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Research ArticleCurrent Conveyor Based Window Comparator Circuits
Sudhanshu Maheshwari
Department of Electronics Engineering, Zakir Husain College of Engineering and Technology, Aligarh, India
Correspondence should be addressed to Sudhanshu Maheshwari; sudhanshu [email protected]
Received 6 August 2016; Accepted 29 September 2016
Academic Editor: Gorazd Stumberger
Copyright © 2016 Sudhanshu Maheshwari. This is an open access article distributed under the Creative Commons AttributionLicense, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properlycited.
This paper introduces a new window comparator circuit utilizing a new current conveyor and two diodes, operable at ±1.25V andcapable of accurately detecting the voltagewindows.Anothermodified circuitwith distinct binary levels suited for automatic controlapplications is also suggested. Exhaustive simulation results showing detection of windows, as small as 50mV and as high as 1 V, areincluded. Comparisons are further drawn with the traditional operational amplifier based circuit and the new circuit is found tobenefit from the use of current-mode active element, namely, Extra-X Current Controlled Current Conveyor.The proposed theoryis well supported through simulation results.
1. Introduction
Analog signal processing utilizing complementary metaloxide semiconductor (CMOS) building blocks has recentlybeen identified as a potential area of research, with a widevariety of applications being continuously reported basedon the assorted current-mode building blocks [1–3]. Win-dow comparators are a class of nonlinear circuits used toestablish the confinement of a signal within a specifiedvoltage range, called the “window.” There are two types ofwindow comparator circuits, namely, the one which sensesthe input signal to produce a high output for the signalconfinement within the window and the second type whichproduces a low output for the signal confinement within thewindow. The output of the circuit for the signal level fallingoutside the specified window range is “low” in the formerand “high” in the latter case. Window comparator circuitsfind wide range of applications, for instance, to monitor thebattery voltage lying within the desired range, in industrialalarms, in level detectors and controls, in digital computers,in production line-testing to sort circuits that fail to meeta specified tolerance, and so forth. The commonly usedwindow comparators are built around operational amplifiers,two in number, along with two diodes [4]. These circuitshave well-known limitations associated with the voltageoperational amplifier (opamp) based circuits, namely, finite
gain-bandwidth product, limited bandwidth, and slew rate,beside the requirement of two opamps themselves.
There is an urge to develop effective circuit designsemploying current-mode active elements in form of currentconveyors for realizing class of linear and nonlinear circuits[5–12]. For instance, a simple comparator has been realizedusing current conveyors [6]. However, to the best of author’sinvestigation, a “window comparator” is not yet reportedin literature, which employs current conveyors. This paperpresents such a circuit which employs a new current conveyorwith an extra X-stage and tuning property, namely, Extra-X Current Controlled Current Conveyor (EXCCCII). Thenew circuit unlike opamp based counterparts uses a singleactive element and exhibits higher performance features,namely, higher frequency of operation, fewer active ele-ments, and detection of both, small and large, magnitudesof voltage windows. Exhaustive study is carried out tovalidate the proposed theory through effective simulationresults.
The rest of the paper is organized in the subsequentorder as follows: Section 2 presents the actual circuit descrip-tion; Section 3 presents the results of the proposed circuit;Section 4 draws comparisons with opamp based windowdetectors; Section 5 adds to the proposed circuit by offering amodified circuit with additional features; Section 6 is devotedto the discussion on possible design of the proposal using
Hindawi Publishing CorporationAdvances in Electrical EngineeringVolume 2016, Article ID 6356203, 8 pageshttp://dx.doi.org/10.1155/2016/6356203
2 Advances in Electrical Engineering
X1 X2Y
Z1+Z2−
VDD
VSS
M16
M1
M4
M7 M8
M9 M10 M11 M12 M13 M14 M15
M2
M5M6
M3
M17 M18 M19 M20 M21 M22 M23
Io
Figure 1: CMOS circuitry for Extra-X Current Controlled Current Conveyor (EXCCCII).
X1
X2
Z1+Y
EXCCCII
D1
D2
Vin
VoutVL
VU
RL
Z2−
Io
Figure 2: Proposed window comparator circuit.
commercial ICs; and Section 7 delivers conclusion to thepaper.
2. Circuit Description
The new proposed window comparator circuit based on thenew current conveyor, given in Figure 1, is shown in Figure 2.The circuit of Figure 1 is characterized by the followingrelationship:
𝑖𝑦 = 0,
𝑉𝑥𝑖 = 𝑉𝑦 + 𝑖𝑥𝑖𝑅𝑥𝑖,
𝑖 = 1, 2,
𝑖𝑧1+ = 𝑖𝑥1,
𝑖𝑧2− = −𝑖𝑥2.
(1)
It may be noted that the currents entering or leaving both𝑋 and 𝑍 terminals are taken to be positive, for positivetype conveyors. It may be noted that current conveyors withpositive current transfer gain benefit from simpler circuitry,compared to the ones with negative current transfer gain.At the core of circuitry are the two mixed translinear loopscomprised of transistors𝑀1 to𝑀6, with intrinsic resistance𝑅𝑥𝑖 (𝑖 = 1, 2) as given below. It is worth pointing thatsaturation region is assumed for the transistors comprisingthe translinear loops. It may be noted that 𝑅𝑥1 = 𝑅𝑥2 for theused design: (𝑊/𝐿)2 = (𝑊/𝐿)3 and (𝑊/𝐿)5 = (𝑊/𝐿)6:
𝑅𝑥𝑖 =1
√8𝜇𝐶𝑜𝑥 (𝑊/𝐿) 𝐼𝑜. (2)
Theparameters in (2) refer to theMOS transistors comprisingthe translinear loop, and 𝐼𝑜 is the bias current of EXCCCII.The two currents flowing in the 𝑍 stages are given as
𝐼𝑍1+ =(𝑉in − 𝑉𝑈)
𝑅𝑥1,
𝐼𝑍2− = −(𝑉in − 𝑉𝐿)
𝑅𝑥2.
(3)
Advances in Electrical Engineering 3
The circuit output is the voltage developed across 𝑅𝐿, whichdepends on the conduction of current through either of thetwo diodes. Therefore, the output voltage can be expressed as
𝑉out = (𝐼𝑍1+ + 𝐼𝑍2−) 𝑅𝐿. (4)
Itmay be noted that either both diodes are off (making output“low”) or only one of the two diodes is on at a time (makingoutput “high”); hence the output effectively depends on onlyone of the two currents in (4). The circuit operation can bedescribed by the following expression:
(i) 𝑉𝐿 ≤ 𝑉in ≤ 𝑉𝑈 : 𝐷1, 𝐷2 both off; 𝑉out is low,
(ii) 𝑉in ≤ 𝑉𝐿 : 𝐷1 off , 𝐷2 on; 𝑉out is high,
(iii) 𝑉in ≥ 𝑉𝑈 : 𝐷1 on, 𝐷2 off ; 𝑉out is high.
(5)
Equation (5) can be interpreted as follows.For 𝑉in values lying in between 𝑉𝐿 and 𝑉𝑈, the output
remains “low,” as none of the diodes turn on in these cases.The output of the window detector is “high” for values of 𝑉inwhich are either below 𝑉𝐿 when 𝐷2 switches on or in excessto 𝑉𝑈, when𝐷1 is on.
Thus the circuit detects the window between the twothreshold levels, namely, 𝑉𝐿 and 𝑉𝑈, by providing a “low”output. If the signal deviates from this window, the outputbecomes “high.” Thus, the proposed circuit falls in thecategory of second type of window detectors, as exemplifiedin the earlier section, the one which produces a “low” outputfor the signal confinement within the “window.”
3. Simulation Results
The CMOS implementation of Extra-X Current ControlledCurrent Conveyor (EXCCCII) is used for verification of theproposed circuit with a supply voltage of ±1.25V and 0.25 𝜇mprocess parameters. The bias current 𝐼𝑜 was taken as 100 𝜇A.For diodes some important parameters used were as follows:IS = 5𝑒 − 8A, BV = 7V, IBV = 1𝑒 − 5A, 𝑀 = 0.5, CJO= 0.18 pF, and RS = 6Ω. The DC transfer characteristicsshowing the input, threshold levels (𝑉𝑈 = 0.5V,𝑉𝐿 = −0.5V),and the output are given in Figure 3. The output is foundto be “low” for the signal values within the window butbecomes “high” when the signal falls outside the window.Theinput signal along with the two threshold levels used and theoutput of the circuit are also shown in Figure 4, justifyingthe theoretical predictions. Accuracy of the circuit is furthertested by reducing the window size from 1V to 50mV (𝑉𝑈 =0.5V,𝑉𝐿 = 0.45V), and the result is shown in Figure 5, whichconfirms the assertion. Thus the circuit is good for detectingboth voltage windows as small as 50mV and as high as 1 V,a feature not exhibited in a very elegant circuit available inliterature [10].
4. Comparative Study
As far as the comparison of the proposed circuit withopamp based ones is concerned, several features are worthmentioning based on the known facts and simulation studies.
−2.0 −1.0 0 1.0 2.0
V(7)V(8)
V(14)
−2.0
0
2.0
SEL→
(V)
−2.0 −1.0 0 1.0 2.0
V(30)
−2.0
0
2.0
(V)
Vin (V)
Vin (V)
Figure 3: First plot showing input {𝑉(7)} and threshold levels{𝑉(8) = 𝑉𝑈 = 0.5V & 𝑉(14) = 𝑉𝐿 = −0.5V}; second plot showingthe output {𝑉(30)} transfer characteristics.
V(14)V(7)
V(8)
−1.0
0
1.0
SEL→
(V)
Time20𝜇s15𝜇s10𝜇s5𝜇s0 s
Time
V(30)
−2.0
0
2.0
(V)
20𝜇s15𝜇s10𝜇s5𝜇s0 s
Figure 4: First plot showing input {𝑉(7)} and thresholds {𝑉(14) =𝑉𝐿 = −0.5V; 𝑉(8) = 𝑉𝑈 = 0.5V}; second plot showing output ofproposed circuit at 100KHz.
(i) Firstly, opamp based circuit uses two opamps [4, 13]as against a single EXCCCII used in the proposedcircuit.
(ii) The tunable nature of EXCCCII allows for outputcurrent adjustment, by way of varying bias current
4 Advances in Electrical Engineering
−2.0 0 2.0
V(30)V(14)
V(8)
−1.0
0
1.0
2.0
(V)
Vin (V)
Figure 5: Transfer characteristics showing 50mV window detection {𝑉(30)} for the threshold levels {𝑉(14) = 𝑉𝐿 = 0.45V & 𝑉(8) = 𝑉𝑈 =0.5V}.
Time
V(8)
−4.0
0
4.0
SEL→
V(1)V(2)
V(6)
−1.0
0
1.0
(V)
(V)
2.0ms1.0ms0 s
Time2.0ms1.0ms0 s
(a)
−4.0
0
4.0
SEL→
−1.0
0
1.0(V
)(V
)
Time
V(8)
1.0ms0.5ms0 s
V(1)V(2)
V(6)Time
1.0ms0.5ms0 s
(b)
Figure 6: (a) Simulation result for opamp (UA741) based design of window comparator at 1 KHz: first plot showing input {𝑉(1)} and thresholdlevels {𝑉(2) = 𝑉𝑈 = 0.5V & 𝑉(6) = 𝑉𝐿 = −0.5V}; second plot showing the output {𝑉(8)}. (b) Simulation result for opamp (UA741) baseddesign of window comparator at 2 KHz: first plot showing input {𝑉(1)} and threshold levels {𝑉(2) = 𝑉𝑈 = 0.5V & 𝑉(6) = 𝑉𝐿 = −0.5V};second plot showing the output {𝑉(8)}.
(hence, 𝑅𝑥), which is not possible in opamp, due toinherent nontunable nature.
(iii) The opamp based circuit [13], simulated using UA-741 model, was found to exhibit satisfactory resultsonly for few KHz signals for the same input andthreshold levels as used for the proposed circuit,due to slew rate, as well as constant gain-bandwidthproduct limitations of opamp. On the other hand,
the proposed circuit using EXCCCII operated formuch higher frequency, namely, 100KHz, as shownin results (Figure 4).
(iv) To further consolidate the above point, results foropamp based circuit for similar input conditions areshown in Figures 6(a) and 6(b), where frequency usedis 1 KHz and 2KHz, respectively, for two sets of shownresults. Inaccuracy in detectionmay be observed even
Advances in Electrical Engineering 5
X1 X2Y Z1+ Z2+
VDD
VSS
M14 M15 M16 M17 M18 M19
M13M12M11M10M9
M8M7
M4
M5M6
M3
M2M1
Io
Figure 7: EXCCCII used for modified circuit.
for 2 KHz signal. It may be noted that supply voltagefor opamp based circuit used was ±10V; frequencyimprovement to some extent was possible at reducedsupply voltages.
(v) The detection of small size window was found to beproblematic for opamp based circuit, due to offseterrors, contrary to the proposed circuit, where 50mVwas shown to be successfully detected (Figure 5).
(vi) For the general purpose opamp, like UA741, unitygain frequency is approximately 1MHz, in contrast tothe used EXCCCII, which is found to exhibit unitygain for voltage transfer and current transfer gains inthe range of approximately 300MHz.
It has to be reemphasized that the employment of current-mode active elements is to be seen as a major cause fortransferring the designs based on traditional voltage modetechniques [2–4].
5. Modified Circuit
The proposed circuit of Figure 2 can be modified by employ-ing 𝑍2+ (positive current transfer from 𝑋2) instead of 𝑍2−(negative current transfer from 𝑋2), and the 𝐷2 polarityreversed, so as to obtain a window comparator capable of notonly detecting the desired voltage window, but also providingdistinct levels of digital outputs for out-of-window signal.Figure 7 shows the circuitry for EXCCCII with positivetransfer gain from 𝑋2 to 𝑍2+, described by the followingrelationship:
𝑖𝑦 = 0,
𝑉𝑥𝑖 = 𝑉𝑦 + 𝑖𝑥𝑖𝑅𝑥𝑖,
𝑖 = 1, 2,
𝑖𝑧1+ = 𝑖𝑥1,
𝑖𝑧2+ = 𝑖𝑥2.
(6)
6 Advances in Electrical Engineering
Vin
Vout
VU
RL
VL
Io
EXCCCIIX1
X2
Y Z1+
Z2+
D1
D2
Figure 8: Modified circuit with three output levels.
Next, the actual modified circuit for window detectionis shown in Figure 8. The circuit is characterized by thefollowing:
𝐼𝑍1+ =(𝑉in − 𝑉𝑈)
𝑅𝑥1,
𝐼𝑍2+ =(𝑉in − 𝑉𝐿)
𝑅𝑥2.
(7)
The operation of the modified circuit is summarized asfollows:
𝑉𝐿 ≤ 𝑉in ≤ 𝑉𝑈, 𝑉out = 0,
𝑉in ≥ 𝑉𝑈, 𝑉out = 𝑉𝑆,
𝑉in ≤ 𝑉𝐿, 𝑉out = −𝑉𝑆.
(8)
The output is “zero” (both diodes off) for signal con-finement within the window. The signal above 𝑉𝑈 (𝐷1 onand 𝐷2 off) causes the output to become “positive,” whereasthe signal below 𝑉𝐿 (𝐷1 off and 𝐷2 on) causes the outputto become “negative,” thus providing a means of automaticfeedback for corrective actions. Equation (8) is a result of thecircuit modification as mentioned above. For input signalswithin the window range, none of the two diodes conduct,thereby keeping the output zero. For inputs greater thanthe upper threshold (𝑉𝑈), 𝐷1 conducts, making the outputpositive (𝑉𝑆), whereas, for input signal below𝑉𝐿,𝐷2 conductsand the output becomes −𝑉𝑆. Figure 9 shows the resultsfor the modified circuit. In (8) the positive and negativeoutputs refer to the saturation levels, namely, 𝑉𝑆 and −𝑉𝑆,respectively. This aspect is clearly evident from Figure 9,where the first plot shows the input signal and the twothreshold levels, whereas the second plot shows the outputof the modified circuit. Three levels of the outputs (zero,positive, and negative) can be seen in Figure 9, as per (8).
For the sake of completeness, the proposed windowcomparator and its modified version presented in this workare further compared with the most relevant works availablein literature. It may again be emphasized that, to the bestknowledge of author, window comparator circuit has notbeen presented yet, employing current conveyor or its vari-ants [1–16]. Table 1 lists the proposed circuits’ comparisons
Time
V(30)
−2.0
0
2.0
V(14)V(7)
V(8)
−1.0
0
1.0
SEL→
200𝜇s100𝜇s0 s
Time200𝜇s100𝜇s0 s
(V)
(V)
Figure 9: First plot showing input {(𝑉(7)} and thresholds {𝑉(14) =𝑉𝐿 = −0.5V & 𝑉(8) = 𝑉𝑈 = 0.5V}; second plot showing the output{𝑉(30)} of modified circuit.
with few available circuits for this electronic function. Theuse of current-mode building block, namely, EXCCCII, alongwith the features obtained makes the proposed windowcomparator circuits a novel enrichment to the literature onthe subject.
6. Discussion on Practicality
It is worth considering the proposed circuits for their practi-cality, but for the chip count requirementsmatching the countrealizable with traditional opamps.The complexity reductionin the set-up is thus not possible, when compared to opampbased circuits, but the performance attained using current-mode active elements is well known. Thus the advantagesof employing current-mode approach are achieved. Morespecifically, the EXCCCII based circuit can be made ICcompatible using two AD-844 chips (for circuit of Figure 8)or three AD-844 chips (for circuit of Figure 2). The useof AD-844 may not result in complexity reduction, butthe advantages of employing it have been often highlightedin open literature [14–16]. However, the use of AD-844inbuilt models does serve the purpose of presenting theexpected results of the proposed circuits, when built aroundcommercially available chips. Figure 10 shows one such resultobtained using AD-844 models for the modified circuit ofFigure 8, where input (100KHz) and threshold levels (𝑉𝑈 =0.5V, 𝑉𝐿 = −0.5V) are seen in the first plot, and the secondone shows the output with three distinct levels. The nature ofresult matches well with the result obtained using EXCCCIIbased circuit of Figure 7, the differences in voltage levelsbeing attributed to the biasing voltage used. This furtherconfirms the validity of the proposals made in the paper.
Advances in Electrical Engineering 7
Table 1: Comparative features of proposed circuits with existing works.
Reference Building block used Number of diodes Accuracy ofwindow detection Supply voltage used (V)
Number of outputlevels for
out-of-window signal[4, 13] 2 opamps 2 Poor ±10 typical 1[10] 4 logic gates — Poor 3 1
Proposed (Figure 2) 1 EXCCCII 2 Good(50mV) ±1.25 1
Proposed (Figure 8) 1 EXCCCII 2 Good(50mV) ±1.25 2
V(9)
V(1)V(2)
V(10)
−1.0
0
1.0
(V)
SEL→−2.0
0
2.0
(V)
Time
0s
2𝜇s
4𝜇s
6𝜇s
8𝜇s
10𝜇s
12𝜇s
14𝜇s
16𝜇s
18𝜇s
20𝜇s
22𝜇s
24𝜇s
26𝜇s
28𝜇s
30𝜇s
Time
0s
2𝜇s
4𝜇s
6𝜇s
8𝜇s
10𝜇s
12𝜇s
14𝜇s
16𝜇s
18𝜇s
20𝜇s
22𝜇s
24𝜇s
26𝜇s
28𝜇s
30𝜇s
Figure 10: AD-844 models’ based results for the circuit of Figure 8.
Thus, the new current conveyor based circuits add to thealready available knowledge on the design and applicationsof current conveyors [15].
7. Conclusion
This paper presents a new window comparator/detectorcircuit based on a new current conveyor, namely, Extra-XCurrent Controlled Conveyor and two diodes. The circuit’sworkability is shown through good results, for detectingvoltagewindows as small as 50mVand as high as 1 V. Anothermodified circuit is further proposed which not only detectsthe desired window, but also provides binary levels of distinctpolarity, making it useful as feedback for automatic control inindustrial and commercial applications.
Competing Interests
Author declares no conflict of interests.
References
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