Analog filter with adjustable filter frequency

Abstract

A low noise analog filter with adjustable filter frequency includes an oscillatory circuit, whose resonance frequency equals the filter frequency of the filter. The oscillatory circuit has a first circuit branch. One of the frequency determining elements is a capacitance and the other an inductance. The low noise analog filter further includes an amplifier with adjustable amplification installed in one of the two circuit branches. The output of the amplifier is connected with its inverting input via the frequency determining element arranged in such circuit branch. In filter operation, the amplifier amplifies, according to the adjusted amplification, a voltage applied across the frequency determining element arranged in such circuit branch and thereby effects a corresponding change of an electrical current flowing through such frequency determining element.

Description

The invention relates to an analog filter with adjustable frequency. Examples of such a filter include bandpass filters with adjustable center frequency and band blocking filters with adjustable blocking frequency.

There are a large number of electronic circuits, in which analog filters with adjustable frequency are applied.

A typical example is circuits of measuring devices, in which these filters are used, for example, for filtering measurement signals registered with a sensor.

Among these are fill level measuring devices working with ultrasound, in the case of which ultrasonic sensors operated preferably at their resonance frequency transmit short ultrasonic wave pulses toward the fill substance and receive their echo signals reflected from the surface of the fill substance back to the sensor after a travel time dependent on the fill level. In such case, the sensor receives not only the wanted signal having the resonance frequency but also disturbance signals. The disturbance signals have, as a rule, disturbance frequencies different from the resonance frequency, and are suppressed by corresponding filtering. For this, a measurement signal is filtered out from the received signal of the sensor by means of a bandpass filter matched to the resonance frequency of the ultrasonic sensor. The resonance frequencies, however, differ from sensor to sensor and are, as a rule, dependent on temperature. In order to be able to cover the total range of possibly arising resonance frequencies, for example, bandpass filters are applied with a fixed center frequency and a very large bandwidth. In such case, disturbance signal suppression is, however, so much poorer, the larger the bandwidth of the bandpass filter.

Alternatively, adjustable bandpass filters are applied. An example is active bandpass filters with multiple cross coupling, in the case of which the center frequency is adjustable via changeable resistances. FIG. 1 shows an example of an embodiment for this. In such case, an input voltage U_i referenced to a reference potential falls across a first resistor R₁ and a first capacitor C connected therewith in series to an inverting input of an amplifier A_u with constant amplification. The non inverting input of the amplifier A_u lies at the reference potential. An output signal of the amplifier A_u is fed back via a second capacitor C of equal capacitance to a first node located between the first resistor R₁ and the first capacitor C and parallel thereto via a second resistor R₂ to a second node located between the first capacitor C and the inverting input. Additionally, the first node is connected via a third resistor R₃ to the reference potential. The output signal of this bandpass filter is the output voltage U_o present at the output of the amplifier A_u referenced to the reference potential. This filter exhibits, however, due to the resistances, a large amount of noise, which, exactly in the case of the filtering of measurement signals, such as they exist e.g. in the case of ultrasound fill-level measuring devices, is very disturbing.

In contrast, passive filters exhibit a very much smaller amount of noise. There is, however, the disadvantage that the filter frequency can be changed only by connecting, or disconnecting, inductances and capacitances determining the filter frequency, or through the use of mechanically adjustable inductances and capacitances. Such an adjustable filter is described in DE 10 2006 052 873 A1, for example.

Core of the filter described there is an LC oscillatory circuit, which includes an inductance and a detunable capacitance, especially a varactor diode. Varactor diodes have, however, small capacitances, e.g. on the order of magnitude of some picofarad, so that these filters are only suitable for filtering signals with very high frequencies.

It is an object of the invention to provide a low noise, analog filter with adjustable filter frequency.

For this, the invention resides in an analog filter with adjustable filter frequency including:

• • An oscillatory circuit,
    • whose resonance frequency equals the filter frequency of the filter,
    • which has a first circuit branch, in which a first frequency determining element is arranged,
    • which has a second circuit branch connected in parallel or in series with the first circuit branch, wherein a second frequency determining element is arranged in the second circuit branch, wherein
    • one of the frequency determining elements is a capacitance and the other an inductance; and,
  • installed in one of the two circuit branches, an amplifier with adjustable amplification,
    • whose output is connected with its inverting input via the frequency determining element arranged in such circuit branch, and
    • which, in filter operation, amplifies, according to the adjusted amplification, a voltage applied across the frequency determining element arranged in such circuit branch and thereby effects a corresponding change of an electrical current flowing through such frequency determining element.

In a first embodiment, the adjusted amplification is greater than 1 and the amplifier increases the electrical current flowing through the frequency determining element.

In a second embodiment, the adjusted amplification is less than 1 and the amplifier decreases the electrical current flowing through the frequency determining element.

In a first variant,

• • the filter is a bandpass filter and the filter frequency is its center frequency, and
  • the oscillatory circuit is a parallel oscillatory circuit, in which the first and the second circuit branch are connected in parallel

Additionally, the invention includes a further development of the first variant, in the case of which

• • in the other circuit branch likewise an amplifier with adjustable amplification is applied,
    • whose output is connected with its inverting input via the frequency determining element arranged in such circuit branch, and
    • which, in filter operation, amplifies, according to the adjusted amplification, a voltage applied across the frequency determining element arranged in such circuit branch and thereby effects a corresponding change of an electrical current flowing through such frequency determining element.

In a second variant,

• • the filter is a band blocking filter and the filter frequency is its blocking frequency, and
  • the oscillatory circuit is a series oscillatory circuit, in which the first and the second circuit branch are connected in series.

In an embodiment, an output signal of the filter is an output voltage, which falls across the oscillatory circuit.

In an additional embodiment, an input signal of the filter is an input voltage, which falls across a third circuit branch, which is connected in series in front of the oscillatory circuit and in which a resistor is arranged.

In another embodiment, an input signal of the filter is an input electrical current, a further circuit branch is placed in front of the oscillatory circuit, and the further circuit branch is connected in parallel with the oscillatory circuit and a resistor is arranged in the further circuit branch.

The invention and other advantages will now be explained in greater detail based on the figures of the drawing, in which ten examples of embodiments are presented; equal elements are provided in the figures with equal reference characters. The figures of the drawing show as follows:

FIG. 1 an active bandpass filter known from the state of the art and having multiple cross coupling;

FIG. 2 a first embodiment of a bandpass filter of the invention, with a parallel oscillatory circuit, in which a voltage applied across an inductance of the parallel oscillatory circuit is amplified by means of an adjustable amplifier and thereby effects a corresponding change of an electrical current flowing through the inductance;

FIG. 3 a second embodiment of a bandpass filter of the invention, with a parallel oscillatory circuit, in which a voltage applied across a capacitance of the parallel oscillatory circuit is amplified by means of an adjustable amplifier and thereby effects a corresponding change of an electrical current flowing through the capacitance;

FIG. 4 a third embodiment of a bandpass filter of the invention, with a parallel oscillatory circuit, in the case of which an amplifier is arranged in both circuit branches;

FIG. 5 a first embodiment of a band blocking filter of the invention, with a series oscillatory circuit, in which a voltage applied across an inductance of the series oscillatory circuit is amplified by means of an adjustable amplifier and thereby effects a corresponding change of an electrical current flowing through the inductance;

FIG. 6 a second embodiment of a band blocking filter of the invention, with a series oscillatory circuit, in which a voltage applied across a capacitance of the series oscillatory circuit is amplified by means of an adjustable amplifier and thereby effects a corresponding change of an electrical current flowing through the capacitance;

FIG. 7 a filter of the invention according to FIG. 2 fed via an electrical current source;

FIG. 8 a filter of the invention according to FIG. 3 fed via an electrical current source;

FIG. 9 a filter of the invention according to FIG. 4 fed via an electrical current source;

FIG. 10 a filter of the invention according to FIG. 5 fed via an electrical current source;

FIG. 11 a filter of the invention according to FIG. 6 fed via an electrical current source;

FIG. 12 the square of the spectral energy density of the noise of the passive bandpass filter of the invention illustrated in FIG. 2 as a function of frequency; and

FIG. 13 the square of the spectral energy density of the noise of the conventional, active, bandpass filter illustrated in FIG. 1 as a function of frequency.

FIGS. 2, 3 and 4 show three examples of embodiments of a first variant of a passive analog filter of the invention with adjustable filter frequency.

The filters illustrated in these figures are bandpass filters and the filter frequency is the center frequency of the bandpass filter. Core of the filter is, in each case, an oscillatory circuit, whose resonance frequency f₀ equals the filter frequency of the respective filter. The oscillatory circuit includes two, parallel connected, circuit branches S1, S2, in which, in each case, a frequency determining element is arranged, of which one is an inductance L and one a capacitance C. In the here illustrated bandpass filters, the inductance L is arranged in the first circuit branch S1 and the capacitance C in the second circuit branch S2 connected in parallel with the first circuit branch S1.

Both circuit branches S1, S2 are connected on the input side to a third circuit branch S3, in which a resistor R is arranged. A input signal of the filter, here an input voltage U_i referenced to a fixed reference potential, e.g. ground, falls across this third circuit branch S3 to the parallel oscillatory circuit. The second and the third circuit branch S2, 53 are likewise connected on the output side to this fixed reference potential. Provided at the output of the filter as the filtered output signal is the output voltage U_o falling across the oscillatory circuit and referenced to the reference potential.

According to the invention, in one of the two circuit branches S1 or S2, an amplifier OPA₁, or, respectively, OPA₂ with adjustable amplification A_L, or A_C is applied, whose output falls across the frequency determining element arranged in such circuit branch S1, S2 to its inverting input. The non inverting input of the amplifier OPA₁, or OPA₂ is connected to the reference potential. The amplifier OPA₁, or OPA₂, in filter operation, amplifies a voltage falling across the frequency determining element arranged in such circuit branch S1 or S2 according to the adjusted amplification A_L, or A_C and effects thereby a corresponding change of an electrical current flowing through such frequency determining element. If the adjusted amplification A_L, or A_C is greater than 1, then the electrical current flowing through the frequency determining element is increased by the amplifier OPA₁, or OPA₂. If the adjusted amplification A_L, or A_C is less than 1, then the electrical current flowing through the frequency determining element is decreased by the amplifier OPA₁, or OPA₂.

The amplifiers OPA₁, and, respectively, OPA₂ are preferably operational amplifiers, whose amplification A_L, or A_C, is adjustable, for example, by means of a digital potentiometer symbolized here by an arrow.

In the case of the example of an embodiment illustrated in FIG. 2, the amplifier OPA₁ is applied in the first circuit branch S1 and connected to the inductance L. This combination of inductance L and amplifier OPA₁ acts therewith as an adjustable inductance L_eff of size:

$L_{\mathrm{eff}}=\frac{L}{A_L+1}$

In this way, there results a resonance frequency f₀ of the parallel oscillatory circuit, adjustable via the amplification A_L, of:

$f_0=\frac{1}{2\pi \sqrt{\frac{\mathrm{LC}}{A_L+1}}}$

The center frequency of this bandpass filter equals the resonance frequency f₀ of this oscillatory circuit and is automatically adjustable based on the amplification A_L.

The bandwidth B of the bandpass filter illustrated in FIG. 2 is:

$B=\frac{1}{2\pi \mathrm{RC}}$

The bandwidth B is therewith adjustable via the resistance R independently of the resonance frequency f₀ of the filter.

In the case of the example of an embodiment illustrated in FIG. 3, the amplifier OPA₂ is applied in the second circuit branch S2 and connected to the capacitance C. This combination of capacitance C and amplifier OPA₂ acts therewith as an adjustable capacitance C_eff of size:

C _eff =C(A_C+1))

In this way, there results a resonance frequency f₀ of the parallel oscillatory circuit, adjustable via the amplification A_C, of:

$f_0=\frac{1}{2\pi \sqrt{\mathrm{LC}\left(A_C+1\right)}}$

The center frequency of this bandpass filter equals the resonance frequency f₀ of this oscillatory circuit and is automatically adjustable based on the amplification A_C.

The bandwidth B of the bandpass filter illustrated in FIG. 3 is:

$B=\frac{1}{2\pi \mathrm{RC}\left(A_C+1\right)}$

The bandwidth B is therewith dependent on the resistance R and the resonance frequency f₀ of the filter.

In the case of the example of an embodiment illustrated in FIG. 4, there is applied in both the first circuit branch S1 as well as also in the second circuit branch S2, in each case, an amplifier OPA₁, OPA₂ with adjustable amplification A_L, A_C, whose output falls across the frequency determining element arranged in the respective circuit branch S1, S2 to its inverting input, and which, in filter operation, amplifies the voltage falling across the frequency determining element arranged in such circuit branch S1, S2 according to the adjusted amplification A_L, A_C and thereby effects a corresponding change of the electrical current flowing through the particular frequency determining element. Also here, the electrical current increases, when the associated amplification A_L, and, respectively, A_C is greater than 1, and it decreases, when the associated amplification A_L and, respectively, A_C is less than 1.

Therewith there results an adjustable inductance L_eff of size:

$L_{\mathrm{eff}}=\frac{L}{A_L+1}$

and an adjustable capacitance C_eff of size:

C _eff C(A_C+1))

Accordingly, there results via the amplifications A_L and A_C an adjustable resonance frequency f₀ of this parallel, oscillatory circuit of:

$f_0=\frac{1}{2\pi \sqrt{\frac{\mathrm{LC}\left(A_C+1\right)}{A_L+1}}}$

In this way, a clearly larger frequency range of the tunable filter frequencies can be covered. In such case, the amplifications A_L, A_C are controlled in opposite directions, in order that their effects do not cancel one another.

The bandwidth B of the bandpass filter illustrated in FIG. 4 is:

$B=\frac{1}{2\pi \mathrm{RC}\left(A_C+1\right)}$

FIGS. 5 and 6 show two examples of embodiments of a second variant of a passive analog filter of the invention with adjustable filter frequency. These illustrated filters are band blocking filters and the filter frequency is the blocking frequency of the band blocking filter. Core of the filter is also here, in each case, a oscillatory circuit, whose resonance frequency f₀ equals the filter frequency of the respective filter. In contrast to the earlier described examples of embodiments, the oscillatory circuit is here a series oscillatory circuit, which has two circuit branches S1, S2, which are connected in series with one another and in which, in each case, a frequency determining element is arranged, of which one is an inductance L and one a capacitance C. In the band blocking filters illustrated here, the inductance L is arranged in the first circuit branch S1 and the capacitance C in the second circuit branch 52 connected in series therewith.

Placed in front of the two, series arranged, circuit branches S1, S2 on the input side is a third circuit branch S3, in which a resistor R is arranged. The input signal of the filter is also here an input voltage U_i, which is referenced to a fixed reference potential, e.g. ground, and which falls across this third circuit branch S3 on the input side to lie against the series oscillatory circuit. The series oscillatory circuit lies on the output side likewise at this fixed reference potential and, at the output of the filter, the output voltage U_o falling across the oscillatory circuit and referenced to the reference potential is available as the filtered output signal.

Also here, according to the invention, an amplifier OPA₁, OPA₂ with adjustable amplification A_L, A_C is applied in one of the two circuit branches S1 or S2. The output falls across the frequency determining element arranged in such circuit branch S1, S2 to the inverting input of the respective amplifier OPA₁, OPA₂. The non inverting input of the amplifier OPA₁, and, respectively, OPA₂ is connected to the reference potential. The amplifier OPA₁, OPA₂, in filter operation, amplifies a voltage falling across the frequency determining element arranged in such circuit branch S1 or S2 according to the adjusted amplification A₁, or A_C and effects thereby a corresponding change of the electrical current flowing through this element. If the adjusted amplification A_L or A_C is greater than 1, then the amplifier OPA₁, or OPA₂ increases the electrical current flowing through the frequency determining element. If the adjusted amplification A_L or A_C is less than 1, then the amplifier OPA₁, or OPA₂ decreases the electrical current flowing through the frequency determining element.

The amplifier OPA₁, OPA₂ is also here preferably an operational amplifier, whose amplification A_L, A_C is adjustable, for example, by means of a digital potentiometer symbolized here by an arrow.

In the case of the example of an embodiment illustrated in FIG. 5, the amplifier OPA₁ is applied in the first circuit branch S1 and connected to the inductance L. This combination of inductance L and amplifier OPA₂ acts therewith as an adjustable inductance L_eff of size:

$L_{\mathrm{eff}}=\frac{L}{A_L+1}$

In this way, there results a resonance frequency f₀ of the series oscillatory circuit, adjustable via the amplification A_L, of:

$f_0=\frac{1}{2\pi \sqrt{\frac{\mathrm{LC}}{A_L+1}}}$

The blocking frequency of this band blocking filter equals the resonance frequency f₀ of this oscillatory circuit and is automatically adjustable based on the amplification A_L.

With the resistor R connected in series with the series oscillatory circuit, the bandwidth B of the band blocking filter illustrated in FIG. 5 is:

$B=\frac{R\left(A_L+1\right)}{2\pi L}$

The bandwidth B is therewith dependent on the resistance R and the resonance frequency f₀ of the filter.

In the case of the example of an embodiment illustrated in FIG. 6, the amplifier OPA₂ is applied in the second circuit branch S2 and connected to the capacitance C. This combination of capacitance C and amplifier OPA₂ acts therewith as an adjustable capacitance C_eff of size:

C _eff C(A_C+1))

In this way, there results a resonance frequency f₀ of the series oscillatory circuit, adjustable via the amplification A, of:

$f_0=\frac{1}{2\pi \sqrt{\mathrm{LC}\left(A_C+1\right)}}$

The blocking frequency of this band blocking filter equals the resonance frequency f₀ of the series oscillatory circuit and is automatically adjustable based on the amplification A_C.

The bandwidth B of the bandpass filter illustrated in FIG. 6 is:

$B=\frac{R}{2\pi L}$

The bandwidth B is therewith adjustable via the resistance R independently of the resonance frequency f₀ of the filter.

Instead of an input voltage the analog filters of the invention can naturally also be fed an input electrical current I_i as input signal. In such case, the third circuit branch S3 with the resistor R connected in series with the respective oscillatory circuit is absent. Instead, a further circuit branch S4 is placed in front of the respective oscillatory circuit. Circuit branch S4 is connected in parallel with the oscillatory circuit and contains a resistor R. This is shown in FIG. 7 using the example of the bandpass filter of FIG. 2, in FIG. 8 using the example of the bandpass filter of FIG. 3, in FIG. 9 using the example of the bandpass filter of FIG. 4, in FIG. 10 using the example of the band blocking filter of FIG. 5 and in FIG. 11 using the example of the band blocking filter of FIG. 6.

The formulas set forth above for the filters illustrated in FIGS. 2 to 6 for the adjustable inductance L_eff, adjustable capacitance C_eff, resonance frequency f₀ and bandwidth B of the respective filters hold analogously, wherein, in the above cited formulas, at the position of the resistance R connected in front in series in the third circuit branch S3 is placed the resistance R in the fourth circuit branch S4.

The filters of the invention have the advantage that, for adjusting the filter frequency, thus the center frequency of the bandpass filters, or the blocking frequency of the band blocking filters, only small amplifications A_L, A_C are required. Furthermore, no adjustable resistances are required, and voltages falling across resistances, or electrical currents flowing therethrough, are not amplified. Accordingly, there is in the case of the filters of the invention also no amplification of the unavoidably arising noise of ohmic resistors. Correspondingly, the filters are characterized by extremely low noise, especially in comparison to active filters.

FIG. 12 shows, in a log-log graph, the square of the spectral energy density E², in V²/Hz, of the noise, here of the voltage noise, of the passive bandpass filter of the invention illustrated in FIG. 2 as a function of frequency f in Hz over a frequency range of 10 kHz to 100 kHz.

In the comparison thereto, FIG. 13 shows, likewise in a log-log graph, the square of the spectral energy density E², in V²/Hz, of the noise, here of the voltage noise, of the conventional, active, bandpass filter illustrated in FIG. 1 as a function of frequency f in Hz over the same frequency range.

For this comparison, the two filters were designed in such a manner that they have the same center frequency and the same bandwidth. The two curves have, in each case, a marked maximum at the center frequency. As can be seen from the two FIGS. 12 and 13, the spectral energy density of the noise of the filter of the invention lies, over the entire illustrated frequency range, clearly below that of the conventional, active, bandpass filter. Especially, the difference in the relevant region of the center frequency in the illustrated comparison amounts to more than two powers of ten.

REFERENCE CHARACTERS

• U_i input voltage
• U_o output voltage
• I_i input electrical current
• L inductance
• C capacitance
• S₁ first circuit branch
• S₂ second circuit branch
• S₃ third circuit branch
• S₄ further circuit branch
• OPA₁ amplifier
• OPA₂ amplifier
• R resistor, resistance

Claims

1-9. (canceled)

10. An analog filter with adjustable filter frequency, comprising: an oscillatory circuit:whose resonance frequency equals the filter frequency of the filter;which has a first circuit branch, in which a first frequency determining element is arranged;which has a second circuit branch connected in parallel or in series with said first circuit branch, wherein a second frequency determining element is arranged in said second circuit branch, and wherein one of the frequency determining elements is a capacitance and the other an inductance; and,an amplifier installed in one of said two circuit branches, with adjustable amplification:whose output is connected with its inverting input via said frequency determining element arranged in such circuit branch; andwhich, in filter operation, amplifies, according to said adjusted amplification a voltage applied across said frequency determining element arranged in such circuit branch and thereby effects a corresponding change of an electrical current flowing through such frequency determining element.

11. The analog filter as claimed in claim 10, wherein: said adjusted amplification is greater than 1, and said amplifier increases the electrical current flowing through the frequency determining element.

12. The analog filter as claimed in claim 10, wherein: said adjusted amplification is less than 1, and said amplifier decreases the electrical current flowing through the frequency determining element.

13. The analog filter as claimed in claim 10, wherein: the filter is a bandpass filter and the filter frequency is its center frequency; andsaid oscillatory circuit is a parallel oscillatory circuit, in which said first and said second circuit branch are connected in parallel.

14. The analog filter as claimed in claim 13, wherein: in the other circuit branch likewise an amplifier with adjustable amplification is applied, whose output is connected with its inverting input via the frequency determining element arranged in such circuit branch, and which, in filter operation, amplifies, according to said adjusted amplification, a voltage applied across said frequency determining element arranged in such circuit branch and thereby effects a corresponding change of an electrical current flowing through such frequency determining element.

15. The analog filter as claimed in claim 10, wherein: the filter is a band blocking filter and the filter frequency is its blocking frequency; andsaid oscillatory circuit is a series oscillatory circuit, in which said first and said second circuit branch are connected in series.

16. The analog filter as claimed in claim 10, wherein: a output signal of the filter is an output voltage, which drops across the oscillatory circuit.

17. The analog filter as claimed in claim 10, wherein: an input signal of the filter is an input voltage, which drops across a third circuit branch, which is connected in series in front of said oscillatory circuit and in which a resistor is arranged.

18. Analog filter as claimed in claim 10, wherein: an input signal of the filter is an input electrical current; anda further circuit branch is placed in front of said oscillatory circuit, and said further circuit branch is connected in parallel with the oscillatory circuit, and contains a resistor.