Chapter 6
Signal Conditioning Circuit
Signal Conditioning Circuit
Power Supplies and
Power Supplies and
Chapter 6
Signal Conditioning Circuit
Power Supplies and Amplifiers
Power Supplies and Amplifiers
6.1 An electronic instrumentation system consists of:Fig (6-1) Block Diagram Showing Components of Instrumentation Systemg ( ) g g p y
6.1.2 Power Supplies:
(1) Batteries.
(2) Line voltage power supply.
( ) g p pp y
6.1.2.1 Batteries:
(1) Less expensive (Main advantage)
(2) D ith ti (M i di d t )
(2) Decay with time (Main disadvantage)
Table (6-1) Types of Batteries Lead calcium
Ni k l d i Li hi B i
Recharger (LCR) Nickel cadmium Lithium Batteries
- Voltage ranging: 4-12 volt -Capacity: 16 VAh/lb
Storage life: 6 months at
- Cell: 1.2 volt
- Capacity: 16 VAh/Ib Rechargeable: 500 times
- Lithium Iodine OR
Lithium manganese oxide (MnO ) - Storage life: 6 months at
300°K (room temperature)
- Recharging: 500 times - Advantages: Easy to use
- Rechargeable: 500 times - Lithium manganese oxide (MnO2) - High individual cell voltage(20-30v) - Not rechargeable
- Low decay under load - Long shelf life
-High capacity (110 VAh/Ib)
6.1.2.2 Line Voltage Supply:
Main : 110 220V (Input Voltage)
6.2 Zener Diode:
When a diode is reverse biased with a large enough voltage, the diode allows a large reverse current to flow. This is called diode breakdown. For most diodes the breakdown value is at least 50 V and may extend to kilovolts. A special class of diodes is designed to exploit this characteristic. They are known as zener, avalanche, or voltage-regulator diodes. This family of diodes exhibits steep breakdown curves with well-defined breakdown voltages, thus they can maintain a nearly constant voltage over a wide range of currents as
h i fi (6 3) Thi h t i ti k th d did t f
shown in fig (6-3). This characteristic makes them good candidates for building simple voltage regulators, because they can maintain a stable DC voltage in the presence of a variable supply voltage and variable load resistance
resistance.
To properly use the zener diode in a circuit, the zener should be reverse biased with a voltage kept in excess of its breakdown or zener voltage Vz.
Using a zener diode in series with a resistor as shown in Figure 4 results in a
Using a zener diode in series with a resistor as shown in Figure.4 results in a simple circuit known as a voltage regulator. The output voltage of the circuit Vout, is maintained or regulated by the zener diode at the zener voltage Vz.
Even when the current through the zener diode changes (g g ( IZZ in the figureg (6-3), the output voltage remains relatively constant (i.e., VZ is small).
Fig. (6-3) Zener Diode Symbol and Current-voltage Relationship
The narrowness of the voltage range for a given current change is a measure of the voltage regulation of the circuit. If the input voltage and load do not change much this circuit is effective in obtaining steady and lower DC change much, this circuit is effective in obtaining steady and lower DC voltage values from a source, even if the source is not well regulated.
Since the load applied to the voltage regulator will change with time in most applications and the voltage source will - exhibit fluctuations, careful
id i b id h ff h l d l V F h
consideration must be paid to the effect on the regulated voltage VZ. For the circuit shown in Figure. 6-3, the zener current is related to the circuit voltages according to (1) R V V Iz in z
To determine how changes in current are related to changes in voltage, we take the finite differential of Equation l, which yields
The zener diode is a nonlinear circuit element, and therefore Vz is not
di l i l I H i i f l d fi d i i (2) V V2 R I Iz in
directly proportional to Iz However, it is useful to define a dynamic resistance Rd that is the slope of the zener characteristic curve at a particular operating point. This allows us to express the zener current change in terms of the zener voltage change:
Normally a manufacturer specifies the nominal zener current Izt, and the (3) d z z R V I ,
maxi-mum dynamic impedance (Rd) at the nominal zener current. In a circuit design using a zener diode the zener current must exceed IzP, otherwise the zener may operate near the "knee" of the characteristic curve where regulation is poor (i e where there is a large change in voltage with a small regulation is poor (i.e., where there is a large change in voltage with a small change in zener current).
By substituting Equation.3 into Equation. 2 and solving for Vz, we can express changes in the regulator output voltage Vout in terms of fluctuations in the source voltage Vin:
in d b z out V R R R V V (4)
Therefore, the circuit acts like a voltage divider (for a change in voltage) with the zener diode represented by its dynamic resistance at the operating current of the circuit.
of the circuit.
6.3 Zener Regulation Performance:
To determine the regulation performance of the zener diode circuit shown in Figure (6-4)(a) for a voltage source Vi whose value ranges between 20 and Figure. (6 4)(a) for a voltage source Vin whose value ranges between 20 and 30 V. For the zener diode we select a 1N4744A manufactured by National Semiconductor from the family 1N4728A to 1N4752A (having different zener voltage values).It is a 15 V, 1W zener diode. We select a value of R based on
h ifi i f hi di d
the specifications of this diode.
To limit the maximum power dissipation to less than 1W, the current through the diode must be limited to
mA V
W
Izmax 1 /15 66.7
Therefore, using Equation 1, the value for resistance R should be chosen to be at least.
The closest acceptable standard resistance value is 240 . From the manufacturer's
( )/ 30 15 /66.7 225 max max min V V I V V mA R in z z p
specifications for this zener diode, its dynamic resistance Rdis l4 at 17mA. The current IZ in this example is larger than this value, so the operating point of the zener diode is on the wellregulated portion of the characteristic curve. Using the given value for Rd in Equation 3 we can approximate the resulting output voltage range:
which is a measure of regulation of this circuit. This can be expressed as a
t f th t t lt f l ti V V V R R V V in R d d z out 30 20 0.55 240 14 14
percentage of the output voltage for a relative measure:
6.4 Effects of Load on Voltage Regulator Design:
Fi (6 4)( ) ill i l l l i i h R i l d % 7 . 3 % 100 15 55 . 0 % 100 V V V V out out
Figure (6-4)(a) illustrates a simple voltage regulator circuit where RL is a load resis-tance and Vin is an unregulated source whose value exceeds the zener voltage Vz. The purpose of this circuit is to provide a constant DC voltage Vz across the load with a corresponding constant current through the load. Providing a stable regulated voltage to a system containing digital integrated circuits is a common application.
If we assume the zener diode is ideal (i.e., its breakdown current-voltage curve is vertical), we can draw some conclusions about the regulator circuit.
Fi h l d l ill b V l h di d i bj
First, the load voltage will be Vz as long as the zener diode is subject to reverse breakdown. Therefore, the load current ILis
Fig. (6-4)(b) Zener Diode Voltage Regulator Circuit
Second the load current will be the difference between the unregulated input
Second, the load current will be the difference between the unregulated input current Ii and the zener diode current IZ:
(5)
z in L I I
L
As long as VZ is constant and the load does not change, IL remains constant.
This means that the diode current changes to absorb changes from the
unregulated source.
Third, the unregulated source current Iin is given by (6)
R V V
R is known as a current-limiting resistor since it limits the power dissipated by the zener diode. If IZ gets too large, the zener diode fails.
6.5 Zener Diode Voltage Regulator Design:
To design a regulated 15 V DC source mechatronic system, and we would like to use the voltage regulator circuit shown in Figure.(6-4). Furthermore,g g g ( ) , suppose we have access to only a poorly regulated DC source Vin whose nominal value is 24 V.
As the load RL changes, the zener current IZ increases for larger RL and decreases for smaller RL If e kno the ma im m possible load resistance decreases for smaller RL. If we know the maximum possible load resistance (assuming that the output never is an open circuit), we can size the zener diode with regard to its power dissipation character istics and select a current-limiting resistor. Combining Equations. 5 and 6 and using the maximum value of the load RLmax gives
(7) max max RL V I Iz in z
This is the largest current the zener experiences. The power dissipated by the zener diode is V (8) z L z in z z z V R V I V I P max max max
Iin is controlled by the current-limiting resistor R. Substituting Equation 7 in 8 yields
Furthermore, for this design problem, we assume that RLmax is 240 and we (9) max max 2 L z z R V Vz R Vz Vin P , g p , Lmax
wish to select a 1 W zener. Therefore,
We can no sol e for the minim m req ired c rrent limiting resistance R:
240 225 ) 15 ( 15 24 2 min V V R V V IW
We can now solve for the minimum required current-limiting resistance R:
The closest acceptable standard resistance value is
69.7
min
R
6.6 Advantages:
Zener diodes are useful in circuits where it is necessary to derive smaller regulates' voltages from a single higher-voltage source. When designing zener diode circuits, one must select appropriate current-limiting resistors given the power limitations of the diodes.
Although the zener diode voltage regulator is cheap and simple to use, it has some drawbacks: The output voltage cannot be set to a precise value, and some drawbacks: The output voltage cannot be set to a precise value, and regulation against source ripple and changes in load is limited.
6.7 Voltage Regulators:
The present chapter introduces the operation of power supply circuits built
i fil ifi d h l l (R f Ch 2 f h
using filters, rectifiers, and then voltage regulators. (Refer to Chapter 2 for the initial description of diode rectifier circuits.) Starting with an ac voltage, a steady do voltage is obtained by rectifying the ac voltage then filtering to a do level and, finally, regulating to obtain a desired fixed do voltage. The, y, g g g regulation is usually obtained from an IC voltage regulator unit, which takes a do voltage and provides a somewhat lower do voltage, which remains the same even if the input do voltage varies or the output load connected to the do
oltage changes voltage changes.
A block diagram containing the parts of a typical power supply and the voltage at various points in the unit is shown in Fig. (6-5). The ac voltage, typically 120V rms, is connected to a transformer, which steps that ac voltage down to the level for the desired do output. A diode rectifier then provides a full-wave rectified voltage that is initially filtered by a simple capacitor filter to produce a do voltage. This resulting do voltage usually has some ripple or ac voltage variation A regulator circuit can use this do input to provide a do ac voltage variation. A regulator circuit can use this do input to provide a do voltage that not only has much less ripple voltage but also remains the same do value even if the input do voltage varies somewhat or the load connected to the output do voltage changes. This voltage regulation is usually obtained using one of a number of popular voltage regulator IC units.
Figure (6-5) Block Diagram Showing Parts of a Power Supply
6.8 General Filter Considerations:
A rectifier circuit is necessary to convert a signal having zero average value
A rectifier circuit is necessary to convert a signal having zero average value into one that has a nonzero average. The output resulting from a rectifier is a pulsating do voltage and not yet suitable as a battery replacement. Such a voltage could be used in, say, a battery charger, where the average do voltage is large enough to provide a charging current for the battery. For do supply voltages, as those used in a radio, stereo system, computer, and so on, the pulsating do voltage from a rectifier is not good enough. A filter circuit is necessary to provide a steadier do voltage.
6.9 Filter Voltage Regulation and Ripple Voltage:
Before going into the details of a filter circuit, it would be appropriate to consider the usual methods of rating filter circuits so that we can compare a consider the usual methods of rating filter circuits so that we can compare a circuit's effectiveness as a filter. Figure (6-6) shows a typical filter output voltage, which will be used to define some of the signal factors the filtered output of Fig. (6-6) has a do value and some ac variation (ripple). Although a battery has essentially a constant or do output voltage the dc voltage derived battery has essentially a constant or do output voltage, the dc voltage derived from an ac source signal by rectifying and filtering will have some ac variation (ripple). The smaller the ac variation with respect to the do level, the better the filter circuit's operation.
Fi (6 6) Fitt V lt W f Sh i d d Ri l V lt Figure (6-6) Fitter Voltage Waveform Showing dc and Ripple Voltages
Consider measuring the output voltage of a filter circuit using a do voltmeter and an ac (rms) voltmeter. The dc voltmeter will read only the average or dc level of the output voltage. The ac (rms) meter will read only the rms value of the acp g ( ) y component of the output voltage (assuming the ac signal is coupled through a capacitor to block out the dc level).
Definition: Ripple Ripple voltage(rms) V rms Example (1): r= =Ripple voltage(rms) (10) Dc voltage % 100 de r V rms V p e ( ):
Using a do and ac voltmeter to measure the output signal from a filter circuit, we obtain readings of 25 V do and 1.5 V rms. Calculate the ripple of the filter output voltage. Solution: % 6 % 100 25 5 . 1 % 100 V V V rms V r de r 6.10 Voltage Regulation:
Another factor of importance in a power supply the amount the dc output voltage changes over a range of circuit operation. The voltage provided at the output under no load condition (no current drawn from the supply) is reduced output under no-load condition (no current drawn from the supply) is reduced when load current is drawn from the supply (under load). The amount the dc voltage changes between the no-load and load conditions is described by a factor called voltage regulation.
Voltage regulation : (11) no load volt Voltage - full load voltage
full load voltage
Example (2): A d lt l id 60 V h th t t i l d d Wh (12) g % 100 . . % FL FL NL V V V R V
A dc voltage supply provides 60 V when the output is unloaded. When connected to a load, the output drops to 56 V calculate the value of voltage regulation.
S l ti Solution:
Eq. (12)
If the value of full-load voltage is the same as the no-load voltage, the voltage regulation calculated is 0% which is the best expected This means that the
% 1 . 7 % 100 56 56 60 % 100 . % V V V V V V R V FL FL NL
regulation calculated is 0%, which is the best expected. This means that the supply is a perfect voltage source for which the output voltage is independent of the current drawn from the supply. The smaller the voltage regulation, the better the operation of the voltage supply circuit.
6.11 Ripple Factor of Rectified Signal:
Although the rectified voltage is not a filtered voltage, it contains a dc component and a ripple component. We will see that the full-wave rectifiedp pp p signal has a larger dc component and less ripple than the half-wave rectified voltage.
For a half-wave rectified signal, the output dc voltage is
The rms value of the ac component of the output signal can be calculated (see Appendix B) to be
Vde=0.318 Vm (13)
The percent ripple of a half-wave rectified signal can then be calculated as
Vr(rms)= 0.385 Vm (14)
For a full-wave rectified voltage the dc value is
(15) % 121 % 100 318 . 0 385 . 0 % 100 m m de r V V V rms V r
For a full wave rectified voltage the dc value is
The rms value of the ac component of the output signal can be calculated (see
Vdc = 0.636 Vm (16)
The rms value of the ac component of the output signal can be calculated (see Appendix B) to be
Vr (rmx) = 0.308 Vm (17)
(18) % 48 % 100 636 . 0 308 . 0 % 100 m m dc rms r V V V V r
In summary, a full-wave rectified signal has less ripple than a half-wave rectified signal and is thus better to apply to a filter.
6.12 Capacitor Filter:
A very popular filter circuit is the capacitor-filter circuit shown in Fig. (6-7). A capacitor is connected at the rectifier output, and a dc voltage is obtained across the capacitor Fig re (6 7) (a) sho s the o tp t oltage of a f ll a e across the capacitor. Figure (6-7) (a) shows the output voltage of a full-wave rectifier before the signal is filtered, while Fig (6-7) (b) shows the resulting waveform after the filter capacitor is connected at the rectifier output. Notice that the filtered waveform is essentially a dc voltage with some ripple (or ac variation) .
Figure ( 6-7 ) Capacitor Filter Preparation: (a) full=wave Rectifier Voltage; (b) Filtered Output Voltage
ac input, Figure (6-8)(a) shows a full-wave bridge rectifier and the outputp g ( )( ) g p waveform obtained from the circuit when connected to a load (RL). If no load were connected across the capacitor, the output waveform would ideally be a constant dc level equal in value to the peak voltage (V.) from the rectifier circuit
circuit.
However, the purpose of obtaining a dc voltage is to provide this voltage for use by various electronic circuits, which then constitute a load on the voltage supply. Since there will always be a load on the filter output we must consider this practical case in there will always be a load on the filter output, we must consider this practical case in our discussion.
6.13 Output Waveform Times:
Figure (6-8) (b) shows the waveform across a capacitor filter Time T is the time
Figure (6-8) (b) shows the waveform across a capacitor filter. Time T1 is the time during which diodes of the full-wave rectifier conduct, charging the capacitor up to the peak rectifier voltage, Vm Time T2 is the time interval during which the rectifier voltage drops below the peak voltage, and the capacitor discharges through the load. Since the charge-discharge cycle occurs for each half-cycle for a full-wave rectifier the period of charge-discharge cycle occurs for each half-cycle for a full-wave rectifier, the period of the rectified waveform is T/2, one-half the input signal frequency. The filtered voltage, as shown in Fig (6-9), shows the output waveform to have a dc level Vdc and a ripple voltage Vr (rms) as the capacitor charges and discharges. Some details of these waveforms and the circuit elements are considered next
waveforms and the circuit elements are considered next.
6.14 Ripple Voltage, Vr (RMS):
Appendix B provides the details for determining the value of the ripple
l i f h h i i Th i l l b
voltage in terms of the other circuit parameters. The ripple voltage can be calculated from (19) C R V C I fC Idc rms V dc dc r 4 . 2 41 . 2 3 4
Where Idcis in mill amperes, C is in microfarads, and RL is in kilohms.
E l (3) (19) C R C fC L 3 4 Example (3):
Calculate the ripple voltage of a full-wave rectifier with a 100- F filter capacitor connected to a load drawing 50 mA.
S l ti Solution: 6.15 Dc Voltage, Vdc: V rms V Eq r 1.2 100 ) 50 ( 7 . 2 ) ( : ) 19 .( g ,
From Appendix B, we can express the dc value of the waveform across the filter capacitor as I I 417 (20) C I V fC I V V dc m dc m dc 17 . 4 4
Where Vm is the peak rectifier voltage, Idc is the load current in mill amperes, and C is the filter capacitor in microfarads.
Example (4):
If the peak rectified voltage for the filter circuit of Example (4) is 30V, calculate the filter dc voltage.
Solution: 6 16 Filt C it Ri l V C I V V Eq dc m dc 27.9 100 ) 50 ( 17 . 4 30 71 . 4 : ) 20 .(
6.16 Filter Capacitor Ripple:
Using the definition of ripple [Eq. (10)], Eq. (19), and Eq. (20), with Vdc Vms, we can obtain the expression for the output waveform ripple of a full-wave rec-tifier and filter-capacitor circuit.p
where Id is in mill amperes C is in microfarads Vd is in volts and RL is in
% 100 4 . 2 % 100 4 . 2 % 100 ) ( C R CV I V rms V r L dc dc dc r (21)
where Idsis in mill amperes, C is in microfarads, Vdcis in volts, and RL is in kilohms.
Example (5):
Calculate the ripple of a capacitor filter for a peak rectified voltage of 30V, capacitor C = 50 F, and a load current of 50 mA.
Solution: % 3 . 4 % 100 ) 9 . 27 ( 100 ) 50 ( 4 . 2 % 100 4 . 2 : ) 21 .( d dc CV I r Eq
We could also calculate the ripple using the basic definition
) 9 . 27 ( 100 dc CV % 3 . 4 % 100 2 . 1 % 100 ) ( V rms V r r
6.17 Diode Conduction Period and Peak Diode Current:
From the previous discussion, it should be clear that larger values of
9 . 27 V Vdc
capacitance provide less ripple and higher average voltage, thereby providing better filter action. From this one might conclude that to improve the performance of a capacitor filter it is only necessary to increase the size of the filter capacitor The capacitor however also affects the peak current drawn filter capacitor. The capacitor, however, also affects the peak current drawn through the rectifying diodes, and as will be shown next, the larger the value
of the capacitor, the larger the peak current drawn through the rectifying diodes.
Recall that the diodes conduct during period T1 (see Fig.6-10), during which
Recall that the diodes conduct during period T1 (see Fig.6 10), during which time the diode must provide the necessary average current to charge the capacitor. The shorter time interval the larger the amount of the charging current. Figure (6-10) shows this relation for a half-wave rectified signal (it would be the same basic operation for full-wave).
Fi (6 10) O V l d Di d C W f
Figure (6-10) Output Voltage and Diode Current Waveforms: (a) Small C (b) Large C
Notice that for smaller values of capacitor, with T1 larger, the peak diode current is less than for larger values of filter capacitor
current is less than for larger values of filter capacitor.
Since the average current drawn from the supply must equal the average diode current during the charging period, the following relation can be used (assuming constant diode current during charge time):
From which we obtain
peak dc I T T I 1 d k I T I Where T1 = diode conduction time
T = 1/f (f = 2 X 60 for full-wave) dc peak I T I 1
Idc = average current drawn from filter
Ipeak =peak current through conducting diodes
6.18 RC Filter:
It is possible to further reduce the amount of ripple across a filter capacitor by using an additional RC filter section as shown in Fig. (6-11) the purpose of the added RC section is to pass most of the dc component while attenuating (reducing) as much of the ac component as possible.
Figure (6-11) RC Filter Stage
Rectifier output Figure (6-12) shows a full-wave rectifier with capacitor filter followed by an RC filter section The operation of the filter circuit can be followed by an RC filter section. The operation of the filter circuit can be analyzed using superposition for the do and ac components of signal.
Figure (6-12 ) Full-Wave Rectifier and RC Filter Circuit
6 19 D O i f RC Fil S i
6.19 Dc Operation of RC Filter Section:
Figure (6-13) (a) shows the dc equivalent circuit to use in analyzing the RC filter circuit of Fig. (6-13)(b) Since both capacitors are open-circuit for dc operation, the resulting output dc voltage is
dc L L dc V R R R V ,
Example (6):
Calculate the dc voltage across a 1-k load for an RC filter section (R = 120, C = 10 F). The do voltage across the initial filter capacitor is Vdc= 60 V.
Solution: Solution:
6 20 Ac Operation of RC Filter Section:
V V V R R R V Eq dc L L dc (60 ) 53.6 1000 120 1000 : ) 20 .( ,
6.20 Ac Operation of RC Filter Section:
Figure (6-14)(b) shows the ac equivalent circuit of the RC filter section. Due to the voltage-divider action of the capacitor ac impedance and the load resistor, the ac component of voltage resulting across the load is
For a full-wave rectifier with ac ripple at 120 Hz, the impedance of a (22) ) ( ) ( , rms V R X rms r V c r
capacitor can be calculated using
(23) C
Xc1.3
Example (7):
Calculate the dc and ac components of the output signal across load RL in the
i i f Fi (6 14) C l l h i l f h f
circuit of Fig.(6-14). Calculate the ripple of the output waveform.
Figure (6-14) RC Filter Circuit for Example (7)
Solution: DC Calculation: DC Calculation: AC Calculation: Th RC ti iti i d i V V k k V R R R V Eq dc L L dc 150 136.4 5 500 5 : ) 20 .( ,
The RC section capacitive impedance is
The ac component of the output voltage, calculated using Eq.(10),is 0.13 130 10 3 . 1 3 . 1 : ) 22 .( k C X Eq c p p g , g q ( ), rms V V V R X rms Vr c r (15 ) 3.9 500 130 ) ( ,
The ripple of the output waveform is then % 86 . 2 % 100 7 . 3 % 100 , V rms V r r
6.21 Discrete Transistor Voltage Regulation:
Two types of transistor voltage regulators are the series voltage regulator and the shunt voltage regulator. Each type of circuit can provide an output dc
4 . 136 , V Vdc g g yp p p
voltage that is regulated or maintained at a set value even if the input voltage varies or if the load connected to the output changes.
6 22 Series Voltage Regulation: 6.22 Series Voltage Regulation:
The basic connection of a series regulator circuit is shown in the block diagram of Fig. (6-15). The series element controls the amount of the input voltage that gets to the output. The output voltage is sampled by a circuit that provides a feedback voltage to be compared to a reference voltage.
1. If the output voltage increases, the comparator circuit provides a control signal to
cause the series control element to decrease the amount of the output voltage thereby maintaining the output voltage
maintaining the output voltage.
2. If the output voltage decreases, the comparator circuit provides a control signal to
cause the series control element to increase the amount of the output voltage. 6 23 Series Regulator Circuit:
6.23 Series Regulator Circuit:
1. A simple series regulator circuit is shown in Fig. (6-16). Transistor Q1 is the series
control element, and Zener diode DZ provides the reference voltage. The regulating operation can be described as follows:
2 If the output voltage decreases the increased base-emitter voltage causes transistor Q 2. If the output voltage decreases, the increased base-emitter voltage causes transistor Q1
to conduct more, thereby raising the output voltage- -maintaining the output constant.
3. If the output voltage increases, the decreased base-emitter voltage causes transistor Q1
to conduct less, thereby reducing the output voltage- maintaining the output constant.
Example (8):
Calculate the output voltage and Zener current in the regulator circuit of Fig.
(6 17) f R 1 k
(6-17) for RL = 1 k .
Figure (6-17) Circuit for Example (8 )
Solution: Solution: V V V V V Vo z BE 12 0.7 11.3 V V V V V VCE i o 20 11.3 8.7 mA V V V IR 36.4 220 8 220 12 20 For RL = 1 k mA Ik V R V I L o L 11.3 3 . 11 A mA I I c 11.3 226 A IB c 226 50 A mA I I Iz R a 36.4 226
6.24 Improved Series Regulator:
An improved series regulator circuit is that of Fig. (6-18). Resistors R1 and R2
t li i it Z di d D idi f lt d
act as a sampling circuit, Zener diode DZ providing a reference voltage, and transistor Q2 then controls the base current to transistor Q1 to vary the current passed by transistor Q1 to maintain the output voltage constant.
If the output voltage tries to increase, the increased voltage sampled by R1 and R2 increased voltage V2, causes the base-emitter voltage of transistor Q2 to go up
Figure (6-18) Improved Series Regulator Circuit
since VZ remains fixed). If Q2 conducts more current, less goes to the base of transistor Qt, which then passes less current to the load, reducing the output voltage thereby maintaining the output voltage constant. The opposite takes place if the output. Voltage tries to decrease, causing less current to be place if the output. Voltage tries to decrease, causing less current to be supplied to the load, to keep the voltage from decreasing.
The voltage V2 provided by sensing resistors R1 and R2 must equal the sum of the base-emitter voltage of Q2 and the Zener diode, that is,
Solving Eq. (23) for the regulated output voltage, Vo,
(24) o z BE V R R R V V V 2 1 2 2 2 Example (9): (25) 2 2 2 1 BE z o V V R R R V
What regulated output voltage is provided by the circuit of Fig (6-18) for the following circuit elements: R1 = 20 k , R2 = 30 k , and VZ = 8.3 V?
Solution:
From Eq. (24), the regulated output voltage will
6.25 Op- Amp Series Regulator:
V V V k k k Vo 8.3 0.7 15 30 30 20
6.25 Op Amp Series Regulator:
Another version of series regulator is that shown in Fig. (6-19). The op-amp compares the Zener diode reference voltage with the feedback voltage from sensing resistors Rl and R2. If the output voltage varies, the conduction of
t i t Q i t ll d t i t i th t t lt t t Th t t
transistor Q1 is con trolled to maintain the output voltage constant. The output voltage will be maintained at a value of
(26) z o V R R V 2 1 1
Figure (6-19) Op-amp Series Regulator Circuit
Example (10):
Calculate the regulated output voltage in the circuit of Fig. (6-20)
Figure (6-20) Circuit for Example (10)
6.26 Current Limiting Circuit:
One form of short-circuit or overload protection is current limiting, as shown in Fig (6-21) as load current I increases the voltage drop across the short in Fig. (6-21) as load current IL increases, the voltage drop across the short circuit sensing resistor Rsc increases. When the voltage drop across Rsc becomes large enough, it will drive Q2 on, diverting current from the base of transistor Q1, thereby reducing the load current through transistor Q1, and preventing any additional current to load R The action of components R preventing any additional current to load RL. The action of components RSV and Q2 provides limiting of the maximum load current.
Figure (6-21) Current-limiting Voltage Regulator
6.27 Fold Back Limiting:
Current limiting reduces the load voltage when the current becomes larger than the limiting value. The circuit of Fig (6-22) provides fold back limiting,
hi h d b th th t t lt d t t t t ti th l d
which reduces both the output voltage and output current protecting the load from over current, as well as protecting the regulator.
Figure (6-22) Fold back-limiting Series Regulator Circuit
Fold back limiting is provided by the additional voltage-divider network of R4 and R in the circuit of Fig (6 22) (over that of Fig) the divider circuit senses and RS in the circuit of Fig. (6-22) (over that of Fig) the divider circuit senses the voltage at the output (emitter) of Ql. When IL increases to its maximum value, the voltage across Rsc becomes large enough to drive Q2 on, thereby providing current limiting. If the load resistance is made smaller, the voltage driving Q2 on becomes less, so that IL drops when VL also drops in value-this action being fold back limiting. When the load resistance is returned to its rated value, the circuit resumes its voltage regulation action.
6.28 Shunt Voltage Regulation:
A shunt voltage regulator provides regulation by shunting current away from
h l d l h l Fi (23) h h bl k di
the load to regulate the output voltage. Figure (23) shows the block diagram of such a voltage regulator. The input unregulated voltage provides current to the load. Some of the current is pulled away by the control element to maintain the regulated output voltage across the load. If the load voltage triesg p g g to change due to a change in the load, the sampling circuit provides a feedback signal to a comparator, which then provides a control signal to vary the amount of the current shunted away from the load. As the output voltage tries to get larger for e ample the sampling circ it pro ides a feed back tries to get larger, for example, the sampling circuit provides a feed-back signal to the comparator circuit, which then provides a control signal to draw increased shunt current, providing less load current, thereby keeping the regulated voltage from rising.
6.29 Basic Transistor Shunt Regulator:
A simple shunt regulator circuit is shown in Fig. (6-24). Resistor Rs drops the
l d l b h d d h li d h
unregulated voltage by an amount that depends on the current supplied to the load, RL. The voltage across the load is set by the Zener diode and transistor base-emitter volt age.
Figure (6-24) Transistor Shunt Voltage Regulator
If the load resistance decreases, a reduced drive current to the base of Q1 results, shunting less collector current. The load current is thus larger, thereby maintaining the regulated voltage across the load. The output voltage to the load is (27) BE z V V VL
Example (11):
Determine the regulated voltage and circuit currents for the shunt regulator of Fi (6 25)
Fig (6-25).
Figure (6-25) Circuit for Example (11)
Solution: Solution:
The load voltage is For the given load,
V V V V Eq.(26): L 8.2 0.7 8.9 mA V V I L L 89 9 . 8
With the unregulated input voltage at 22 V the current through RS is
mA R I L L 100 89 mA V V R V V I i L s 109 120 9 . 8 22
so that the collector current is
Ic = Is – IL = 109mA = 20mA
(The current through the Zener and transistor base-emitter is smaller than Ic by the transistor beta )
by the transistor beta.)
6.30 Improved Shunt Regulator:
The circuit of Fig (6-26) shows an improved shunt voltage regulator circuit. The Zener diode provides a reference voltage so that the voltage across R1 senses the output voltage. As the output voltage tries to change, the current shunted by transistor Q1 is varied to maintain the output voltage constant. Transistor Q2 provides a larger base current to transistor Q1 than the circuit of Transistor Q2 provides a larger base current to transistor Q1 than the circuit of Fig.(6-26), so that the regulator handles a larger load current. The output
voltage is set by the Zener voltage and that across the two transistor base-emitters,
V V V + V + V (28)
Vo = VL = VZ + VBE2 + VBEI (28)
6.31 Shunt Voltage Regulator Using op-Amp:
Figure (6-27) shows another version of a shunt voltage regulator using an
op--l Th Z l i d h f db k
amp as voltage comparator. The Zener voltage is compared to the feedback voltage obtained from voltage divider R1 and R2 to provide the control drive current to shunt element Q1. The current through resistor Rs is thus controlled to drop a voltage across Rp g ss so that the output voltage is maintained.p g
Figure (6-27) Shunt Voltage Regulator Using op-amp
6.32 Switching Regulation:
A type of regulator circuit that is quite popular for its efficient transfer of
A type of regulator circuit that is quite popular for its efficient transfer of power to the load is the switching regulator. Basically, a switching regulator passes voltage to the load in pulses, which are then filtered to provide a smooth dc voltage: Figure (6-28) shows the basic components of such a voltage regulator. The added circuit complexity is well worth the improved operating efficiency obtained.
Figure (6-28) Block Representation of Three-Terminal Voltage Regulator
6.33 IC Voltage Regulators:
Voltage regulators comprise a class of widely used ICs. Regulator IC units contain the circuitry for reference source, comparator amplifier, control device and overload protection all in a single IC Although the internal device, and overload protection all in a single IC. Although the internal construction of the IC is somewhat different from that described for discrete voltage regulator circuits, the external operation is much the same. IC units provide regulation of either a fixed positive voltage, a fixed negative voltage, or an adjustably set voltage
or an adjustably set voltage.
A power supply can be built using a transformer connected to the ac supply line to step the ac voltage to desired amplitude, then rectifying that ac voltage, filtering with a capacitor and RC filter, if desired, and finally regulating the do voltage using an IC regulator The regulators can be selected for operation do voltage using an IC regulator. The regulators can be selected for operation with load currents from hundreds of mill amperes to tens of amperes, corresponding to power ratings from mill watts to tens of Watts.
6.34 Three-Terminal Voltage Regulators:
Figure (6-29) shows the basic connection of a three-terminal voltage regulator IC to a load The fixed voltage regulator has an unregulated do input voltage, Vi, to a load. The fixed voltage regulator has an unregulated do input voltage, Vi, applied to one input terminal, a regulated output do voltage, Vo, from a second terminal, with the third terminal connected to ground. For a selected regulator, IC device specifications list a voltage range over which the input voltage can vary to maintain a regulated output voltage over a range of load current. Theg p g g specifications also list the amount of output voltage change resulting from a change in load current (load regulation) or in input voltage (line regulation).
6.35 Fixed Positive Voltage Regulators:
Th i 78 l t id fi d l t d lt f 5 t 24 V Fi
The series 78 regulators provide fixed regulated voltages from 5 to 24 V. Figure (6-29) shows how one such IC, a 7812, is connected to provide voltage regulation with output from this unit of + 12V dc. An unregulated input voltage Vi is filtered by capacitor C1 and connected to the IC's IN terminal. The IC's OUT terminal provides a regulated + 12V which is filtered by capacitor C2 (mostly for any high provides a regulated + 12V which is filtered by capacitor C2 (mostly for any high-frequency noise).
The third IC terminal is connected to ground (GND). While the input voltage may vary over some permissible voltage range and the output load may vary
bl h l i i hi
over some acceptable range, the output voltage remains constant within specified voltage variation limits.
These limitations are spelled out in the manufacturer's specification sheets. A table of positive voltage regulator ICs is provided in Table (6-2) .p g g p ( )
Table (6-2): Positive Voltage Regulators in 7800 Series
IC Part Output Voltage(V) Minimum Vi (V)
7805 +5 7.3 7806 +6 8.3 7808 +8 10.5 7810 +10 12.5 7812 +12 14.6 7815 +15 17 7
The connection of a 7812 in a complete voltage supply is shown in the
7815 +15 17.7
7818 +18 21.0
7824 +24 27.1
connection of Fig. (6-30) the ac line voltage (120 V rms) is stepped down to 18 V rms across each half of the center-tapped transformer. A full-wave rectifier and capacitor filter then provides an unregulated dc voltage, shown as a dc voltage of about 22V with ac ripple of a few volts as input to the as a dc voltage of about 22V with ac ripple of a few volts as input to the voltage regulator. The 7812 IC then provides an output that is a regulated +12 V dc.
Figure (6-30) + 12 V Power Supply
6.36 Positive Voltage Regulator Specifications:
The specifications sheet of voltage regulators is typified by that shown in Fig. (6-31) for the group of series 7800 positive voltage regulators Some
( ) g p p g g
consideration of a few of the more important parameters should be made. Nominal output voltage Regulator 5 V 7805 5 V 7805 6 V 7806 8 V 7808 10V 7812 15V 7815
Fig (6-31) Voltage Regulator terminals
18V 7818
Absolute maximum ratings:
Input voltage 40 V
Continuous total dissipationp 2 W Operating free-air temperature range -65 to 150 C
IC 7812 Electrical Characteristics:
Table (6-3) : specification sheet data for voltage regulator ICs. 7812 Table (6 3) : specification sheet data for voltage regulator ICs. 7812
Parameter Min. Typ. Max. Units
Output voltage 11.5 12 12.5 V Input regulation 3 120 MV Ripple rejection 55 71 DB Output regulation 4 100 mV Output resistance 0.018 Dropout voltage 2.0 V Sh t i it t t t 350 A Output voltage:
Table (6 3) shows the specification for the 7812 that the output voltage is
Short-circuit output current 350 mA
Peak output current 2.2 A
Table (6-3) shows the specification for the 7812 that the output voltage is typically + 12 V but could be as low as 11.5 V or as high as 12.5 V.
Output regulation:
The output voltage regulation is seen to be typically 4 mV to a maximum of
The output voltage regulation is seen to be typically 4 mV to a maximum of 100 mV (at output currents from 0.25 to 0.75 A). This information specifies that the output voltage can typically vary only 4 mV from the rated 12 V dc.
Short-circuit output current:
The amount of current is limited to typically 0.35 A if the output were to be short-circuited (presumably by accident or by another faulty component)
short-circuited (presumably by accident or by another faulty component).
Peak output current:
While the rated maximum current is 1.5 A for this series of IC, the typical peak output current that might be drawn by a load is 2.2 A. This shows that peak output current that might be drawn by a load is 2.2 A. This shows that although the manufacturer rates the IC as capable of providing 1.5 A, one could draw somewhat more current (possibly for a short period of time).
Dropout voltage:p g
The dropout voltage, typically 2 V is the minimum amount of voltage across the input-output terminals that must be maintained if the IC is to operate as a regulator. If the input voltage drops too low or the output rises so that at least 2 V is not maintained across the IC input-output, the IC will no longerp p , g provide voltage regulation. One therefore maintains an input voltage large enough to assure that the dropout voltage is provided.
6.37 Fixed Negative Voltage Regulators:
Th i 7900 IC id ti lt l t i il t th
The series 7900 ICs provide negative voltage regulators, similar to those providing positive voltages. A list of negative voltage regulator ICs is provided in Table (4). As shown, IC regulators are available for a range of fixed negative voltages; the selected IC providing the rated output voltage as
l h i l i i i d h h i i i l
long as the input voltage is maintained greater than the minimum input value. For example, the 7912 provides an output of -12 V as long as the input to the regulator IC is more negative than -14.6 V.
TABLE (6-4): Negative Voltage Regulators in 7900 Series IC Part Output Voltage (V) Minimum Vi (V)
7905 -5 -7.3 7906 -6 -8.4 7908 -8 -10.5 7909 -9 -11.5 7912 -12 -14.6 Example (12): 7912 12 14.6 7915 -15 -17.7 7918 -18 -20.8 7924 -24 -27.1 p ( )
Draw a voltage supply using a full-wave bridge rectifier, capacitor filter, and IC regulator to provide an output of +5 V.
Solution Solution
The resulting circuit is shown in Fig. (6-32).
Example (13)
For a transformer output of 15 V and a filter capacitor of 250 F, calculate the
i i i l h d l d d i 400 A
minimum input voltage when connected to a load drawing 400 mA.
Solution:
The voltages across the filter capacitor are
241I 24(400)
Since the input swings around this do level the minimum input voltage can
V C I peak Vr 6.65 250 ) 400 ( 4 . 2 3 41 . 2 3 V V V V V Vdc m r 15 6.65 8.35
Since the input swings around this do level, the minimum input voltage can drop to as low as
Since this voltage is greater than the minimum required for the IC regulator
Iow V V peak V V V
Vi dc r 15 6.65 8.35
(from Table (6-3), Vi = 7.3 V), the IC can provide a regulated voltage to the given load.
Example (14): Example (14):
Determine the maximum value of load current at which regulation is maintained for the circuit of Fig. (6-32).
Solution:
T i t i V ( i ) 7 3 V
To maintain Vi(min) 7.3 V,
peak V V V V V
so that Th l f l d i h V V peak V rms Vr r 4.4 3 7 . 7 3 ) (
The value of load current is then
Any current above this value is too large for the circuit to maintain the
mA V C rms V Ide r 458 4 . 2 250 4 . 4 4 . 2 y g regulator output at +5 V.
6.38 Adjustable Voltage Regulators:
Voltage reg lators are also a ailable in circ it config rations that allo the
Voltage regulators are also available in circuit configurations that allow the user to set the output voltage to a desired regulated value. The LM317, for example, can be operated with the output voltage regulated at any setting over the range of voltage from 1.2 to 37 V Figure (6-33) shows how the regulated output voltage of an LM317 can be set.
Resistors R1 and R2 set the output to any desired voltage over the adjustment range (1.2 to 37 V). The output voltage desired can be calculated using.
With typical IC values of
(29) 2 1 2 1 I R R R V Vo ref adj
Figure (6-33) Connection of LM317 Adjustable-Voltage Regulator
Example (15)
D t i th l t d lt i th i it f Fi (6 33) ith R 240
Determine the regulated voltage in the circuit of Fig. (6-33) with R1 = 240 and R2=2.4k . Solution: Eq. (28): V V k A k Vo o (100 )(2.4 240 4 . 2 1 25 . 1 V V V 024 13 99 75 13 13.75V 0.24V 13.99V
Example (16):
Determine the regulated output voltage of the circuit in Fig. (6-34).
Figure (6 34) Positive Adjustable Voltage Regulator for Example (16) Figure (6-34) Positive Adjustable-Voltage Regulator for Example (16)
Solution:
The output voltage calculated using Eq. (28) is
A k V
k V
V 125 1 1.8 100 18 108
A check of the filter capacitor voltage shows that an input-output difference of 2 V can be maintained up to at least 200 mA load current.
A k V k V Vo 100 1.8 10.8 240 8 . 1 1 25 . 1
6.39 Performance Characteristics of Power Supplies:
For the range (o 40v), (o 3A)
1. Load Effect:
a) For constant voltage source: 0 01 % + 200 a) For constant voltage source: 0.01 % + 200 b) For constant current source: 0.02% + 500
Solution:
EX : If the current is 2 AMP
0022 . 0 20 10 200 20 100 01 . 0 20 6
EX2: If the current is 2 AMP
Solution: 2 So rce Effect 0045 . 0 2 10 500 2 100 02 . 0 2 6 2. Source Effect:
Source effect is the change in output for change in line voltage (input) a) Constant voltage source : 0.01 % + 200
b) Constant current source : 0.02% + 500)
3. Temperature Effect:
It is the change in the output voltage or current per degree centigrade (°C)
following the warm-up period of 30 minutes. a) Constant voltage source : 0.01 % + 200
b)Constant current source : 0.01% + 1
4 Drift Stability: 4. Drift Stability:
It is a change in the output under constant load over an 8 hours period following the 30min warm-up period is:
a) For Constant voltage source: 0.03% + 500 b)For Constant current source: 0.03% + 3
5. The output Impedance of the power supply:
Typical values of the output impedance L=1 H
r =2 m
6.40 Amplifiers:
An amplifier increases the amplitude of a signal without affecting the phase relationships of different components of the signal. When choosing or design-ing an amplifier, we must consider size, cost, power consumption,g g p , , , p p , input impedance, output impedance, gain, and bandwidth. Physical size depends on the components used to construct the amplifier.
Generally, we model an amplifier as a two-port device, with an input and output voltage referenced to ground, as illustrated in Figure.(6-35). The output voltage referenced to ground, as illustrated in Figure.(6 35). The voltage gain of an amplifier is defined as the ratio of the output and input voltage amplitudes: (30) out v V V A
Normally we want an amplifier to exhibit amplitude linearity, where the gain is constant for all frequencies. However, amplifiers may be designed to intentionally amplify only certain frequencies, resulting in a filtering effect. In
( )
in
V
intentionally amplify only certain frequencies, resulting in a filtering effect. In such cases, the output characteristics are governed by the amplifier's bandwidth and associated cutoff frequencies.
The input and output impedances of an amplifier, Zin and Zout, are found by measuring the ratio of the respective voltage and current:
For the operational amplifiers Z is larger than 100 k and Z is a few ohms (31) (32) in in in V I V / out out out V I Z /
For the operational amplifiers, Zinis larger than 100 k and Zoutis a few ohms or less.
In amplification the work inside the linear region.
6.41 The Ideal Operational Amplifier:
The schematic symbol for an ideal op amp as shown in Fig (6-3)(1). It is a
diff i l i i l lifi h i d h i fi i i
differential input, single output amplifier that is assumed to have infinite gain. The - symbol is sometimes used in the schematic to denote the infinite gain and the assumption that it is an ideal op amp. The voltages are all referenced to a common ground. The op amp is connection to an external power supply,g p p p pp y, usually plus and minus 15 V.
Fig. (6-36)(a) Op amp Terminology and Schematic Representation
Fig (6-37) Op Amp Equivalent Circuit
As illustrated in Figure.36-b an op amp circuit usually includes feedback from the output to the negative (inverting) input. This so-called closed loop configuration results in stabilization of the amplifier and control of the gain. When feedback is absent in an op amp circuit, the op amp is said to have an open loop configuration. This configuration results in considerable instability due to the infinite gain, and it is seldom used. The utility of feedback will become evident in the examples presented in the following sections.
Figure (6-37) illustrates an ideal model that can aid in analyzing circuits contain-ing op amps. This model is based on the following assumptions that describe an ideal op amp:
1. It has infinite impedance at both inputs hence no current is drawn from the
input circuits. Therefore,
2. It has infinite gain. As a consequence, the difference between the input voltages must be 0; otherwise, the output would be infinite. This is denoted in
Fi 10 b h h i f h i
Figure. 10 by the shorting of the two inputs.
V+ = V- (34)
Fig (6 38) 741 op amp pin out Fig. (6-38) 741 op amp pin-out
Therefore, Even though we indicate a short between the two inputs, we assume no current may flow through this short.
3. It has zero output impedance. Therefore, the output voltage does not depend
on the output current.
Note that Vout, V+, and V- are all referenced to a common ground. Also, for stable linear behavior there must be feedback between the output and the stable linear behavior, there must be feedback between the output and the inverting input.
We need only Kirchhoff's laws and Ohm's law to completely analyze op amp circuits. Actual op amps are usually packaged in eight-pin dual in-line
k (DIP) i d i i (IC) hi Th d i i f l
package (DIP) integrated circuit (IC) chips. The designation for a general purpose op amp produced by many IC manufacturers is 741. It is illustrated in Figure (38) with its pin configuration (pin-out). As with all ICs, one end of the chip is marked with an indentation or spot, and the pins are numberedp p , p counterclockwise and consecutively starting with 1 at the left side of the marked end. For a 741 series op amp, pin 2 is the inverting input, pin 3 is the non-inverting input, pins 4 and 7 are for the external power supply, and pin 6 is the op amp o tp t Pins l 5 and 8 are not normall connected Fig re (38) is the op amp output. Pins l, 5, and 8 are not normally connected. Figure (38) illustrates the internal design of a 741 IC available from National Semiconductor. Note that the circuits are composed of transistors, resistors, and capacitors that are easily manufactured on a single silicon chip. The most valuable details for the user are the input and output parts of the circuit having characteristics that might affect externally connected components.
6 42 Inverting Amplifier: 6.42 Inverting Amplifier:
An inverting amplifier is constructed by connecting two external resistors to an op amp as shown in Figure (6-39). As the name implies, this circuit inverts and amplifies the input voltage. Note that the resistor RF forms the feedback loop. This feedback loop always goes to the inverting input of the op amp, implying negative feedback.
We now use Kirchhoff s laws and Ohm's law to analyze this circuit. First, we replace the op amp with its ideal model shown within the dashed box in
Fi (6 40) A l i Ki hh ff' l d C d ili i
Figure (6-40). Applying Kirchhoff's current law at node C and utilizing assumption l, that no current can flow into the inputs of the op amp,
Iinin = -ioutout (35)( )
Fig (6-39) Inverting Amplifierg ( ) g p
Also, since the two inputs are assumed to be shorted in the ideal model, C is effec-tively at ground potential:
Since the voltage across resistor R is Vin – Vc = Vin from Ohm's low,
Vc= 0 (36)
g in c in, ,
And since the oltage across resistor R is V V V
Vin = iinR (37)
And since the voltage across resistor RF is Vout- Vc = Vout,
S b tit ti E ti 34 i t E ti 37 i
Vout = ioutRF (38)
Substituting Equation.34 into Equation.37 gives
Vout = iinRF (39)
Dividing Equation.38 by Equation.36 yields the input/ output relationship: (40) R R V V F in out
Fig (6-41) Illustration of Inversion
Therefore, the voltage gain of the amplifier is determined simply by the external, g g p p y y resistors RF and R, and it is always negative. The reason this circuit is called an inverting amplifier is that it reverses the polarity of the input signal. This results in a phase shift of 1800 for periodic signals. For example, if the square wave V
in. shown in
Figure (6-41) is connected to an inverting amplifier with a gain of -2, the output Voutis inverted and amplified resulting in a larger amplitude signal 180° out of phase with the inverted and amplified, resulting in a larger amplitude signal 180° out of phase with the input.
6.43 Non-inverting Amplifier:
The schematic of a non-inverting amplifier is shown in Figure (42). As the nameg p g ( ) implies, this circuit amplifies the input voltage without inverting the signal. Again, we can apply Kirchhoff s laws and Ohm's law to determine the voltage gain of this amplifier.
The voltage at node C is Vin since the inverting and non-inverting inputs are at the same voltage Therefore applying Ohm's law to resistor R
voltage. Therefore, applying Ohm's law to resistor R,
(41)
R V Iin in
and applying it to resistor RF, (42) in out V V i (42) F out R i
Fig (6-42) Noninverting Amplifier Fig (6 42) Noninverting Amplifier
Fig (6-43) Equivalent Circuit for Noninverting Amplifierg ( ) q g p
Solving Equation.41 for Vout, gives (43) in F out out i R V V
Applying KCL at node C gives Fig (43)
(43) (44) in F out out out in i i So Equation.40 can be written as
( ) (45) out in R i Vin out
Using Equations.42and 44, the voltage gain can be written as
(46) R R R i R i R i V V i V V F out out F out in in out in out 1
Therefore, the non-inverting amplifier has a positive gain greater than or equal to 1. This is useful in isolating one portion of a circuit from another by transmitting a scaled voltage without drawing appreciable current. If we let
out in
in
g g g pp
RF = 0 and R = , the resulting circuit can be represented as shown in Figure 44. This circuit is known as a buffer or follower since Vout= Vin. It has high input impedance and low output impedance. This circuit is useful in applications where you need to couple to a voltage signal without loading the source of the voltage The high input impedance of the op amp effectively source of the voltage. The high input impedance of the op amp effectively isolates the source from the rest of the circuit.
6.44 Difference Amplifier (Dual
inputs):- The difference amplifier circuit shown in Figure (6-45) is used to subtract
l i l I l i hi i i h i i l f
analog signals. In analyzing this circuit, we can use the principle of superposition, which states that, whenever multiple inputs are applied to a linear system (e.g., an op amp circuit), we can analyze the circuit and determine the response for each of the individual inputs independently.p p p y
Fig (6-45) Difference Amplifier Circuit
The sum of the individual responses is equivalent to the overall response to the multiple inputs. Specifically, when the inputs are ideal voltage sources, to
l h d h h h d If
analyze the response due to one source, the other sources are shorted. If some inputs are, current sources, they are replaced with open circuits.
The first step in analyzing the circuit in Figure (6-45) is to replace V2 with a short circuit, effectively grounding R, y g g 22. As shown in Figure. (6- 46), the resultg ( ), is an inverting amplifier.
Therefore, from Equation.(39), the output due to input V1 is
(47)
V R
V F
The second step in analyzing the circuit in Figure 45 is to replace short circuit, effectively grounding R1as shown in Figure 47a. This equivalent to
(47) 1 1 1 V R Vout 1
the circuit shown in Figure (6-20) (b) where the input voltage is since V2 is divided between resistors R2 and RF.
(48) 2 3 V R R R V F
The circuit in Figure 47b is a non-inverting amplifier. Therefore, the output due to input V2 is given by Equation. 45
( ) 2 R R F (49) 3 1 2 1 V R R Vout F
