<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">CS</journal-id><journal-title-group><journal-title>Circuits and Systems</journal-title></journal-title-group><issn pub-type="epub">2153-1285</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/cs.2014.51003</article-id><article-id pub-id-type="publisher-id">CS-41936</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  New Electronically-Controllable Lossless Synthetic Floating Inductance Circuit Using Single VDCC
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>inesh</surname><given-names>Prasad</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Javed</surname><given-names>Ahmad</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Electronics and Communication Engineering, 
Maharaja Agrasen Institute of Technology, Rohini, New Delhi, India</addr-line></aff><aff id="aff1"><addr-line>Department of Electronics and Communication Engineering, Faculty of Engineering 
and Technology, Jamia Millia Islamia, New Delhi, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>dprasad@jmi.ac.in(IP)</email>;<email>javedahmade@gmail.com(JA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>01</month><year>2014</year></pub-date><volume>05</volume><issue>01</issue><fpage>13</fpage><lpage>17</lpage><history><date date-type="received"><day>November</day>	<month>8,</month>	<year>2013</year></date><date date-type="rev-recd"><day>December</day>	<month>8,</month>	<year>2013</year>	</date><date date-type="accepted"><day>December</day>	<month>15,</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   A new electronically-controllable lossless floating inductance (FI) circuit (without any matching condition) has been presented, which employs only one Voltage Differencing Current Conveyor (VDCC), one grounded capacitor and one grounded resistor. The main aim of the paper is to present a new floating inductance simulator using single active device with minimum passive components. The proposed floating inductance simulator can be electronically controllable by changing the bias current. The workability of the new presented FI circuit has been verified using SPICE simulation with TSMC CMOS 0.18 μm process parameters. 
 
</p></abstract><kwd-group><kwd>VDCC; Floating Inductance Simulation; Filters</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Although many circuits for the simulation of grounded&#160; and floating inductance using different active building blocks such as operational amplifiers [1-5], current conveyors [6-13], current feedback amplifiers [14,15], current differencing buffered amplifiers [16,17], current differencing transconductance amplifiers [18,19], operational transconductance amplifiers [20,21], operational mirrored amplifiers [<xref ref-type="bibr" rid="scirp.41936-ref22">22</xref>], voltage differencing differential input buffered amplifiers [23,24], and voltage differencing transconductance amplifier [<xref ref-type="bibr" rid="scirp.41936-ref25">25</xref>] have been reported in the literature. In [<xref ref-type="bibr" rid="scirp.41936-ref26">26</xref>], many active building blocks have been presented, and VDCC is one of them. The usefulness of recently introduced active building block “VDCC” is well-defined in [<xref ref-type="bibr" rid="scirp.41936-ref27">27</xref>]. In [<xref ref-type="bibr" rid="scirp.41936-ref27">27</xref>], the authors proposed grounded inductance simulator circuits using single VDCC and two passive components. To the best knowledge of the author, no floating inductance simulator circuit using single VDCC and two passive components has been reported in the open literature so far.</p><p>Therefore, the main objective of this paper is to propose a new circuit which employs one VDCC, one grounded capacitor and one grounded resistor to realize electronically-controllable lossless matchless FI circuit. The presented circuit has also the features like only two passive components (i.e. one grounded capacitor (as desired for IC implementation) and one grounded resistor) and low active and passive sensitivities. The validity of the presented new circuit has been verified using SPICE simulation with TSMC CMOS 0.18 μm process parameters.</p></sec><sec id="s2"><title>2. The Proposed New Configuration</title><p>The symbolic notation of recently proposed active building block, VDCC is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, where P and N are input terminals and Z, X, W<sub>P</sub> and W<sub>N </sub>are output terminals. All of the terminals exhibit high impedance, except the X terminals [<xref ref-type="bibr" rid="scirp.41936-ref27">27</xref>]. The VDCC is characterized by the Equation (1).</p><disp-formula id="scirp.41936-formula86001"><label>(1)</label><graphic position="anchor" xlink:href="3-7600310\544af51e-ab56-4814-af28-b16af3444e39.jpg"  xlink:type="simple"/></disp-formula><p>The proposed FI circuit is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>A routine circuit analysis of the new FI circuit shown in  <xref ref-type="fig" rid="fig2">Figure 2</xref> yields</p><disp-formula id="scirp.41936-formula86002"><label>(2)</label><graphic position="anchor" xlink:href="3-7600310\3dc15d1a-0168-4690-9cfc-f5cdd84c6e41.jpg"  xlink:type="simple"/></disp-formula><p>which shows that the circuit simulates a floating lossless electronically-controllable inductance with the inducbtance value given by</p><disp-formula id="scirp.41936-formula86003"><label>(3)</label><graphic position="anchor" xlink:href="3-7600310\fd1f1462-f81a-4f29-b673-a08bc99d4ce8.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Non-Ideal Analysis and Sensitivity Performance</title><p>The proposed FI circuit consisting various non-ideal parasitics is shown in  <xref ref-type="fig" rid="fig3">Figure 3</xref>. The X-terminal parasitic impedance consisting of a resistance <img src="3-7600310\5a1647e8-80b2-47d7-9294-e98741ef3350.jpg" /> in series with inductance<img src="3-7600310\212fd95c-268d-430b-8ebb-16be92a43b3d.jpg" />, the parasitic impedance at the W<sub>P</sub>-terminal consisting of a resistance <img src="3-7600310\0a9466dc-9ce5-4608-9f0a-e3f30b76111e.jpg" /> in parallel with capacitance<img src="3-7600310\14b742e0-c873-4dd2-ac85-df583bc9153b.jpg" />, the parasitic impedance at the W<sub>N</sub>- terminal consisting of a resistance <img src="3-7600310\1c976e1a-c987-4d45-8700-a85fe32369bf.jpg" /> in parallel with capacitance <img src="3-7600310\501e555a-7bf7-4e08-b04b-4e757084d5c7.jpg" /> and the parasitic impedance at the Zterminal consisting of a resistance<img src="3-7600310\3d88b172-4efd-4ce6-b1a4-b221710ab993.jpg" />.</p><p>For the circuit shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>, the input-output currents and voltages relationship is given by</p><disp-formula id="scirp.41936-formula86004"><label>(4)</label><graphic position="anchor" xlink:href="3-7600310\ccf656ba-63dd-4122-af3d-c179ed2b7759.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="3-7600310\4f63d7fa-b122-41cb-b282-8a1e2f4801bf.jpg" /></p><p>The non-ideal equivalent circuit of FI of <xref ref-type="fig" rid="fig3">Figure 3</xref> is derivable from Equation (4) and is shown in  <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><p>Where <img src="3-7600310\f148afcd-4c3c-4874-948c-223ac20cad59.jpg" /> and<img src="3-7600310\4c5ef3c7-7a36-42ad-b178-7450f5dc788d.jpg" />, <img src="3-7600310\e0d0f618-808e-432f-b1d6-76f6e4f2ae28.jpg" />, <img src="3-7600310\0b792b8a-02d9-4969-b283-a9daec71d3ee.jpg" /></p><p>The various sensitivities of L<sub>FI </sub>with respect to active and passive elements are:</p><disp-formula id="scirp.41936-formula86005"><label>(5)</label><graphic position="anchor" xlink:href="3-7600310\a2a7157f-dfe8-434f-aad8-ee62acd049e9.jpg"  xlink:type="simple"/></disp-formula><p>Thus, all the passive and active sensitivities of FI circuit are low.</p></sec><sec id="s4"><title>4. Application Examples of New FI Circuit</title><p>The workability of the proposed FI circuits are demonstrated by realizing (i) a band pass filter (BPF) (<xref ref-type="fig" rid="fig5">Figure 5</xref>) and (ii) a fourth order Butterworth low pass filter with a cutoff frequency 500 kHz was designed using the normalised proto-type shown in  <xref ref-type="fig" rid="fig6">Figure 6</xref> [<xref ref-type="bibr" rid="scirp.41936-ref15">15</xref>].</p><p>The transfer function realized by the configuration shown in <xref ref-type="fig" rid="fig5">Figure 5</xref> is given by</p><disp-formula id="scirp.41936-formula86006"><label>(6)</label><graphic position="anchor" xlink:href="3-7600310\dbb7fca8-3c2e-4bc9-81a8-c8b60db5985a.jpg"  xlink:type="simple"/></disp-formula><p>From Equation (6), it is clear that centre frequency is tunable by R<sub>2</sub>.</p><p>The performance of the proposed FI circuit was verified by SPICE simulations. The frequency response of the FI circuit was obtained by using CMOS-based VDCC [<xref ref-type="bibr" rid="scirp.41936-ref27">27</xref>]. The following values were used for FI circuit: C = 0.01 nF, g<sub>m</sub> = 277.833 μA/V, R = 10 kΩ. From the frequency response of the simulated FI circuit (<xref ref-type="fig" rid="fig7">Figure 7</xref>) it has been observed that the inductance value remains constant upto 10 MHz.</p><p>The application circuits shown in Figures 5 and 6 were also been simulated using CMOS VDCCs. The component values used were for Figures 5: C<sub>1</sub> = 0.01 nF, C<sub>2</sub> = 0.02 nF, R<sub>1</sub> = 10 kΩ, R<sub>2</sub> = 3.6 kΩ, g<sub>m</sub> = 277.833 μA/V and for  <xref ref-type="fig" rid="fig6">Figure 6</xref>: R<sub>S</sub> = R<sub>L</sub> = 1 KΩ, L<sub>1d</sub> = 0.2437 mH (g<sub>m</sub> = 277.833 μA/V, C<sub>1</sub> = 0.01 nF, R<sub>1</sub> = 6.77 kΩ), L<sub>2d</sub> = 0.5884 mH (g<sub>m</sub> = 277.833 μA/V, C<sub>2</sub> = 0.01 nF, R<sub>1</sub> = 16.225 kΩ), C<sub>1d</sub> = 0.5884 nF, C<sub>2d</sub> = 0.2437 nF (after appropriate frequency and impedance scaling). The VDCC were biased with &#177;0.9 volts D.C. power supplies with I<sub>B1</sub> = 50 μA (for g<sub>m</sub> = 277.833 μA/V). Figures 8 and 9 show the simulated band pass filter and 4<sup>th</sup>-order Butterworth filter responses respectively. A comparison of proposed FI with other published floating inductor is shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Thus, the above simulation results confirm the validity of the applications of the proposed FI circuit.</p></sec><sec id="s5"><title>5. Conclusions</title><p>A new electronically-controllable loss-less FI circuit without any matching condition has been proposed which employs one VDCC, one grounded capacitor and one grounded resistor. The proposed circuit offers the following advantageous features: 1) only two passive components i.e. one grounded capacitor (as desired for IC implementation) and one grounded resistor; 2) no matching condition; 3) fully electronically controllable (by changing bias currents); and 4) low active and passive sensitivities. 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