CHAPTER 10: Op-Amp Limitations pptx

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 diffe

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:

• 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

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

Input Bias Current

Equal resistance in series with both inputs cancels

almost all the VDROP caused by IIB

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: I IO = | I IB+ | - | I IB- |

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

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

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

Output Voltage Swing: V O

Once VO hits the voltage rails, it clips

Output Voltage Swing

Clipping also occurs if output current is too high

Bandwidth

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

Bode Plots:

Gain vs Frequency

Bode plots show gain vs frequency characteristics

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)

Bandwidth: A CL & A OL

• 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

Bandwidth

Example of the bandwidth of a closed-loop gain

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)

Slew-Rate

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

Slew-Rate

An op-amp’s slew-rate (SR) limits the range of

sinewave signals it will amplify:

fMAX = SR  106 / 2  V P) 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

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