f – Frequency – Hz 1M 10 M f – Frequency – Hz Figure 25 Figure 26 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 13 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS OUTPUT AMPLITUDE vs FREQUENCY OUTPUT AMPLITUDE vs FREQUENCY 2 2 1 RF = 1 kΩ 0 –1 Output Amplitude – dB Output Amplitude – dB 1 RF = 360 Ω RF = 100 Ω –2 –3 –4 –5 –6 VCC = ± 5 V Gain = –1 RL = 150 Ω VO(PP) = 0.4 V –7 100 k RF = 1 kΩ 0 –1 RF = 360 Ω RF = 100 Ω –2 –3 –4 VCC = ± 2.5 V Gain = –1 RL = 150 Ω VO(PP) = 0.4 V –5 –6 1M 10 M 100 M –7 100 k 500 M 1M 10 M f – Frequency – Hz f – Frequency – Hz Figure 27 Figure 28 OUTPUT AMPLITUDE vs FREQUENCY 16 VCC = ± 15 V Output Amplitude – dB 14 12 10 VCC = ± 2.5 V 8 6 4 2 0 100 k Gain = 5 RF = 3.9 kΩ RL = 150 Ω VO(PP) = 0.4 V 1M 10 M 100 M f – Frequency – Hz Figure 29 14 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 500 M 100 M 500 M THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS SMALL AND LARGE SIGNAL FREQUENCY RESPONSE SMALL AND LARGE SIGNAL FREQUENCY RESPONSE 3 –3 –6 0 VO – Output Voltage Level – dBV VO – Output Voltage Level – dBV 0 3 VCC = ± 15 V Gain = 2 RF = 300 Ω RL= 150 Ω VI = 0.5 V RMS VI = 0.25 V RMS –9 –12 VI = 125 mV RMS –15 –18 VI = 62.5 mV RMS –21 –24 100 k –3 –6 VI = 0.25 V RMS –9 –12 VI = 125 mV RMS –15 –18 VI = 62.5 mV RMS –21 1M 10 M 100 M –24 100 k 500 M 1M f – Frequency – Hz –12 VI = 0.25 V RMS –15 18 VI = 125 mV RMS –21 –24 VI = 62.5 mV RMS –27 –30 100 k –3 –6 VO – Output Voltage Level – dBV VO – Output Voltage Level – dBV –9 500 M SMALL AND LARGE SIGNAL FREQUENCY RESPONSE VCC = ± 15 V Gain = –1 RF = 430 Ω RL = 150 Ω VI = 0.5 V RMS 100 M Figure 31 SMALL AND LARGE SIGNAL FREQUENCY RESPONSE –3 10 M f – Frequency – Hz Figure 30 –6 VCC = ± 5 V Gain = 2 RF = 300 Ω RL = 150 Ω VI = 0.5 V RMS VCC = ± 5 V Gain = –1 RF = 430 Ω RL = 150 Ω VI = 0.5 V RMS –9 –12 VI = 0.25 V RMS –15 18 VI = 125 mV RMS –21 –24 VI = 62.5 mV RMS –27 1M 10 M 100 M 500 M –30 100 k f – Frequency – Hz 1M 10 M 100 M 500 M f – Frequency – Hz Figure 32 Figure 33 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 15 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 TYPICAL CHARACTERISTICS 1-V STEP RESPONSE 1-V STEP RESPONSE 0.6 0.6 0.4 VO – Output Voltage – V VO – Output Voltage – V 0.4 VCC = ± 15 V Gain = 2 RF = 300 Ω RL = 150 Ω See Figure 2 0.2 0 –0.2 VCC = ± 2.5 V Gain = 2 RF = 300 Ω RL = 150 Ω See Figure 2 –0.4 0.2 0 –0.2 –0.4 –0.6 –0.6 0 50 100 150 200 250 0 300 200 t – Time – ns 800 1000 800 1000 Figure 35 4-V STEP RESPONSE 20-V STEP RESPONSE 2.5 15 2 10 VO – Output Voltage – V 1.5 VO – Output Voltage – V 600 t – Time – ns Figure 34 1 0.5 0 –0.5 VCC = ± 5 V Gain = –1 RF = 430 Ω RL = 150 Ω See Figure 3 –1 –1.5 –2 0 200 400 600 RL = 1 kΩ 5 VCC = ± 15 V Gain = 2 RF = 330 Ω See Figure 2 Offset For Clarity 0 RL = 150 Ω –5 –10 –2.5 800 1000 –15 0 t – Time – ns 200 400 600 t – Time – ns Figure 37 Figure 36 16 400 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION theory of operation The THS6062 is a high-speed, operational amplifier configured in a voltage feedback architecture. It is built using a 30-V, dielectrically isolated, complementary bipolar process with NPN and PNP transistors possessing fTs of several GHz. This results in an exceptionally high-performance amplifier that has a wide bandwidth, high slew rate, fast settling time, and low distortion. A simplified schematic is shown in Figure 38. (7) VCC + (1,7) OUT IN – (2,6) IN + (3,5) (4) VCC – Figure 38. THS6062 Simplified Schematic POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 17 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION The ADSL remote terminal receive band consists of 255 separate carrier frequencies each with its own modulation and amplitude level. With such an implementation, it is imperative that signals received off the telephone line have as high a signal-to-noise ratio (SNR) as possible. This is because of the numerous sources of interference on the line. The best way to accomplish this high SNR is to have a low-noise receiver on the front-end. It is also important to have the lowest distortion possible to help minimize against interference within the ADSL carriers. The THS6062 was designed with these two priorities in mind. By taking advantage of the superb characteristics of the complimentary bipolar process (BICOM), the THS6062 offers extremely low noise and distortion while maintaining a high bandwidth. There are some aspects that help minimize distortion in any amplifier. The first is to extend the bandwidth of the amplifier as high as possible without peaking. This allows the amplifier to eliminate any nonlinearities in the output signal. Another thing that helps to minimize distortion is to increase the load impedance seen by the amplifier, thereby reducing the currents in the output stage. This will help keep the output transistors in their linear amplification range and will also reduce the heating effects. This can be seen in Figures 17 to 20, which show a 1-kΩ load distortion is much better than a 150 Ω load. One client side terminal circuit implementation, shown in Figure 39, uses a 1:2 transformer ratio. While creating a power and output voltage advantage for the line drivers, the 1:2 transformer ratio reduces the SNR for the received signals. The ADSL standard, ANSI T1.413, stipulates a noise power spectral density of –140 dBm/Hz, which is equivalent to 31.6 nV/√Hz for a 100 Ω system. Although many amplifiers can reach this level of performance, actual ADSL system testing has indicated that the noise power spectral density may typically be ≤ –150 dBm/Hz, or ≤ 10 nV/√Hz. With a transformer ratio of 1:2, this number reduces to less than 5 nV/√Hz. The THS6062, with an equivalent input noise of 1.6 nV/√Hz, is an excellent choice for this application. Coupled with a very low 1.2 pA/√Hz equivalent input current noise and low value resistors, the THS6062 will ensure that the received signal SNR will be as high as possible. 18 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION 6V 0.1 µF THS6022 Driver 1 VI+ + 6.8 µF 12.5 Ω + _ 1:2 1 kΩ 100 Ω Telephone Line 1 kΩ 0.1 µF 6.8 µF + –6 V 6V 0.1 µF THS6022 Driver 2 VI– + 1 kΩ 6.8 µF 12.5 Ω + _ 499 Ω 499 Ω – + THS6062 Receiver 1 VO+ 1 kΩ 1 kΩ 0.1 µF 499 Ω 6.8 µF + 6V –6 V 1 kΩ 0.1 µF Driver Block 499 Ω – VO– + THS6062 Receiver 2 –6 V 0.01 µF Receiver Block Figure 39. THS6062 Client-Side ADSL Application POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 19 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION noise calculations and noise figure Noise can cause errors on very small signals. This is especially true for the amplifying small signals. The noise model for current feedback amplifiers (CFB) is the same as voltage feedback amplifiers (VFB). The only difference between the two is that the CFB amplifiers generally specify different current noise parameters for each input, while VFB amplifiers usually only specify one noise current parameter. The noise model is shown in Figure 40. This model includes all of the noise sources as follows: • • • • en = amplifier internal voltage noise (nV/√Hz) IN+ = noninverting current noise (pA/√Hz) IN– = inverting current noise (pA/√Hz) eRx = thermal voltage noise associated with each resistor (eRx = 4 kTRx ) eRs RS en Noiseless + _ eni IN+ eno eRf RF eRg IN– RG Ǹǒ Ǔ Figure 40. Noise Model The total equivalent input noise density (eni) is calculated by using the following equation: e + ni Where: en 2 ǒ ) IN ) Ǔ )ǒ ǒ 2 R S IN– R ǓǓ ǒ Ǔ ø RG ) 4 kTRs ) 4 kT RF ø RG F 2 k = Boltzmann’s constant = 1.380658 × 10–23 T = temperature in degrees Kelvin (273 +°C) RF || RG = parallel resistance of RF and RG ǒ Ǔ To get the equivalent output noise of the amplifier, just multiply the equivalent input noise density (eni) by the overall amplifier gain (AV). e no + eni AV + e ni 1 ) RR F (Noninverting Case) G As the previous equations show, to keep noise at a minimum, small value resistors should be used. As the closed-loop gain is increased (by reducing RG), the input noise is reduced considerably because of the parallel resistance term. This leads to the general conclusion that the most dominant noise sources are the source resistor (RS) and the internal amplifier noise voltage (en). Because noise is summed in a root-mean-squares method, noise sources smaller than 25% of the largest noise source can be effectively ignored. This can greatly simplify the formula and make noise calculations much easier to calculate. 20 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION noise calculations and noise figure (continued) For more information on noise analysis, please refer to the Noise Analysis section in Operational Amplifier Circuits Applications Report (literature number SLVA043). This brings up another noise measurement usually preferred in RF applications, the noise figure (NF). Noise figure is a measure of noise degradation caused by the amplifier. The value of the source resistance must be defined and is typically 50 Ω in RF applications. NF + 10log ȱȧ Ȳǒ ȳȧ Ǔȴ e 2 ni 2 e Rs Because the dominant noise components are generally the source resistance and the internal amplifier noise voltage, we can approximate the noise figure as: ȱȧ ȡȧǒ ȧȧ )Ȣ ȧȲ e NF + 10log 1 Ǔ )ǒ ) 2 n IN 4 kTR Ǔ ȣȧȤȳȧ 2 R S S ȧȧ ȧȴ Figure 40 shows the noise figure graph for the THS6062. NOISE FIGURE vs SOURCE RESISTANCE 16 f = 10 kHz TA = 25°C 14 Noise Figure – dB 12 10 8 6 4 2 0 10 100 1k Source Resistance – Ω 10 k Figure 41. Noise Figure vs Source Resistance POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 21 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION optimizing frequency response Internal frequency compensation of the THS6062 was selected to provide very wide bandwidth performance and still maintain a very low noise floor. In order to meet these performance requirements, the THS6062 must have a minimum gain of 2 (–1). Because everything is referred to the noninverting terminal of an operational amplifier, the noise gain in a G = –1 configuration is the same as in a G = 2 configuration. One of the keys to maintaining a smooth frequency response, and hence, a stable pulse response, is to pay particular attention to the inverting terminal. Any stray capacitance at this node causes peaking in the frequency response (see Figure 42 and Figure 43). There are two things that can be done to help minimize this effect. The first is to simply remove any ground planes under the inverting terminal of the amplifier. This also includes the trace that connects to this terminal. Additionally, the length of this trace should be minimized. The capacitance at this node causes a lag in the voltage being fed back due to the charging and discharging of the stray capacitance. If this lag becomes too long, the amplifier will not be able to correctly keep the noninverting terminal voltage at the same potential as the inverting terminal’s voltage. Peaking and possibly oscillations will then occur. OUTPUT AMPLITUDE vs FREQUENCY 9 Output Amplitude – dB 8 7 3 CIN– = 10 pF 2 6 No CIN– (Stray C Only) 5 4 3 2 300 Ω CIN– 300 Ω VI 0 100 k _ CIN–= 10 pF 0 No CIN– (Stray C Only) –1 –2 –3 –4 150 Ω VCC = ± 15 V Gain = –1 RF = 360 Ω RL = 150 Ω VO(PP) = 0.4 V 1 VO + 50 Ω 1 22 4 VCC = ± 15 V Gain = 2 RF = 300 Ω RL = 150 Ω VO(PP) = 0.4 V Output Amplitude – dB 10 OUTPUT AMPLITUDE vs FREQUENCY 360 Ω 360 Ω VI _ CIN– 56 Ω + VO 150 Ω –5 1M 10 M 100 M 500 M –6 100 k 1M 10 M f – Frequency – Hz f – Frequency – Hz Figure 42 Figure 43 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 100 M 500 M THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION optimizing frequency response (continued) The next thing that helps to maintain a smooth frequency response is to keep the feedback resistor (Rf) and the gain resistor (Rg) values fairly low. These two resistors are effectively in parallel when looking at the ac small-signal response. This is why in Figure 29, a feedback resistor of 3.9 kΩ with a gain resistor of 1 kΩ only shows a small peaking in the frequency response. The parallel resistance is only 800 Ω. This value, in conjunction with a very small stray capacitance test PCB, forms a zero on the edge of the amplifier’s natural frequency response. To eliminate this peaking, all that needs to be done is to reduce the feedback and gain resistances. One other way to compensate for this stray capacitance is to add a small capacitor in parallel with the feedback resistor. This helps to neutralize the effects of the stray capacitance. To keep this zero out of the operating range, the stray capacitance and resistor value’s time constant must be kept low. But, as can be seen in Figures 23 – 28, a value too low starts to reduce the bandwidth of the amplifier. Table 1 shows some recommended feedback resistors to be used with the THS6062. Table 1. Recommended Feedback Resistors GAIN Rf for VCC = ±15 V, ± 5 V, 5 V 2 300 Ω –1 360 Ω 5 3.3 kΩ (low stray-c PCB only) driving a capacitive load Driving capacitive loads with high performance amplifiers is not a problem as long as certain precautions are taken. The first is to realize that the THS6062 has been internally compensated to maximize its bandwidth and slew rate performance. When the amplifier is compensated in this manner, capacitive loading directly on the output will decrease the device’s phase margin leading to high frequency ringing or oscillations. Therefore, for capacitive loads of greater than 10 pF, it is recommended that a resistor be placed in series with the output of the amplifier, as shown in Figure 44. A minimum value of 20 Ω should work well for most applications. For example, in 75-Ω transmission systems, setting the series resistor value to 75 Ω both isolates any capacitance loading and provides the proper line impedance matching at the source end. 360 Ω 360 Ω Input _ 20 Ω Output THS6062 + CLOAD Figure 44. Driving a Capacitive Load POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 23 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION offset voltage The output offset voltage, (VOO) is the sum of the input offset voltage (VIO) and both input bias currents (IIB) times the corresponding gains. The following schematic and formula are used to calculate the output offset voltage: RF IIB– RG + – VI VO + RS ǒ ǒ ǓǓ ǒ ǒ ǓǓ IIB+ V OO + VIO 1 ) R R F G " IIB) RS 1 ) R R F G " IIB– RF Figure 45. Output Offset Voltage Model circuit layout considerations In order to achieve the high-frequency performance of the THS6062, it is essential that proper printed-circuit board high frequency design techniques be followed. A general set of guidelines is given below. In addition, a THS6062 evaluation board is available to use as a guide for layout or for evaluating the device performance. D D D D D 24 Ground planes – It is highly recommended that a ground plane be used on the board to provide all components with a low inductive ground connection. However, in the areas of the amplifier inputs and output, the ground plane can be removed to minimize the stray capacitance. Proper power supply decoupling – Use a 6.8-µF tantalum capacitor in parallel with a 0.1-µF ceramic capacitor on each supply terminal. It may be possible to share the tantalum among several amplifiers depending on the application, but a 0.1-µF ceramic capacitor should always be used on the supply terminal of every amplifier. In addition, the 0.1-µF capacitor should be placed as close as possible to the supply terminal. As this distance increases, the inductance in the connecting trace makes the capacitor less effective. The designer should strive for distances of less than 0.1 inches between the device power terminals and the ceramic capacitors. Sockets – Sockets are not recommended for high-speed operational amplifiers. The additional lead inductance in the socket pins will often lead to stability problems. Surface-mount packages soldered directly to the printed-circuit board is the best implementation. Short trace runs/compact part placements – Optimum high frequency performance is achieved when stray series inductance has been minimized. To realize this, the circuit layout should be made as compact as possible, thereby minimizing the length of all trace runs. Particular attention should be paid to the inverting input of the amplifier. Its length should be kept as short as possible. This will help to minimize stray capacitance at the input of the amplifier. Surface-mount passive components – Using surface-mount passive components is recommended for high frequency amplifier circuits for several reasons. First, because of the extremely low lead inductance of surface-mount components, the problem with stray series inductance is greatly reduced. Second, the small size of surface-mount components naturally leads to a more compact layout, thereby minimizing both stray inductance and capacitance. If leaded components are used, it is recommended that the lead lengths be kept as short as possible. POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION general PowerPAD design considerations The THS6062 is available packaged in a thermally-enhanced DGN package, which is a member of the PowerPAD family of packages. This package is constructed using a downset leadframe upon which the die is mounted [see Figure 46(a) and Figure 46(b)]. This arrangement results in the lead frame being exposed as a thermal pad on the underside of the package [see Figure 45(c)]. Because this thermal pad has direct thermal contact with the die, excellent thermal performance can be achieved by providing a good thermal path away from the thermal pad. The PowerPAD package allows for both assembly and thermal management in one manufacturing operation. During the surface-mount solder operation (when the leads are being soldered), the thermal pad can also be soldered to a copper area underneath the package. Through the use of thermal paths within this copper area, heat can be conducted away from the package into either a ground plane or other heat dissipating device. The PowerPAD package represents a breakthrough in combining the small area and ease of assembly of surface mount with the, heretofore, awkward mechanical methods of heatsinking. DIE Side View (a) Thermal Pad DIE End View (b) Bottom View (c) NOTE A: The thermal pad is electrically isolated from all terminals in the package. Figure 46. Views of Thermally Enhanced DGN Package Although there are many ways to properly heatsink this device, the following steps illustrate the recommended approach. Thermal pad area (68 mils x 70 mils) with 5 vias (Via diameter = 13 mils) Figure 47. PowerPAD PCB Etch and Via Pattern POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 25 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION general PowerPAD design considerations 1. Prepare the PCB with a top side etch pattern as shown in Figure 47. There should be etch for the leads as well as etch for the thermal pad. 2. Place five holes in the area of the thermal pad. These holes should be 13 mils in diameter. They are kept small so that solder wicking through the holes is not a problem during reflow. 3. Additional vias may be placed anywhere along the thermal plane outside of the thermal pad area. This helps dissipate the heat generated by the THS6062DGN IC. These additional vias may be larger than the 13-mil diameter vias directly under the thermal pad. They can be larger because they are not in the thermal pad area to be soldered so that wicking is not a problem. 4. Connect all holes to the internal ground plane. 5. When connecting these holes to the ground plane, do not use the typical web or spoke via connection methodology. Web connections have a high thermal resistance connection that is useful for slowing the heat transfer during soldering operations. This makes the soldering of vias that have plane connections easier. In this application, however, low thermal resistance is desired for the most efficient heat transfer. Therefore, the holes under the THS6062DGN package should make their connection to the internal ground plane with a complete connection around the entire circumference of the plated-through hole. 6. The top-side solder mask should leave the terminals of the package and the thermal pad area with its five holes exposed. The bottom-side solder mask should cover the five holes of the thermal pad area. This prevents solder from being pulled away from the thermal pad area during the reflow process. 7. Apply solder paste to the exposed thermal pad area and all of the IC terminals. 8. With these preparatory steps in place, the THS6062DGN IC is simply placed in position and run through the solder reflow operation as any standard surface-mount component. This results in a part that is properly installed. The actual thermal performance achieved with the THS6062DGN in its PowerPAD package depends on the application. In the example above, if the size of the internal ground plane is approximately 3 inches × 3 inches, then the expected thermal coefficient, θJA, is about 58.4°C/W. For comparison, the non-PowerPAD version of the THS6062 IC (SOIC) is shown. For a given θJA, the maximum power dissipation is shown in Figure 48 and is calculated by the following formula: P Where: + D ǒ Ǔ T –T MAX A q JA PD = Maximum power dissipation of THS6062 IC (watts) TMAX = Absolute maximum junction temperature (150°C) TA = Free-ambient air temperature (°C) θJA = θJC + θCA θJC = Thermal coefficient from junction to case θCA = Thermal coefficient from case to ambient air (°C/W) 26 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION general PowerPAD design considerations (continued) MAXIMUM POWER DISSIPATION vs FREE-AIR TEMPERATURE Maximum Power Dissipation – W 3.5 DGN Package θJA = 58.4°C/W 2 oz. Trace And Copper Pad With Solder 3 2.5 SOIC Package High-K Test PCB θJA = 98°C/W 2 TJ = 150°C DGN Package θJA = 158°C/W 2 oz. Trace And Copper Pad Without Solder 1.5 1 0.5 SOIC Package Low-K Test PCB θJA = 167°C/W 0 –40 –20 0 20 40 60 80 TA – Free-Air Temperature – °C 100 NOTE A: Results are with no air flow and PCB size = 3”× 3” Figure 48. Maximum Power Dissipation vs Free-Air Temperature More complete details of the PowerPAD installation process and thermal management techniques can be found in the Texas Instruments Technical Brief, PowerPAD Thermally Enhanced Package. This document can be found at the TI web site (www.ti.com) by searching on the key word PowerPAD. The document can also be ordered through your local TI sales office. Refer to literature number SLMA002 when ordering. The next thing that should be considered is the package constraints. The two sources of heat within an amplifier are quiescent power and output power. The designer should never forget about the quiescent heat generated within the device, especially a multiamplifier device. Because these devices have linear output stages (Class A-B), most of the heat dissipation is at low output voltages with high output currents. Figure 49 and Figure 50 show this effect, along with the quiescent heat, with an ambient air temperature of 50°C. When using VCC = 5 V or ±5 V, there is generally not a heat problem, even with SOIC packages. But, when using VCC = ±15 V, the SOIC package is severely limited in the amount of heat it can dissipate. The other key factor when looking at these graphs is how the devices are mounted on the PCB. The PowerPAD devices are extremely useful for heat dissipation. But the device should always be soldered to a copper plane to fully use the heat dissipation properties of the PowerPAD. The SOIC package, on the other hand, is highly dependent on how it is mounted on the PCB. As more trace and copper area is placed around the device, θJA decreases and the heat dissipation capability increases. The currents and voltages shown in these graphs are for the total package. Because the THS6062 is a dual amplifier, the sum of the RMS output currents and voltages should be used to choose the proper package. POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 27 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 APPLICATION INFORMATION general PowerPAD design considerations (continued) MAXIMUM RMS OUTPUT CURRENT vs RMS OUTPUT VOLTAGE DUE TO THERMAL LIMITS VCC = ± 5 V Tj = 150°C TA = 50°C 180 1000 Maximum Output Current Limit Line | IO | – Maximum RMS Output Current – mA | IO | – Maximum RMS Output Current – mA 200 160 140 Package With θJA < = 110°C/W 120 100 80 SO-8 Package θJA = 167°C/W Low-K Test PCB 60 MAXIMUM RMS OUTPUT CURRENT vs RMS OUTPUT VOLTAGE DUE TO THERMAL LIMITS 40 20 0 TJ = 150°C TA = 50°C VCC = ± 15 V Maximum Output Current Limit Line DGN Package θJA = 58.4°C/W 100 SO-8 Package θJA = 98°C/W High-K Test PCB SO-8 Package θJA = 167°C/W Low-K Test PCB 10 0 4 1 2 3 | VO | – RMS Output Voltage – V 5 0 Figure 49 3 6 9 12 | VO | – RMS Output Voltage – V 15 Figure 50 evaluation board An evaluation board is available for the THS6062 (literature number SLOP221). This board has been configured for very low parasitic capacitance in order to realize the full performance of the amplifier. For more information, refer to the THS6062 EVM User’s Guide (literature number SLOU036) To order the evaluation board contact your local TI sales office or distributor. 28 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 MECHANICAL DATA D (R-PDSO-G**) PLASTIC SMALL-OUTLINE PACKAGE 14 PIN SHOWN 0.050 (1,27) 0.020 (0,51) 0.014 (0,35) 14 0.010 (0,25) M 8 0.008 (0,20) NOM 0.244 (6,20) 0.228 (5,80) 0.157 (4,00) 0.150 (3,81) Gage Plane 0.010 (0,25) 1 7 0°– 8° A 0.044 (1,12) 0.016 (0,40) Seating Plane 0.069 (1,75) MAX 0.010 (0,25) 0.004 (0,10) PINS ** 0.004 (0,10) 8 14 16 A MAX 0.197 (5,00) 0.344 (8,75) 0.394 (10,00) A MIN 0.189 (4,80) 0.337 (8,55) 0.386 (9,80) DIM 4040047 / D 10/96 NOTES: A. B. C. D. All linear dimensions are in inches (millimeters). This drawing is subject to change without notice. Body dimensions do not include mold flash or protrusion, not to exceed 0.006 (0,15). Falls within JEDEC MS-012 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 29 THS6062 LOW-NOISE ADSL DUAL DIFFERENTIAL RECEIVER SLOS228B – JANUARY 1999 – REVISED JUNE 1999 MECHANICAL DATA DGN (S-PDSO-G8) PowerPAD PLASTIC SMALL-OUTLINE PACKAGE 0,38 0,25 0,65 8 0,25 M 5 Thermal Pad (See Note D) 0,15 NOM 3,05 2,95 4,98 4,78 Gage Plane 0,25 1 0°– 6° 4 3,05 2,95 0,69 0,41 Seating Plane 1,07 MAX 0,15 0,05 0,10 4073271/A 01/98 NOTES: A. B. C. D. All linear dimensions are in millimeters. This drawing is subject to change without notice. Body dimensions include mold flash or protrusions. The package thermal performance may be enhanced by attaching an external heat sink to the thermal pad. This pad is electrically and thermally connected to the backside of the die and possibly selected leads. E. Falls within JEDEC MO-187 PowerPAD is a trademark of Texas Instruments Incorporated. 30 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 IMPORTANT NOTICE Texas Instruments and its subsidiaries (TI) reserve the right to make changes to their products or to discontinue any product or service without notice, and advise customers to obtain the latest version of relevant information to verify, before placing orders, that information being relied on is current and complete. All products are sold subject to the terms and conditions of sale supplied at the time of order acknowledgement, including those pertaining to warranty, patent infringement, and limitation of liability. TI warrants performance of its semiconductor products to the specifications applicable at the time of sale in accordance with TI’s standard warranty. Testing and other quality control techniques are utilized to the extent TI deems necessary to support this warranty. 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