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GB2059213A - Active inductors - Google Patents

Active inductors Download PDF

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Publication number
GB2059213A
GB2059213A GB7931770A GB7931770A GB2059213A GB 2059213 A GB2059213 A GB 2059213A GB 7931770 A GB7931770 A GB 7931770A GB 7931770 A GB7931770 A GB 7931770A GB 2059213 A GB2059213 A GB 2059213A
Authority
GB
United Kingdom
Prior art keywords
active
amplifier
resistors
inductor
inductors
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
GB7931770A
Other versions
GB2059213B (en
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
STC PLC
Original Assignee
Standard Telephone and Cables PLC
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Standard Telephone and Cables PLC filed Critical Standard Telephone and Cables PLC
Priority to GB7931770A priority Critical patent/GB2059213B/en
Publication of GB2059213A publication Critical patent/GB2059213A/en
Application granted granted Critical
Publication of GB2059213B publication Critical patent/GB2059213B/en
Expired legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H11/00Networks using active elements
    • H03H11/02Multiple-port networks
    • H03H11/04Frequency selective two-port networks
    • H03H11/12Frequency selective two-port networks using amplifiers with feedback
    • H03H11/1217Frequency selective two-port networks using amplifiers with feedback using a plurality of operational amplifiers
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H11/00Networks using active elements
    • H03H11/46One-port networks
    • H03H11/48One-port networks simulating reactances
    • H03H11/485Simulating inductances using operational amplifiers

Landscapes

  • Networks Using Active Elements (AREA)

Abstract

A known active inductor of the type shown in Figure 1 can be made to have a high Q, with characteristics independent of roll-off frequency and input impedance to first order when the relationships between the resistors 2, 4 and 5 are chosen to be in the ratios 2R:R: (1 + 2ROOT 2)R respectively. Two such inductors can be connected to form a fully floating active inductor, which may be connected between two earthed inductors. <IMAGE>

Description

SPECIFICATION Active filters This invention relates to precision active filters, in particular for use in telecommunication systems.
In telecommunication systems there are requirements for high performance active filters whose performance is substantially independent of both the gain and the input impedance of the operational amplifiers used in the filter. Many designs for active filters are available from widely published handbooks.
Generally the components can readily be regarded as simple capacitors, inductors, resistors and inductive transformers.
A high performance active filter requires a high quality active inductor. One known inductor is of the type shown in Figure 1. The arrangement of Figure 1 comprises a first operational amplifier 1 to the positive input of which the input signal is applied. The output of the first amplifier 1 is coupled via a resistor 2 to the negative input of a second similar operational amplifier 3. The negative input of amplifier 1 and the positive input of amplifier 3 are connected together and are grounded through a resistor 4. The output of amplifier 1 is connected via a feedback resistor 5 to negative input of amplifier 1 and the output of amplifier 3 is connected via a feedback capacitor 6 to the negative input of amplifier 3. Finally the output of amplifier 3 is connected via a feedback resistor 7 to the positive input of amplifier 1.
According to the present invention there is provided an active inductor of the type hereinbefore referred to wherein the values of the resistors between the output of the first amplifier and the negative input of the second matching amplifier, between the output of the first amplifier and the negative input thereof, and between the negative input of the first amplifier and ground are respectively in the ratios 2R: R : (1 + V2)R, where R is given value of resistance.
The use of such values provides an inductor capable of producing a high Q, with characteristics independent of roll-off frequency and input impedance to first order, as the relationship between the passive components are suitably chosen. In this context "input impedance" refers to the active input impedance.
Clearly the input impedance of the operational amplifiers appears in parallel with the active inductor.
Embodiments of the invention will now be described with reference to the accompanying drawings, wherein: Figure 1 illustrates a high Active inductor, Figure 2 illustrates a fully floating high Q inductor, and Figure 3 illustrates an active filter incorporating a fully floating inductor.
The basic circuit of Figure 1 has already been described. To obtain optimum results the values of resistors 2,4 and 5 are 2R, Rand (1 + V2)R respectively. The inductance L is given by the formula 2(1 + V2)RTC where T is the value of resistance 7 and C is the value of capacitor 6. This circuit has optimum performance regarding sensitivity to D.C. gain and to second order effects or roll-offfrequency at particular frequencies.
The frequency for minimum sensitivity to gain is V2-1 4nRC This value also minimises the change in the inductance value due to the roll off.
The frequency for minimum second order effects of the roll off frequency is 0.306 f= 4aRC Because these frequencies are fairly close, an overall optimum will generally come at 0.36 f=~ 4nRC Thus, if a distinct resonance is desired the component values should be chosen so that the resonance tames at this frequency.
A floating inductor may be realised by taking two identical inductors according Figure 1 and connecting Giie earthed points together as shown in Figure 2.
if the values of 7 and 7' are made equal, the inductance L = 4(1 + /2)ROC. If 7 and 7' are different the arrangement of Figure 2 still looks like an inductor from both ends, but acts also as an impedance converter (this has no transformer equivalent, as power gain is involved). This can be useful where a filter requires different values on two sides of a floating inductor, and it is desired to use uniform capacitors throughout.
It may be noted that a floating inductor may readily be connected between two grounded inductors where a coupled resonator is required. Such a design is illustrated in Figure 3. It will be appreciated that the two pairs of amplifiers 1,3 and 1', 3' form the equivalent of one floating inductor, whilst amplifiers 1', 3', and 1", 3" form the equivalent of another floating inductor.

Claims (7)

1. An active inductor of the type hereinbefore referred to wherein the values of the resistors between the output of the first amplifier and the negative input of the second amplifier, between the output of the first amplifier and the negative input thereof, and between the negative input of the first amplifier and ground are respectively in the ratios 2R R: (1 + 2)R, where R is given value of resistance.
2. An active inductor arrangement including two inductors according to claim 1 connected together such that each forms a virtual ground for the other, resistors of value (1 + 0/2) Rare in series.
3. An active inductor arrangement including more than one inductor according to claim 1, wherein the resistors of value (1 + ) R are formed of parallel resistors, some of these resistors being connected to ground, and others in series with like resistors to create a network of grounded and floating inductors.
4. An active resonant circuit incorporating active inductors according to any one of claims 1-3 in which the component values are chosen so that 0.36 4aRC is approximately equal to the resonant frequency, where C is the value of the capacitive feedback around the second amplifier.
5. An active filter arrangement incorporating active inductors as claimed in any one of claim 1-4.
6. An active inductor substantially as illustrated in Figure 1 or Figure 2 of the accompanying drawings.
7. An active filter arrangement substantially as described with reference to Figure 3 of the accompanying drawings.
GB7931770A 1979-09-13 1979-09-13 Active inductors Expired GB2059213B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
GB7931770A GB2059213B (en) 1979-09-13 1979-09-13 Active inductors

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB7931770A GB2059213B (en) 1979-09-13 1979-09-13 Active inductors

Publications (2)

Publication Number Publication Date
GB2059213A true GB2059213A (en) 1981-04-15
GB2059213B GB2059213B (en) 1984-02-08

Family

ID=10507799

Family Applications (1)

Application Number Title Priority Date Filing Date
GB7931770A Expired GB2059213B (en) 1979-09-13 1979-09-13 Active inductors

Country Status (1)

Country Link
GB (1) GB2059213B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2365235A (en) * 2000-07-20 2002-02-13 British Broadcasting Corp A circuit for simulating an impedance

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2365235A (en) * 2000-07-20 2002-02-13 British Broadcasting Corp A circuit for simulating an impedance
GB2365235B (en) * 2000-07-20 2004-07-21 British Broadcasting Corp A circuit for simulating an impedance

Also Published As

Publication number Publication date
GB2059213B (en) 1984-02-08

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Legal Events

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PCNP Patent ceased through non-payment of renewal fee