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1 John Brown Art Kay Tim Green Tina-TI SynthesizeTina-ize The Four Musketeers of HPL AnalyzeRecognize High Current V-I Circuits
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2 V-I Circuit “Recognize” Objectives Potential Applications, End Equipment, Markets Circuit Topologies Circuit Stability Issues Power Dissipation Issues Transient Protection Issues PCB Issues Semiconductor Overstress Issues
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3 V-I Circuit “Analyze, Synthesize, Tina-ize ” Objectives Provide Synthesis Techniques for Common Topologies Provide Tools to Simplify Stability Analysis Provide Analysis Techniques for Power Dissipation Provide Solutions for Common Transient Problems Provide Tips for PCB Layouts Provide Tricks for Tina-TI Analysis
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4 Power Amplifiers Strategy for Markets 1. High Volume Growth Communications Optical Networking ONET (TECs, Laser Diode Pumps, Avalanche Photodiode Bias HV) DLP Digital Light Projectors (high voltage OPA) Industrial Electromechanical (OPA, PWM) Automotive Electromechanical (OPA, PWM) 2. Gen Std Catalog Products Steady Growth Industrial, Medical, Lab, ATE, Some Audio, Consumer High Speed Buffers, High Voltage, High Current OPAs
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5 Power Amplifiers Applications in Markets 1. Test, Particularly Automated ATE Analog Pin Driver, Power V & I Excitation 2. Power Line Communication High Pulse Current Drive Through Transformer or Capacitor Coupled ac Power Line (Residential & Commercial) 3. Displays High Current Driver for Dithering Projected Light Beam, High Voltage for Ink Jet Printers 4. Industrial, Medical, Scientific, Analytical, and Laboratory TEC Drivers, Electromechanical Linear Valve/Positioner Drivers, Motors, Power Supplies 5. Optical Networking / Gen Laser Systems TEC Drivers (Thermo-electric Coolers), Laser Pumps 6. Some Audio Headphone and Speaker Drivers 7. Some Automotive Power Steering Pumps, Window Motors COMPETITION 1. Mostly Discrete 2. National Semiconductor, ST, Maxim, Allegro, ON-SEMI, International Rectifier, Infineon, Toshiba
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6 Review - Essential Principles Poles, Zeros, Bode Plots Op Amp Loop Gain Model Loop Gain Test β and 1/β Rate-of-Closure Stability Criteria Loop Gain Rules-of-Thumb for Stability R O and R OUT
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7 Commercial Break (Shameless Self-Promotion) See 15 Part Series: “Operational Amplifier Stability” http://www.analogzone.com/acqt0704.htm
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8 Poles and Bode Plots Pole Location = f P Magnitude = -20dB/Decade Slope Slope begins at f P and continues down as frequency increases Actual Function = -3dB down @ f P Phase = -45°/Decade Slope through f P Decade Above f P Phase = -90° Decade Below f P Phase = 0° A(dB) = 20Log 10 (V OUT /V IN )
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9 Zeros and Bode Plots Zero Location = f Z Magnitude = +20dB/Decade Slope Slope begins at f Z and continues up as frequency increases Actual Function = +3dB up @ f Z Phase = +45°/Decade Slope through f Z Decade Above f Z Phase = +90° Decade Below f Z Phase = 0° A(dB) = 20Log10(VOUT/VIN)
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10 Op Amp: Intuitive Model
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11 Op Amp Loop Gain Model V OUT /V IN = Acl = Aol/(1+Aolβ) If Aol >> 1 then Acl ≈ 1/β Aol: Open Loop Gain β: Feedback Factor Acl: Closed Loop Gain 1/ = Small Signal AC Gain = feedback attenuation
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12 Stability Criteria
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13 Traditional Loop Gain Test Op Amp Loop Gain Model Op Amp is “Closed Loop” SPICE Loop Gain Test: Break the Closed Loop at V OUT Ground V IN Inject AC Source, V X, into V OUT Aolβ = V Y /V X
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14 β and 1/β β is easy to calculate as feedback network around the Op Amp 1/β is reciprocal of β Easy Rules-Of-Thumb and Tricks to Plot 1/β on Op Amp Aol Curve
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15 Plot (in dB) 1/β on Op Amp Aol (in dB) Aolβ = Aol(dB) – 1/β(dB) Note how Aolβ changes with frequency Proof (using log functions): 20Log 10 [Aolβ] = 20Log 10 (Aol) - 20Log 10 (1/β) = 20Log 10 [Aol/(1/β)] = 20Log 10 [Aolβ] Loop Gain Using Aol & 1/β
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16 Stability Criteria using 1/β & Aol At fcl: Loop Gain (Aol ) = 1 Rate-of-Closure @ fcl = (Aol slope – 1/β slope) *20dB/decade Rate-of-Closure @ fcl = STABLE **40dB/decade Rate-of-Closure@ fcl = UNSTABLE
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17 Loop Gain Bandwidth Rule: 45 degrees for f < fcl Aolβ (Loop Gain) Phase Plot Loop Stability Criteria: <-180 degree phase shift at fcl Design for: <-135 degree phase shift at all frequencies <fcl Why?: Because Aol is not always “Typical” Power-up, Power-down, Power-transient Undefined “Typical” Aol Allows for phase shift due to real world Layout & Component Parasitics
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18 Poles & Zeros Transfer: (1/β, Aol) to Aolβ Aol & 1/β PlotLoop Gain Plot (Aolβ) To Plot Aolβ from Aol & 1/β Plot: Poles in Aol curve are poles in Aolβ (Loop Gain)Plot Zeros in Aol curve are zeros in Aolβ (Loop Gain) Plot Poles in 1/β curve are zeros in Aolβ (Loop Gain) Plot Zeros in 1/β curve are poles in Aolβ (Loop Gain) Plot [Remember: β is the reciprocal of 1/β]
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19 Frequency Decade Rules for Loop Gain Loop Gain View: Poles: fp1, fp2, fz1; Zero: fp3 Rules of Thumb for Good Loop Stability: Place fp3 within a decade of fz1 fp1 and fz1 = -135° phase shift at fz1 fp3 < decade will keep phase from dipping further Place fp3 at least a decade below fcl Allows Aol curve to shift to the left by one decade
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20 Op Amp Model for Derivation of R OUT From: Frederiksen, Thomas M. Intuitive Operational Amplifiers. McGraw-Hill Book Company. New York. Revised Edition. 1988. R OUT = R O / (1+Aolβ)
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21 Op Amp Model for Loop Stability Analysis R O is constant over the Op Amp’s bandwidth R O is defined as the Op Amp’s Open Loop Output Resistance R O is measured at I OUT = 0 Amps, f = 1MHz (use the unloaded R O for Loop Stability calculations since it will be the largest value worst case for Loop Stability analysis) R O is included when calculating for Loop Stability analysis
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22 R O & Op Amp Output Operation Bipolar Power Op Amps CMOS Power Op Amps Light Load vs Heavy Load
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23 R O Measure w/DC Operating Point: I OUT = 0mA
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24 R O Measure w/DC Operating Point: I OUT = 0mA R O = VOA / AM1 R O = 9.61mVrms / 698.17μArms R O = 13.765Ω
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25 R O Measure w/DC Operating Point I OUT = 4.45mA Sink
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26 R O Measure w/DC Operating Point I OUT = 4.45mA Sink R O = VOA / AM1 R O = 3.45Vrms / 706.25µArms R O = 4.885Ω
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27 R O Measure w/DC Operating Point I OUT = 5.61mA Source
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28 R O Measure w/DC Operating Point I OUT = 5.61mA Source R O = VOA / AM1 R O = 3.29mVrms / 700.98μArms R O = 4.693Ω
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29 R O Measure w/DC Operating Point I OUT = 2.74A Source
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30 R O Measure w/DC Operating Point I OUT = 2.74A Source R O = VOA / AM1 R O = 314.31uVrms / 550.1μArms R O = 0.571Ω
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31 R O Measure w/DC Operating Point I OUT = 2.2A Sink
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32 R O Measure w/DC Operating Point I OUT = 2.2A Sink R O = VOA / AM1 R O = 169.92uVrms / 635.16μArms R O = 0.267Ω
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33 R O Measure w/DC Operating Point I OUT = 0A
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34 R O Measure w/DC Operating Point I OUT = 0A R O = VOA / AM1 R O = 4.42mVrms / 702.69μArms R O = 6.29Ω
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35 R O Measure w/DC Operating Point I OUT = 1A Sink
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36 R O Measure w/DC Operating Point I OUT = 1A Sink R O = VOA / AM1 R O = 166.76μVrms / 540.19μArms R O = 0.309Ω
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37 R O Measure w/DC Operating Point I OUT = 1A Source
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38 R O Measure w/DC Operating Point I OUT = 1A Source R O = VOA / AM1 R O = 166.61μVrms / 540.34μArms R O = 0.308Ω
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39 Non-Inverting Floating Load V-I Basic Topology Stability Analysis (w/effects of Ro) 1/ & Aol Test Loop Gain Test Transient Test Small Signal BW for Current Control
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40 Non-Inverting V-I Floating Load IOUT = VP / RS IOUT = {(R2*VIN) / (R1A + R1B + R2)} / RS +5V 3.03A -5V -3.03A VP Op Amp Point of Feedback is VRS Op Amp Loop Gain forces +IN (VP) = -IN = VRS +1V -1V
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41 Non-Inverting V-I Floating Load R O Reflected Outside of Op Amp
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42 Non-Inverting V-I Floating Load FB#1 DC 1/ Derivation
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43 Non-Inverting V-I Floating Load FB#1 1/ Derivation
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44 Non-Inverting V-I Floating Load FB#1 1/ Data for R O No Load & Full Load I OUT RORO fz DC 1/ No Load0A 13.765 165Hz33.49dB Full Load1A 0.267 22.25Hz16.06dB
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45 OPA548 Data Sheet Aol
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46 Non-Inverting V-I Floating Load FB#1 1/ Plot for R O No Load & Full Load
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47 Non-Inverting V-I Floating Load FB#1 1/ Tina SPICE
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48 Non-Inverting V-I Floating Load FB#1 1/ Tina SPICE Results
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49 Non-Inverting V-I Floating Load FB#1 1/ Tina SPICE Results
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50 Non-Inverting V-I Floating Load FB#1 Loop Gain Tina SPICE Results
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51 Non-Inverting V-I Floating Load FB#1 Transient Analysis Tina SPICE Circuit
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52 Non-Inverting V-I Floating Load FB#1 Transient Analysis Tina SPICE Results
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53 Non-Inverting V-I Floating Load Add FB#2 and Predict 1/ Note: Load Current Control begins to roll-off in frequency where FB#2 dominates
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54 Large β Small β Answer: The largest β (smallest 1/β) will dominate! How will the two feedbacks combine?
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55 Non-Inverting V-I Floating Load FB#2 Circuit
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56 Non-Inverting V-I Floating Load FB#2 High Frequency 1/
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57 Non-Inverting V-I Floating Load FB#2 fz1
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58 Non-Inverting V-I Floating Load Tina SPICE Loop Test
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59 Non-Inverting V-I Floating Load Aol and 1/ Tina SPICE Results
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60 Non-Inverting V-I Floating Load Loop Gain Tina SPICE Results
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61 Non-Inverting V-I Floating Load I OUT /V IN AC Response Circuit
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62 Non-Inverting V-I Floating Load I OUT /V IN AC Tina SPICE Results
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63 Non-Inverting V-I Floating Load I OUT /V IN Transient Circuit
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64 Non-Inverting V-I Floating Load I OUT /V IN Transient Tina SPICE Results
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65 Inverting V-I Floating Load IOUT = {-VIN*(RF/RI)} / RS IOUT = -VIN*{RF/ (RI*RS)} +5V -3.03A -5V +3.03A Op Amp Point of Feedback is VRS Op Amp Loop Gain forces VRS = -VIN (RF/RI) -1V+1V Stability Analysis & Compensation Techniques similar to Non-Inverting V-I Floating Load
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66 Grounded Load V-I Improved Howland Current Pump Basic Topology Stability Analysis (w/effects of Ro) 1/ & Aol Test Loop Gain Test Transient Test Small Signal BW for Current Control
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67 Improved Howland Current Pump IL Accuracy Circuit RT allows for trim to optimum Z OUT and improved DC Accuracy
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68 Improved Howland Current Pump V-I DC Accuracy Calculations 1% Resistors (w/RT=0) could yield only 9% Accuracy at T=25°C Still useful for V-I control in Motors/Valves V-Torque Control Outer position feedback adjusts V for final position
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69 Improved Howland Current Pump General Equation Set RX=RF and RZ=RI
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70 Improved Howland Current Pump Simplified Equation
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71 Improved Howland AC Analysis Op Amp sees differential [(-IN) – (+IN)] feedback = - - + (Must be positive number else oscillation!) RF RI
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72 Improved Howland AC Analysis
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73 Improved Howland AC Analysis Include Effects of RO RF RI
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74 Improved Howland - Calculation
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75 Improved Howland + Calculation
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76 Improved Howland 1/ Calculation
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77 Improved Howland - Calculation RO = Full Load
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78 Improved Howland + Calculation RO = Full Load
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79 Improved Howland 1/ Calculation RO = Full Load
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80 Improved Howland 1/ Calculation No Load & Full Load ILROfzfp DC 1/ Hi-f 1/ No Load0A 6.29 75.8Hz31.83kHz17.62dB77.17dB Full Load1A 0.308 44.08Hz31.83kHz19.45dB77.15dB Change in RO from No Load to Full Load has no significant impact on the 1/ Plot
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81 OPA569 Data Sheet Aol
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82 Improved Howland 1/ Plot - Full Load
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83 Improved Howland 1/ Tina SPICE Plot - Full Load
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84 Improved Howland Loop Gain Tina SPICE Plot - Full Load
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85 Improved Howland Tina Transient Analysis Circuit RF RI
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86 Improved Howland Tina Transient Analysis Results
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87 Improved Howland Modified 1/ for Stability
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88 + FB#2 Calculation to Modify 1/ for Stability
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89 Improved Howland AC Analysis Final Design for Stability RF RI
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90 Improved Howland AC Analysis 1/ - Final Design for Stability fcl
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91 Improved Howland AC Analysis Loop Gain - Final Design for Stability fcl
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92 Improved Howland AC Transfer Analysis IL/VIN - Final Design for Stability RF RI
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93 Improved Howland AC Transfer Analysis IL/VIN - Final Design for Stability
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94 Improved Howland Transient Analysis IL/VIN - Final Design for Stability RF RI
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95 Improved Howland Transient Analysis IL/VIN - Final Design for Stability
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96 High Current V-I General Checklist Large Signal & Transient SOA Considerations (V=L*di/dt) Bipolar Output Stages & Oscillations High Current Grounding High Current PCB Traces High Current Supply Issues Power Supply Bypass (Low f & High f) Transient Protection (Supply, VIN, VOUT) Power Dissipation Considerations (see “V-I Circuits Using External Transistors” section) Consider: Short Circuit to Ground Power Dissipation Heatsink Selection Current Sense Resistor (RS) Power Dissipation
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97 V-I Large Signal Limits: V=Ldi/dt
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98 Violate the Laws of Physics and Pay the Price!
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99 Instant V-I Reversal SOA Violations
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100 Output Stages fosc > UGBW oscillates unloaded? -- no oscillates with V IN =0? -- no Some Op Amps use composite output stages, usually on the negative output, that contain local feedback paths. Under reactive loads these output stages can oscillate. The Output R-C Snubber Network lowers the high frequency gain of the output stage preventing unwanted oscillations under reactive loads. PROBLEM SOLUTION
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101 Ground Loops fosc < UGBW oscillates unloaded? -- no oscillates with V IN =0? -- yes Ground loops are created from load current flowing through parasitic resistances. If part of V OUT is fed back to Op Amp +input, positive feedback and oscillations can occur. Parasitic resistances can be made to look like a common mode input by using a “Single-Point” or “Star” ground connection. SOLUTION PROBLEM
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102 PCB Traces fosc < UGBW oscillates unloaded? -- may or may not oscillates with V IN =0? -- may or may not DO NOT route high current, low impedance output traces near high impedance input traces. DO route high current output traces adjacent to each other (on top of each other in a multi-layer PCB) to form a twisted pair for EMI cancellation.
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103 Supply Lines Load current, IL, flows through power supply resistance, Rs, due to PCB trace or wiring. Modulated supply voltages appear at Op Amp Power pins. Modulated signal couples into amplifier which relies on supply pins as AC Ground. Power supply lead inductance, Ls, interacts with a capacitive load, CL, to form an oscillatory LC, high Q, tank circuit. fosc < UGBW oscillates unloaded? -- no oscillates with V IN =0? -- may or may not PROBLEM
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104 Proper Supply Line Decouple C LF : Low Frequency Bypass 10μF / Amp Out (peak) Aluminum Electrolytic or Tantalum < 4 in (10cm) from Op Amp C HF : High Frequency Bypass 0.1μF Ceramic Directly at Op Amp Power Supply Pins R HF : Provisional Series C HF Resistance 1Ω < R HF < 10Ω Highly Inductive Supply Lines SOLUTION
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105 Transient Protection
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106 V-I Circuits Using External Transistors Choosing the Transistor Power Dissipation Considerations Traditional Floating Load Circuit Novel V-I Using Opposite Polarity Transistor
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107 Example: OPA335 and Bipolar Transistor Supply: 5V Utility Gain Buffer Output Swing: 0V to 5V Load:20ohm (250mA max) How do we choose the BJT?
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108 Bipolar Junction Transistor (BJT) NPN Base Collector Emitter PNP Base Collector Emitter
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109 Design Process for Selecting Transistor Do simple rule of thumb calculations Select device using parametric search (Digikey example) Do detailed analysis Repeat if design goals are not achieved.
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110 Simple Rule of Thumb Calculations 1.Power / Package 2.Collector Current 3.Base Current 4.Vceo (Collector to Emitter Break Down Voltage) 5.Vbe (Base to Emitter Voltage)
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111 DC Power Dissipation When is there maximum power in the output transistor? DC Signal P
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112 AC Sinusoidal Signal AC Power Dissipation When is there maximum power in the output transistor? P
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113 Maximum Power in the External Transistor Use the DC Maximum Power Dissipation for Worst Case Double the power for margin over temperature
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114 PackageMaxPower T A = 25C No heat sink MaxPower T A = 85C No heat sink MaxPower T C = 25C R θJA 1in 2 pad R θJC SOT-230.30.151400250--na-- SOT-2230.750.4317580--na-- DPAC IPAC 1.50.6520100506.25 TO-220215062.5--na--2.78 TO-34.22.210030--na--1.25 Characteristics of Different Package Types For our example
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115 TO-3 TO-220 IPAK DPAK SOT-223 SOT-23 Different Package Types
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116 1.Power / Package 2.Collector Current 3.Base Current 4.Vceo (Collector to Emitter Break Down Voltage) 5.Vbe (Base to Emitter Voltage) We’ve looked at Power. Now let’s investigate current. Simple Rule of Thumb Calculations
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117 Max Collector Current in the External Transistor The OPA335 is a “rail-to-rail” out Vout_max = Vopa_max – Vbe = 5V – 0.6V = 4.4V Max Output Current = (Vout_max)/RL =4.4V / (20Ω) = 220mA Add 20% margin Ic_max rating > (220mA)(1.5) = 330mA
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118 Maximum Base Current in the External Transistor Standard BJT Power Transistor: Typical hfe_min = 20. Base Current = Ic_max / hfe_min = 220mA / (20) = 11mA (too high) Use a Darlington. Typical minimum hfe_typ = 1000. Base Current = Ic_max / hfe_min = 220mA / (1000) = 220uA (good) Use less than 2mA for good swing to the rail. Darlington
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119 1.Power / Package 2.Collector Current 3.Base Current 4.Vceo (Collector to Emitter Break Down Voltage) 5.Vbe (Base to Emitter Voltage) Now let’s investigate voltage ratings. Simple Rule of Thumb Calculations
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120 BJT Breakdown Voltages Max voltage across any junction is 5V Most transistor breakdown > 50V Add a protection resistor in the base Limit base current Provide Capacitive Isolation
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121 Do simple rule of thumb calculations Select device using parametric search (Digikey example) Do detailed analysis Repeat if design goals are not achieved. Design Process Here is the are the results of the rule of thumb calculations Power Rating > 225mW Package Type: SOT23 Ic_max rating > 330mA Type: Darlington NPN Using Digikey parametric search Narrow from 4638 8 transistors.
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122 The result of the Digikey parametric search. We choose the least expensive one MMBT6427 @ $0.104. Parametric Search Results
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123 Do simple rule of thumb calculations Select device using parametric search (Digikey example) Do detailed analysis Repeat if design goals are not achieved. Design Process Now we verify if our choice will really work!
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124 MMBT6427 Data Sheet Look at the “Maximum Ratings” No problem -- were working with 5V. Ic_max= 220mA (lots of margin)
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125 Maximum Power / Junction Temperature Maximum power dissipation dictates device (junction) temperature Device temperature is also effected by -- Ambient temperature -- Package Type (Data specifications) -- Heat sink -- Air flow
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126 Maximum Power / Junction Temperature Power_Maximum = 112.5mW Rule of thumb: double Power_Maximum. Power_Rating > 225mW (edge of Spec) Are we ok? MMBT6427 Transistor
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127 Look at Thermal Model Thermal model with no heat sink Analogous to an electrical circuit T J = P D ( R θJA ) + T A T – is analogous to voltage R – is analogous to resistance P – is analogous to current
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128 Use the Thermal Model Assuming T A = 25 o C T J = P D ( R θJA ) + T A = (112.5mW)(556 o C/W) + 25 o C = 87.5 o C What is the maximum ambient operating temperature? Tmax_ambient = 150 o C – 62.5 o C = 87.5 o C (Enough margin?)
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129 T J = P D ( R θJC + R θCS + R θSA ) + T A P D – The power dissipation of the transistor T J – The junction temperature T C – The case temperature T S – The heat sink temperature T A – The ambient temperature Thermal Model for the Heat Sink
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130 Case R θCS R θJC R θSA Heat Sink Ambient Junction Here is the Mechanical Description
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131 T= P D ( R θJC + R θCS + R θSA ) + T A Junction to Case – R θJC Typical Transistor in a TO220 Package
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132 T= P D ( R θJC + R θCS + R θSA ) + T A Case to Sink – R θCS
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133 T= P D ( R θJC + R θCS + R θSA ) + T A Sink to Ambient – R θJC Example Heat Sink
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134 T= P D ( R θJC + R θCS + R θSA ) + T A Sink to Ambient – R θJC Natural Convection is 100 Feet /min
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135 Detailed Analysis So Far 1.Breakdown Voltages 2.Ic_max 3.Power / Junction Temperature 4.V BE / Output Swing 5.I B / Op-Amp Drive
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136 1.4V 250mA Output Swing (Consider Vbe) Vout_buffer_max = 5V – 1.4V = 3.6V Disadvantage of the Darlington Darlington MMBT6427 Transistor 1.4V
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137 Typical ΔVbe = -2mV/ o C At -25 o C ΔVbe = (-2mV/ o C)(T – Troom) ΔVbe = (-2mV/ o C)(-25 o C – 25 o C) = 0.1V Vbe = 1.4V + 0.1V = 1.5V At 85C Vbe = 1.4V - 0.12V = 1.28V Output Swing (Consider Vbe over Temperature)
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138 What’s the Real Output Swing? What’s the Real Max Current Out? Iout_max Estimate: Iout_max = Vout/RL = 5/20 = 250mA From the Graph: Vbe = 1.4V Refine Iout_max: Iout_max = (Vout – Vbe)/RL = (5 -1.4)/20 = 180mA Refine Vbe: Vbe = 1.37V 1.4V 250mA 180mA 1.37V MMBT6427 Transistor
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139 Is the Base Current Okay? Worst Case hfe = 2.7k Ib_max = Ic_max / hfe_min Ib_max = 250mA / 2700 = 92.5uA (no problem) MMBT6427 Transistor
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140 Summary of Buffer Design Using Bipolar Transistor Spec.Design Worst Case Transistor Data Sheet Rating Comment Max Current250mA500mA Max Vbe1.5VLimits the buffer output swing to 3.5V Max Ambient Temperature 87.5CDetermined using power dissipation and the thermal model. Ib – Max Base Current 92.5uA Vce5V40V Vcb540V
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141 Bipolar Junction Transistor (BJT) NPN Base Collector Emitter PNP Base Collector Emitter
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142 What about design using Power MOSFETS? N-Channel Gate Drain Source P-Channel Gate Drain Source
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143 Power MOSFET vs Power BJT Power MOSFET Voltage to Current device – no gate current Vgs depends on transistor and Id Vgs typically ranges 2V to 10V Power BJT Current to Current I device – base current significant Vbe = 0.7V for standard Vbe = 1.4V for Darlington Design process for MOSFET similar to BJT
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144 Current Sources Design Example Two Different Topologies Traditional Floating LoadInverted Transistor Floating Load 1.Easy To Stabilize 2.Headroom Limited by V BE (V GS ) 3.Bandwidth Limited By Load 1.More Difficult to Stabilize 2.More headroom than “Traditional” 3.Wider Bandwidth than “Traditional”
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145 Standard Floating Load Current Source with BJT Current Boost Vin = V G1 *1k/(1k+9k) Vin = 0.1V G1 Vrsen = Vin I_load = Vrsen/Rsen LOAD Sense Resistor + Vrsen -
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146 LOAD Sense Resistor + Vrsen - Series Resistor Limits Base Current and Isolates Op-Amp From Capacitance. Traditional Floating Load Current Source DC Analysis Asymmetrical supplies Increased output swing faster di/dt
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147 SpecDesign Worst CaseTransistor Data sheet Ib max1.5A/750 = 2mAhfe_min = 750 Op-Amp Swing25 – 1.0 = 24V @125C 25 – 1.5 = 23.5V @-25C Output Swing BJT 24 – 2.4 = 21.6V @125C 23.5 – 2.6 = 20.9V @-25C Iout Max21.6V/15 = 1.39A @125C 20.9V/15 = 1.39A @-25C Icmax=4A Pmax(25) 2 /(4*15)=10.12W--see Tj -- Ta max76.5C (Ta max> 60C) Tj @ Ta=60C=Pd(Rjc + Rjs + Rsa) + Ta =10.12W(3.13 + 0.44 + 3.7) + 60 =133C Tjmax=150C (Using heat sink) DC Analysis of Transistor BD675
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148 AC Stability Analysis Short out the signal source Add in the test circuitry
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149 Before Tina SPICE Do a Hand Analysis Find 1/β by looking at the feedback path. 1/ β = Vtest/Vfb This section is a simple buffer
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150 Before Tina SPICE Do a Hand Analysis Replace the buffer with a wire, and analyze as a series circuit.
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151 Hand Analysis of β (1/β) High and Low Frequency Extremes β Transfer Function
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152 33dB 16Hz 20dB/d ec Problem 40dB/dec rate-of- closure 1/β Curve Using Information from the Transfer Function AOL
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153 Add another feedback path to stabilize the circuit. This circuit’s 1/β plot. Using Information from the Transfer Function How will the two feedbacks combine?
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154 Large β Small β Answer: The largest β (smallest 1/β) will dominate! How will the two feedbacks combine?
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155 General Example: How would the red and blue curves add? Remember curves shown are 1/β curves, not β curves!
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156 General Example: How would the red and blue curves add? Remember that the curves shown are 1/β curves, not β Curves! The combined feedback will follow the smallest 1/β curve (the larges β).
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157 FB#2 FB#1 1decade Move the FB#2 curve up or down until there is 1 decade margin between the AOL curve and the intersection with the FB#1 curve. 1decade Set the cut frequency so that there is one decade margin before the intersection of FB#1 and FB#2. How to Select FB#2 to Stabilize the Circuit
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158 FB#2 FB#1 Stable The combination of FB#1 and FB#2 has a 20dB/decade rate-of- closure. How to Select FB#2 to Stabilize the Circuit
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159 How to Separate the Two Paths Break the FB#1 path here!
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160 Solve for β β
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161 Plot for 1/β
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162 Values Required for this Example f = 15Hz, High Freq 1/β = 50dB FB#2 FB#1 1decade f = 15Hz High freq 1/β = 50dB
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163 Using f = 15Hz, High Freq 1/β = 50dB Solve for Rd and Cf
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164 Verify Stability Using Tina-SPICE Plenty of phase margin Worst Case 45 o
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165 Look at Transient Response Using Tina-SPICE
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166 Look at Transient Response Using Tina-SPICE
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167 Phase(Iout/Vin) Mag(Iout/Vin) -3dB -45 o The AC Transfer Function Using Tina-SPICE
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168 Current Sources Design Example Two Different Topologies Traditional Floating LoadInverted Transistor Floating Load 1.Easy To Stabilize 2.Headroom Limited by V BE (V GS ) 3.Bandwidth Limited By Load 1.More Difficult to Stabilize 2.More headroom then “Traditional” 3.Wider Bandwidth then “Traditional” Done with the traditional floating load Lets look at the inverted topology.
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169 Inverted Transistor Floating Load DC Analysis Source Drain Gate Common source configuration. Vgs does not effect headroom.
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170 Inverted Transistor Floating Load DC Analysis Zener protects gate from over voltage. Resistor Isolates Op-Amp from Gate Capacitance
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171 Inverted Transistor Floating Load AC Analysis Add test circuit DC Bias Required for proper functionality
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172 Stability Analysis of Inverted Transistor Floating Load Circuit with No Compensation Note the Complex Conjugate zero (180 o phase shift). 60dB Rate of Closure
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173 Add a Zero into Feedback Path Cin MOSFET
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174 Select f=100Hz so that the zero occurs before the complex conjugate. Add a Zero into Feedback Path
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175 AC Stability Result Zero In Feedback Note: The complex conjugate zero is gone. Loop Gain=0 Phase margin < 0
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176 FB#2 Use another Feedback Path FB#2 will dominate at high frequencies
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177 Use another Feedback Path 20dB/dec 0dB
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178 Hand Calculations for New Feedback Path β
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179 20dB/dec 0dB fc = 1kHz In this example Hand Calculations for New Feedback Path
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180 FB#2 We want to set the cut frequency at about 1kHz Hand Calculations for New Feedback Path
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181 Final Compensation: Look at AC Stability
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182 Plenty of phase margin (65deg) The composite 1/β is relatively flat for all significant loop gain. Final Compensation: Look at AC Stability
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183 Final Compensation: Look at Transient
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184 Final Compensation: Look at Transient
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185 The AC Transfer Function Using Tina-SPICE
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186 Current Sources Design Example Summary Traditional Floating LoadInverted Transistor Floating Load 1.Easy To Stabilize 2.Headroom Limited by V BE (V GS ) 3.Bandwidth Limited By Load 1.More Difficult to Stabilize 2.More headroom then “Traditional” 3.Wider Bandwidth then “Traditional” For the example: Vout Swing Max = 20.9V Bandwidth = 100Hz (Bandwidth is maximized) For the example: Vout Swing Max = 24.65V Bandwidth = 800Hz (This could be compensated for wider bandwidth)
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187 High Power V-I Circuit Applications Power Packages Parallel Outputs for Higher Current V-I Using External Shunt V-I Using Internal Shunt (Burr-Brown Exclusive) Bridge Tied Load Constant Current PWM Driver
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188 Power Operational Amplifier Packages OPA569 HSOP-20 OPA567 QFN-12 5x5mm DRV104 SO-14DRV103 SO-8 OPA561 HTSSOP-20 LOG114 QFN-16 4x4mm OPA548 TO-220-7 OPA549 ZIP-11 3584 TO-3 (History) OPA548 DDPAK-7 OPA569 & OPA564 Bottom Pwr Pad OPA564 HSOP-20 Top Pwr Pad
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189 Power Operational Amplifier Packages OPA569 OPA567 QFN 12-pin Chip Cap QFN-28-pin SON-8-pin SSOP 20-pin
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190 Power Amplifier OPA567, 569, 561 & DRV103, 104 Adapter Boards Available From Tucson OPA567 OPA569 Here’s 2 of Them
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191 Paralleling Outputs for More Drive Current Power Op Amps
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192 OPA548 Power Op Amp Application Paralleling for More Output Current +8V to 60V Total Supply NOTES: (1) Works well for G 10. Gains (resistor ratios) of the two amplifiers should be carefully matched to ensure equal current sharing. (2) As configured (ILIM connected to V–) output current limit is set to 10A (peak). Each amplifier is limited to 5A (peak). Other current limit values may be obtained, see Figure 3, “Adjustable Current Limit”. 3A cont 6A continuous Output Swing to Rail Spec with 3A Load (V+) – 4.1V (V–) + 3.7V
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193 OPA569 Power Op Amp Application Paralleling for More Output Current Vos is Averaged and BW, SR are That of One Amplifier +2.7V to 5.5V Total Supply 2A cont Output Swing to Rail with 2A Load (V+) – 0.3V (V–) + 0.3V 4A continuous
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194 Bridge Tied Load for Floating Output Power Op Amps
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195 OPA549 Power Op Amp Application Bridge => 2x Voltage & 4x Power Out VTEC = 14V Won’t Swing Very Close to Supply Rail but Drives 8A Out +24V 5V High Power TEC, up to 8A Output Swing to Rail with 8A Load (V+) – 4.8V (V–) + 4.6V +24V 5V Neil Albaugh Circuit Simulation Physical Contact With a Circuit
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196 OPA569 Power Op Amp Application Bridge => 2x Voltage & 4x Power Out Can be 3V Usually +2.5V Output Needs to Swing Close to Supply Rail Only IC in Industry That Does This!!! 300mV Physical Contact With a Circuit Can be 3V High Power TEC, up to 2A
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197 Feedback using External Shunt Resistor Designing Power Current Sources
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198 OPA541 Power Op Amp Application Howland Power Current Source Transfer Function 500mA out per 10V in = 50mA per Volt RS 1Ω Rtrim 1Ω I V RL
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199 OPA541 Power Op Amp Application Howland Power Current Source Transfer Function 600mA out per 10V in = 60mA per Volt
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200 OPA541 Power Op Amp Application Howland Power Current Source
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201 OPA569 Power Op Amp Application -5V Single Supply with +Vin Constant Current Using Ext I SHUNT Feedback Grounded Anode
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202 OPA569 Power Op Amp Application -5V Single Supply with +Vin Grounded Anode LED Driver Scope Photo +1V 0V -1.25V -2. 25V LED On LED Off 0V Minus Voltage Plus Voltage
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203 OPA569 Power Op Amp Application -5V Single Supply with +Vin Grounded Anode LED Driver Scope Photo LED On LED Off 40 sec Fall 50 sec Fall Minus Voltage +1V 0V -1.25V -2. 25V 0V Plus Voltage
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204 OPA569 Power Op Amp Application -5V Single Supply with +Vin Grounded Anode LED Driver Scope Photo LED Off LED On 15msec Rise Slow 100 sec Rise Minus Voltage +1V 0V -1.25V -2. 25V 0V Plus Voltage
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205 OPA569 Power Op Amp Application -5V Single Supply with +Vin Grounded Anode LED Driver Scope Photo LED On LED Off 12 sec Fall Minus Voltage +1V 0V -1.25V -2. 25V 0V Plus Voltage
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206 OPA569 Power Op Amp Application -5V Single Supply with +Vin Grounded Anode LED Driver Scope Photo LED Off LED On 1.5msec Rise Slow 12 sec Rise Minus Voltage +1V 0V -1.25V -2. 25V 0V Plus Voltage
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207 OPA569 Power Op Amp Application -5V Single Supply with +Vin Grounded Anode LED Driver Scope Photo LED Off LED On Minus Voltage +1V 0V -1.25V -2.25V 0V Plus Voltage
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208 Feedback using Internal Current Monitor (Instead of External Shunt Resistor) Designing Power Current Sources
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209 OPA569 Power Op Amp Application 2.5V Bipolar Supplies with -Vin Constant Current Using I MONITOR Feedback - + Io Constant Current Vin- 4.2k Feedback Through I MONTIOR OPA569 +2.5V -2.5V R1 5 6 9 12 13 17 18 R SET 33k 350mA I MONTIOR = (1/475 x Io) 3 14 15 -2.5V +2.5V Luxeon Star-0 High Power LED on Heat Sink -2.5V +2.5V Io is Independent of changes in Rload (LED aging). Iin = 2.5V / 4.2k = 0.6mA Vo pin Io = Iin x 475 Io = (Vin / Rin) x 475 = 285mA Grounded Cathode
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210 OPA569 Power Op Amp Application 2.5V Bipolar Supplies with -Vin Grounded Cathode LED Driver LED On LED Off +2.5V -2.5V +2.5V -2.5V +2.5V -2.5V Scope Photo
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211 OPA569 Power Op Amp Application 2.5V Bipolar Supplies with -Vin Grounded Cathode LED Driver LED On LED Off +2.5V -2.5V +2.5V -2.5V +2.5V -2.5V Scope Photo
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212 OPA569 Power Op Amp Application +5V Single Supply with +Vin Constant Current Using I MONITOR Feedback - + Io Constant Current Vin- 4.2k Feedback Through I MONTIOR OPA569 +5V R1 5 6 9 12 13 17 18 R SET 33k 350mA I MONTIOR = (1/475 x Io) 3 14 15 0V +5V Luxeon Star-0 High Power LED on Heat Sink 0V +2.5V Io is Independent of changes in Rload (LED aging) and +5V. Iin = +2.5V / 4.2k = +0.6mA Io = Iin x 475 Io = (Vin / Rin) x 475 = 285mA Vo pin +5V Use REF3025 to make independent of +5V. +2.5V +5V 0V +2.5V 1,500pF Vout V LED 10k +5V to Anode
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213 OPA569 Power Op Amp Application +5V Single Supply with +Vin +5V to Anode LED Driver Scope Photo +5V 0V +5V 0V +2.5V +5V 0V +2.5V LED On LED Off
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214 OPA569 Power Op Amp Application +5V Single Supply with +Vin +5V to Anode LED Driver LED On LED Off Scope Photo +5V 0V +5V 0V +2.5V +5V 0V +2.5V
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215 OPA569 Power Op Amp Application +5V Single Supply with +Vin +5V to Anode LED Driver LED Off LED On Scope Photo +5V 0V +5V 0V +2.5V +5V 0V +2.5V 15 sec Fall 35 sec Delay Charging Internal Gate Cap 25 sec Fall
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216 OPA569 Power Op Amp Application +5V Single Supply with +Vin +5V to Anode LED Driver LED On LED Off Scope Photo +5V 0V +5V 0V +2.5V +5V 0V +2.5V 5 sec Rise 4 sec Rise
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217 OPA569 Power Op Amp Application +5V Single Supply with +Vin +5V to Anode LED Driver Scope Photo +5V 0V +5V 0V +2.5V +3.6V 0V +2.5V LED On LED Off +5V
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218 OPA569 Power Op Amp Application +5V Single Supply with +Vin +5V to Anode LED Driver Scope Photo +5V 0V +5V 0V +2.5V +3.6V 0V +2.5V LED On LED Off +5V
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219 OPA569 Power Op Amp Application +5V Single Supply with +Vin +5V to Anode LED Driver Scope Photo +5V 0V +5V 0V +2.5V +3.6V 0V +2.5V LED On LED Off +2.5V
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220 OPA569 Power Op Amp Application +5V Single Supply with +Vin Constant Current Using I MONITOR Feedback - + Io Constant Current Vin+ 4.2k Feedback Through I MONTIOR OPA569 +5V R1 5 6 9 12 13 17 18 R SET 33k 350mA I MONTIOR = (1/475 x Io) 3 14 15 +0.25V +2.75V Luxeon Star-0 High Power LED on Heat Sink Io is Independent of changes in Rload (LED aging) and +5V. Iin = +2.5V / 4.2k = +0.6mA Io = Iin x 475 Io = (Vin / Rin) x 475 = 285mA Vo pin 0V +2.5V 1,500pF Vout +0.25V +0.25V offset is used to maintain min voltage on I MONITOR Current Source Grounded Cathode
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221 OPA569 Power Op Amp Application +5V Single Supply with +Vin Grounded Cathode LED Driver Scope Photo +5V 0V +2.8V 0V +2.5V LED On LED Off
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222 OPA569 Power Op Amp Application +5V Single Supply with +Vin Grounded Cathode LED Driver Scope Photo +5V 0V +2.8V 0V +2.5V LED On LED Off +2.5V
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223 OPA569 Power Op Amp Application +5V Single Supply with +Vin Grounded Cathode LED Driver Scope Capture 0V +2.5V 0V +2.5V LED On LED Off 0V +2.5V Very Clean, Cf = 33,000pF Clean (small overshoot), Cf = 1,500pF Oscillation (333kHz, 0.64Vp-p), Cf = 0 pF V: 0.2V / small div T: 0.5us / small div 3us per cycle => 333kHz Loop Instability Stable 0.64Vp-p
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224 OPA569 Power Op Amp Application +5V Single Supply with +Vin Grounded Cathode LED Driver Scope Photo +5V 0V +2.8V 0V +2.5V LED On LED Off +2.5V 5 sec Fall
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225 OPA569 Power Op Amp Application +5V Single Supply with +Vin Grounded Cathode LED Driver Scope Photo +5V 0V +2.8V 0V +2.5V LED On LED Off +2.5V 12 sec Delay Charging Internal Gate Cap 12 sec Rise
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226 OPA569 Power Op Amp Application +5V Single Supply with +Vin Grounded Cathode LED Driver Scope Photo +5V 0V +2.8V 0V +2.5V LED On LED Off +2.5V
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227 OPA569 Power Op Amp Application +5V Single Supply with +Vin Grounded Cathode LED Driver Scope Photo +5V 0V +2.8V 0V +2.5V LED On LED Off +2.5V
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228 Feedback using Internal Current Monitor (Instead of External Shunt Resistor) Designing Power Current Sources
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229 OPA569 Power Op Amp Application +5V Single Supply, Current Source Tina Simulation
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230 OPA569 Power Op Amp Application +5V Single Supply, Current Source Tina Simulation
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231 OPA569 Power Op Amp Application +5V Single Supply, Current Source Tina Simulation
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232 OPA569 Power Op Amp Application +5V Single Supply, Current Source Tina Simulation
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233 Voltage Source Drive Designing Power Voltage Sources Tina Simulations
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234 OPA569 Power Op Amp Application +5V Single Supply, Voltage Source Tina Simulation
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235 OPA569 Power Op Amp Application +5V Single Supply, Voltage Source Tina Simulation
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236 OPA569 Power Op Amp Application +5V Single Supply, Voltage Source Tina Simulation
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237 Bridge Tied Load for Floating Output With Constant Current Source Power Op Amps
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238 OPA551 Power Op Amp Application 24V Single Supply, Current Source
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239 OPA551 Power Op Amp Application 24V Single Supply, Current Source
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240 OPA551 Power Op Amp Application 24V Single Supply, Current Source
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241 OPA551 Power Op Amp Application 24V Single Supply, Current Source
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242 OPA725 + Power Transistors Power Op Amp Application 5V Single Supply, Current Source
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243 OPA725 + Power Transistors Power Op Amp Application 5V Single Supply, Current Source
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244 OPA725 + Power Transistors Power Op Amp Application 5V Single Supply, Current Source
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245 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Resistive Load
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246 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Resistive Load
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247 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Resistive Load
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248 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Resistive Load
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249 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Resistive Load
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250 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Resistive Load
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251 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Inductive Load
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252 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Inductive Load
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253 OPA569 Power Op Amp Application +5V Single Supply, Bridge Current Source Tina Simulation Inductive Load
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254 DRV103 / DRV104 Low or Hi PWM Drivers PWM Constant Output Current Application
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255 Up to 3A Out SO-8 PowerPad 8V-40V - + - + V Delay VrefOsc PWM 0.1Ω Load 5.2Ω 9mH INA139 OPA340 2.2nF 10K 2.2nF 191K 100K NC Iset 1A/V Input 5V DRV103 6 5 4132 8 DRV103 Constant Current PWM Driver Low-side Switch DMOS Power Transistor
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256 DRV103 Constant Current PWM Driver
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257 Up to 1.5A peak SO-8 PowerPad 8V-32V DMOS Power Transistor - + - + V Delay VrefOsc PWM Load 5.2Ω 9mH INA139 OPA340 2.2nF 10K 2.2nF 191K 100K NC Iset 0.5A/V Input 5V 470pF 0.2Ω DRV104 10 8,9 5 6,7 11 132 14 DRV104 Constant Current PWM Driver High- side Switch
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258 DRV104 Constant Current PWM Driver
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259 The End… Or Just the Beginning of High Current V-I Circuits? John Brown 520-746-7348 brown_john@ti.com Tim Green 520-746-7780 green_tim@ti.com Art Kay 520-746-6072 kay_art@ti.com Tina SPICE www.designsoftware.com
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