1 / 19

CHAPTER 10

CHAPTER 10. Op-Amp Limitations. OBJECTIVES. Describe and Analyze: Input bias currents Input offset current Input offset voltage Frequency response Slew rate limitations Troubleshooting. Introduction. Ideal op-amps have no limitations, but real ones do:

cailin-miles
Download Presentation

CHAPTER 10

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. CHAPTER 10 Op-Amp Limitations

  2. OBJECTIVES Describe and Analyze: • Input bias currents • Input offset current • Input offset voltage • Frequency response • Slew rate limitations • Troubleshooting

  3. Introduction Ideal op-amps have no limitations, but real ones do: • Small bias currents flow into (or out of) both inputs • The two bias currents are not exactly the same • The differential-pair transistors at the input are not perfectly matched, causing an input offset voltage • The bandwidth is not infinite

  4. Input Bias Current: IIB Op-amps made with BJTs have a very small base current that flows into the input pins (for NPNs) or out of the inputs (for PNPs) on the order of nA • Op-amps made with JFET front-ends have bias currents on the order of pA • Input bias current must be considered when there are large resistor values (RS) in series with the inputs: VDROP = RS IIB • That VDROP looks like an input signal if it occurs on one input but not the other

  5. Input Bias Current Equal resistance in series with both inputs cancels almost all the VDROP caused by IIB

  6. Input Offset Current: IIO Let IIB+ be the bias current for the (+) input and let IIB- be the bias current for the (-) input. Then the input offset current is: IIO = | IIB+ | - | IIB- | Even if the resistances (RS) in series with the inputs are perfectly matched, there will be a voltage, call it VIS, that will look like an input signal: VIS = RS IIO IIO for a modern bipolar op-amps can be picoAmps To minimize VIS, use an op-amp with low IIO

  7. Input Offset Voltage: VIO Input offset voltage comes from the slight mismatch between transistors in the differential pair at the front end of an op-amp. JFET op-amps can have more input offset than bipolar op-amps. Input offset voltage for bipolar op-amps can be in the range of milliVolts for old clunkers like the 741, to microVolts, even down to nanoVolts for newer ones like the LT1112.

  8. Offset Compensation In production, it’s cheaper to buy a better op-amp than to buy a 10-turn pot and pay someone to adjust it

  9. Output Voltage Swing: VO Once VO hits the voltage rails, it clips

  10. Output Voltage Swing Clipping also occurs if output current is too high

  11. Bandwidth Above a certain frequency, the op-amp’s gain drops

  12. Bode Plots: Gain vs. Frequency Bode plots show gain vs. frequency characteristics

  13. Bode Plots • The vertical axis (Y-axis) shows gain in dB. dB of gain is defined to be: dB = 20  Log(f) • The horizontal axis (X-axis) shows the log of frequency. • A decade is a frequency change of 10 to 1. On a Bode plot, the decades are evenly spaced. • The “roll-off” is how fast the gain drops as frequency increases. A typical roll-off is 20dB per decade. • The frequency where the op-amp’s open-loop gain (AOL) falls to 0dB (AV = 1) is called the “unity-gain bandwidth” (UGB) or the “gain-bandwidth product” (GBW)

  14. Bandwidth: ACL& AOL • The closed-loop gain (ACL) of an op-amp circuit is typically much less than the open-loop gain (AOL). • On a Bode plot, ACL is a horizontal line. • At some frequency, call it fB, the horizontal ACL line intersects the roll-off of AOL. • The frequency fB is the bandwidth of the closed-loop circuit. • The intersection point is called the “3dB point” since at that frequency ACL will be down by 3dB.

  15. Bandwidth Example of the bandwidth of a closed-loop gain

  16. Slew-Rate (SR) • The “slew-rate” of an op-amp is the maximum rate of change of VOUT: SR = VOUT / t • To keep bias currents low, the internal currents in an op-amp are limited. Also inside the op-amp is a a few picoFarads of capacitance. • The time it takes to charge or discharge a capacitor depends on the current: t = (C/I)V • So with C and I fixed, the slew rate is also fixed. It’s a parameter on the op-amp’s data sheet in volts per microsecond (V / s)

  17. Slew-Rate a slew-rate of 1V / s (not high, but better than a 741)

  18. Slew-Rate An op-amp’s slew-rate (SR) limits the range of sinewave signals it will amplify: fMAX = SR  106 / 2 VP) where SR is in Volts/s,and VP is the peak amplitude of the sinewave on the output. The equation says we can use higher frequencies if we keep the amplitude low, or we can have higher amplitudes if we keep the frequency low.

  19. Troubleshooting • As always, check to see if DC voltages are within the correct range. • If an op-amp needs to be replaced, use the same part number if possible. • An op-amp with better specs can usually replace a unit with worse specs (almost anything is better than a 741). But be careful: if the new op-amp has a much higher bandwidth than the original, the circuit might oscillate. • If bread-boarding a new circuit, estimate the parameter values you need for the circuit (slew rate, input offset voltage, etc) and compare them to the op-amp’s data sheet.

More Related