Characterizing Bias Current Spikes

Slides:



Advertisements
Similar presentations
Lecture 2 Operational Amplifiers
Advertisements

Noise.
CHAPTER 3: SPECIAL PURPOSE OP-AMP CIRCUITS
Common Emitter Amplifier. Design Rules V RE should be > 100 mV.
BIOPOTENTIAL AMPLIFIERS
Analog Basics Workshop RFI/EMI Rejection
Electronic Devices Ninth Edition Floyd Chapter 10.
Voltage-Series Feedback
TI Information – Selective Disclosure 1 Characterizing Bias Current Spikes A wideband transimpedance amplifier was used to directly view the input current.
Wien-Bridge Oscillator Circuits. Why Look At the Wien-Bridge? It generates an oscillatory output signal without having any input source.
Announcements Troubles with Assignments… –Assignments are 20% of the final grade –Exam questions very similar (30%) Deadline extended to 5pm Fridays, if.
Lecture 31 Electrical Instrumentation. Lecture 32 Electrical Instrumentation Electrical instrumentation is the process of acquiring data about one or.
Lecture161 Instrumentation Prof. Phillips March 14, 2003.
Chapter 13: Operational Amplifiers
Instrumentation Amplifier
Introduction to Op Amps
Announcements Assignment 3 due now, or by tomorrow 5pm in my mailbox Assignment 4 posted, due next week –Thursday in class, or Friday 5pm in my mailbox.
Introduction to Op Amp Circuits ELEC 121. April 2004ELEC 121 Op Amps2 Basic Op-Amp The op-amp is a differential amplifier with a very high open loop gain.
Solving Op Amp Stability Issues Part 1
Part B-5 OSCILLATORS: Condition for oscillations. RC-phase oscillator with transistor and FET, Hartley and colpitts oscillators, Wien bridge oscillator,
Analogue Electronics II EMT 212/4
OSCILLATORS.
EKT314/4 Electronic Instrumentation
Conducted Emissions and Susceptibility Conducted emissions are simpler to investigate than radiated emissions because only the product’s power cord needs.
Unit-3 Tuned Amplifiers
© 2012 Pearson Education. Upper Saddle River, NJ, All rights reserved. Electronic Devices, 9th edition Thomas L. Floyd Electronic Devices Ninth.
ECE 342 – Jose Schutt-Aine 1 ECE 342 Solid-State Devices & Circuits 18. Operational Amplifiers Jose E. Schutt-Aine Electrical & Computer Engineering University.
Biomedical Instrumentation I
Introduction to Operational Amplifiers
1 The Operational Amplifier continued The voltage follower provides unity gain, however, the output impedance is changed according to the o/p impedance.
ECG Measurement System By Nick Rose Under guidance of Dr. Jack Ou Summer 2012 Built off of Chia-Hung Chen, Shi-Gun Pan, and Peter Kinget’s design for an.
Non - Inverting Amplifier
Operational Amplifiers Op Amps – a useful building block K. El-Ayat 11.
Applications of OP-AMP. Introduction Operational amplifier using IC's is inexpensive, versatile and easy to use. For this reason they are used not only.
Lecture 2: Filters.
THERMAL NOISE ESTIMATION IN SWITCHED-CAPACITOR CIRCUITS
Variable-Frequency Response Analysis Network performance as function of frequency. Transfer function Sinusoidal Frequency Analysis Bode plots to display.
PRESENTATION ON:  Voltage Amplifier Presentation made by: GOSAI VIVEK ( )
Differential voltage-gain device that amplifies the difference between the voltages existing at its two input terminal. An instrumentation (or instrumentational)
CHAPTER 20 OPERATIONAL AMPLIFIERS (OP-AMPS). Introduction to operational amplifiers Symbol and Terminals.
1 Noise Figure Improvement using a Front End Transformer Hooman 9/9/13.
The Working Theory of an RC Coupled Amplifier in Electronics.
Electronics SL – Option C.3 HL – Option F.5. Operational Amplifier An amplifier is a device that takes a signal and makes its bigger. – An mp3 player.
TERMINATIONS Copyright F. Canavero, R. Fantino Licensed to HDT - High Design Technology.
Chapter 13 Small-Signal Modeling and Linear Amplification
Operational Amplifier
Operational amplifier
Audio Power Amplifier Detailed Design
Chapter 10: Operational Amplifiers
Feedback Xs Xi Xo + - Xf βf
Inverting and Non-inverting Op-Amp
Feedback Xs Xi Xo + - Xf βf
Basic MOS Amplifiers: DC and Low Frequency Behavior
Analogue Electronic 2 EMT 212
Subject Name: LINEAR IC’s AND APPLICATIONS Subject Code:10EC46 Prepared By: Aparna.P Department: Electronics and Communication Date: /19/2018.
Operational Amplifiers
FET Amplifiers.
OP-AMPS: basics & Inverting-amplifier
Small-Signal Modeling and Linear Amplification
Electronic Circuit-II
Industrial Electronics
Electronics: Demod + 4Q FE
Wien-Bridge Oscillator Circuits
Difference Between Voltage Amplifier and Power Amplifier
Amplifiers: A Bio amplifier is an electrophysiological device, a variation of the instrumentation amplifier, used to gather and increase the signal integrity.
Operational Amplifier (Op-Amp)-μA741
Medical electronics II
Electronic PRINCIPLES
Electronic Circuit-II
Impedance of the 2x50 to 100 ohm transformers.
Presentation transcript:

Characterizing Bias Current Spikes Device Under Test Input Current Wideband TIA A wideband transimpedance amplifier was used to directly view the input current of several chopper amplifiers

Characterizing Bias Current Spikes OPA657 OPA2188 Bias Current (IB) 2 pA 160 pA Current Noise (IN) 1.3 fA/rtHz 7 fA/rtHz Bias current spikes should be apparent above other noise sources

Input Bias Spike Measurement Equipment A shielded enclosure was used to mitigate extrinsic noise Direct connection to the oscilloscope via coax cable Spikes were viewed on a 500 MHz oscilloscope 50 Ohm input impedance DC coupling (maximize bandwidth) Averaging used to remove random noise

OPA2188 Spikes repeat at 2x the chopper clock frequency Larger spike is due to the input commutation Smaller spike is from the synchronous notch filter on the output Largest spike peaks at 850nA Total duration is ~24nS

OPA2333 Commutation frequency is much lower Different input topology Input clock spikes are now of similar magnitude to notch filter spikes Different input topology Transmission gates reduce input current spikes 70 nA peak 216 nS duration

This is not unique to TI auto-zero topologies! AD8639 1.7 uA! This is not unique to TI auto-zero topologies!

Noise Feed-Through Without proper design considerations noise from the input current spikes can appear in the output

Equivalent Schematic Input current spikes can be viewed as current sources on the inputs Input current spikes are outside the opamp bandwidth The opamp can be removed to simplify analysis Current spikes on the non-inverting input are not amplified

Contribution to Output Noise Current spikes on the inverting input are coupled to the load by the feedback network Output noise is dependant upon: Input current spike magnitude Feedback network impedance (RF and RG) Load Impedance (RLOAD)

Noise Measurement Output noise was amplified and viewed on a spectrum analyzer OPA2211 with a gain of 11 HP3588 (10Hz to 150MHz) Data collected using LabView Shielded enclosure and cables VRMS: Output voltage AV: Gain of secondary amplifier KN: Brickwall correction factor (1.056) RBW: Resolution Bandwidth

Gain Effects on Total Noise At high gains chopper noise is not a dominant noise contributor

Load Impedance Effects High load impedances can exacerbate chopper noise from input current spikes

Feedback Network Impedance Large feedback resistor values will also worsen the output noise

Output Filtering Adding an RC output filter can mitigate noise seen by high impedance loads COUT chosen to have an impedance much less than RLOAD at 2x chopping frequency ROUT chosen to maintain opamp stability with the chosen COUT

Output Filtering The corner frequency for the input current spike is actually much lower The filter now includes the feedback resistance RF Filter corner frequency can be chosen to remove noise without affecting desired signal

Output Filtering

Output Filtering Harmonics due to input current spikes are completely eliminated Autozero noise at chopping frequency is within the opamp bandwidth

Output Filtering OPA2188 Without Filtering OPA2188 With Filtering Gain: 101, RF:10k, RG:100 Ohm Oscilloscope 1MOhm input impedance is the load Input current spikes are visible above other noise sources OPA2188 With Filtering Gain: 101 RF: 10k, RG: 100 Ohm Oscilloscope 1MOhm input impedance is the load Triggering oscilloscope becomes difficult due to low noise

Comparison to Non-Autozero Amplifiers The noise level of a filtered chopper amplifier is on-par with non-chopper topologies

Minimizing Chopper Noise Effects Input current spikes are not amplified by the part Spikes on the inverting input will be coupled to the load by the feedback network Minimize feedback resistance values Reduces the voltage produced by current spikes Standard design practice for low-noise, low-drift circuits Load impedance directly contributes to the magnitude of voltage produced by the spike An RC filter is an extremely effective way to reduce output noise Corner frequency can be placed outside of the signal bandwidth Noise through the feedback network experiences a much greater attenuation