(19)
(11)EP 2 401 811 B1

(12)EUROPEAN PATENT SPECIFICATION

(45)Mention of the grant of the patent:
03.01.2018 Bulletin 2018/01

(21)Application number: 10746855.5

(22)Date of filing:  25.02.2010
(51)International Patent Classification (IPC): 
H03F 1/32(2006.01)
H03F 1/52(2006.01)
H03F 3/30(2006.01)
H03F 1/02(2006.01)
H03F 3/187(2006.01)
H03F 3/45(2006.01)
(86)International application number:
PCT/US2010/025455
(87)International publication number:
WO 2010/099349 (02.09.2010 Gazette  2010/35)

(54)

LOW DISSIPATION AMPLIFIER

VERSTÄRKER MIT NIEDRIGEM VERLUSTFAKTOR

AMPLIFICATEUR À FAIBLE DISSIPATION


(84)Designated Contracting States:
AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO SE SI SK SM TR

(30)Priority: 25.02.2009 US 155382 P

(43)Date of publication of application:
04.01.2012 Bulletin 2012/01

(73)Proprietor: THX Ltd
San Rafael, CA 94903 (US)

(72)Inventors:
  • FINCHAM, Lawrence, R.
    San Rafael, CA 94903 (US)
  • JONES, Owen
    San Rafael, CA 94903 (US)

(74)Representative: Dunlop, Hugh Christopher et al
Maucher Jenkins 26 Caxton Street
London SW1H 0RJ
London SW1H 0RJ (GB)


(56)References cited: : 
WO-A1-96/30998
US-A- 3 970 953
US-A- 4 523 152
US-A- 5 594 387
US-A1- 2003 137 344
US-A- 3 530 244
US-A- 4 441 068
US-A- 4 603 282
US-A1- 2002 079 961
US-B1- 7 239 202
  
  • GRAF, R. ET AL.: 'Encyclopedia of Electronic Circuits.', vol. 7, 1999, MCGRAW-HILL, UNITED STATES OF AMERICA, ISBN 0-07-015116-4 pages 42 - 43, XP008166915
  
Note: Within nine months from the publication of the mention of the grant of the European patent, any person may give notice to the European Patent Office of opposition to the European patent granted. Notice of opposition shall be filed in a written reasoned statement. It shall not be deemed to have been filed until the opposition fee has been paid. (Art. 99(1) European Patent Convention).


Description

BACKGROUND OF THE INVENTION


1) Field of the Invention



[0001] The field of the invention generally relates to amplifiers and, more specifically, to an improved method to minimize distortion and power dissipation in a compact amplifier.

2) Background



[0002] Amplifiers are used for many applications including audio signal processing, video processing, communications, control systems, satellites, and so on. Based on its power consumption characteristics, an amplifier may be categorized into one or more categories including Class A, B, AB, D, G or H. A general background of different amplifier classifications may be found, for example, in R. Bortoni, et al., "Analysis, Design and Assessment of Class A, B, AB, G and H Audio Power Amplifier Output Stages Based on MATLAB® Software," 110th Convention of Audio Engineering Society (AES), May 12-15, 2001, pp. 1-14, and in "Audio Power Amplification," J. Audio Eng. Soc., Vol. 54, No. 4, April 2006, pp. 319- 323.

[0003] A Class A amplifier is known to require a relatively large amount of standing power and is inefficient, and thus undesirable in many applications that require low power dissipation. A Class B amplifier can have very low standing power dissipation but introduces distortion. A Class AB amplifier is somewhere between the two, and uses bias currents to reduce the distortion inherent in a Class B amplifier. A Class AB amplifier has a higher power dissipation than a Class B amplifier due to the bias currents.

[0004] As equipment gets smaller, amplifiers become an increasing limitation on the ability to reduce packaging size. The inevitable limited efficiency of an amplifier leads to power dissipation that must be dissipated by a heatsink in order to prevent the amplifier getting too hot; however, a large heatsink can take up an inordinate amount of packaging space. Techniques exist to improve the efficiency over that of a standard Class AB amplifier design, and hence reduce heatsink requirements, but these approaches often lead to compromises in the bandwidth, noise or distortion performance of the amplifier.

[0005] There are at least two aspects to the power dissipation of an amplifier system. The first is commonly known as idle or standing dissipation - that is, power dissipated when the amplifier is delivering no power to the load. With a conventional linear amplifier, this standing dissipation, which includes the bias current applied to the amplifier, is primarily concentrated in the driver and output stage of the amplifier and is generally required in conventional amplifier designs to minimize crossover distortion. In a high performance audio power amplifier of a nominal 100 Watt sine wave power capability into an 8Ω load, for example, the idle current may be of the order of 100-200 milli-amps per channel. With a quiescent power supply voltage of typically +/-45 Volts, this idle current results in roughly 9-18 Watts of idle power dissipation per channel. This can be a significant problem for a stereo amplifier, but for a multi-channel amplifier it is an even larger problem, as the idle dissipation quickly becomes excessive as the number of amplifiers is increased.

[0006] For home audio amplifiers, large heatsinks can often be used to dissipate the power and keep the temperature of the power devices down, but for size-constrained applications such as automotive entertainment systems, the size and weight of the heatsink cannot be tolerated.

[0007] The idle current for an amplification system must generally be set at the time of production for optimum distortion performance and thus increases production costs. The idle current requirements can also change with temperature and age. Therefore, over time or after prolonged use, the quality of the amplifier output may deteriorate.

[0008] To add to the idle power dissipation problem, an amplifier produces extra dissipation, sometimes referred to as dynamic dissipation, when it is delivering a signal to the load. In practice, a nominal 100 Watt capability linear power amplifier may well dissipate 40 Watt worst case when delivering sine wave signals to a load. With music as the audio source for the amplifier, this figure is lower since music has a higher crest factor than sine waves, but may still approach 30 Watts per channel.

[0009] Various techniques have been employed to reduce both the idle power dissipation and the dynamic power dissipation of linear amplifiers. One technique that can be employed to reduce idle power dissipation is to decrease the output stage bias current. However, this causes crossover distortion to increase which is difficult to eradicate with conventional negative feedback around the amplifier. Also, this technique has little effect on the dynamic power dissipation.

[0010] Another approach that can reduce both idle and dynamic dissipation is to use a 'Class G' amplifier configuration. This 'Class G' nomenclature is commonly attributed to Hitachi (see "Highest Efficiency and Super Quality Audio Amplifier Using MOS Power FETs in Class G Operation," IEEE Transactions on Consumer Electronics, Vol. CE-24, No. 3, August 1978), although the basic technique appears to have been described previously (see, e.g., U.S. Patent No. 3,622,899). A'Class G' amplifier arrangement maintains a lower voltage across the output devices under idle conditions whilst also reducing dynamic power dissipation by ensuring that the voltage across the power devices is also reduced when driving signals to the load. Thus both the idle and dynamic power dissipation is reduced. However, the switching of the output devices between the power rails often causes glitches in the output waveform that appear as distortion. These glitches have significant high frequency energy and so are difficult to correct by negative feedback. Careful design can reduce this effect but cannot eliminate it and tends to increase high frequency dynamic power dissipation.

[0011] An alternative way of reducing amplifier dissipation is to implement a switching amplifier, and specifically a so-called 'Class D' architecture. With this design, the linear amplifier is replaced by power switches operating at typically several hundred kilohertz for a high performance audio amplifier. The nominal efficiency of this design into a resistive load can theoretically be very high, although in practice switching losses and output filter losses significantly reduce the actual efficiency. The high switching frequency can cause significant EMI problems which then require bulky inductors to prevent coupling to power supply and output lines, as well as careful screening to avoid radiation. These additions mean that although the basic amplifier components can be small and low cost, the overall size is significantly larger and more costly due to the need for the inductive and filter components. Furthermore, the continual switching causes a significant idle current due to the dynamic switching losses and the pulse width modulation (PWM) process used to generate the switching signal leads to a poor distortion performance compared to a linear amplifier.

[0012] An example of a Class D amplifier is the model TDF8590TH amplifier available from NXP Semiconductors, a company headquartered in the Netherlands. When this amplifier is configured to provide a nominal 100 Watt sine wave power to an 8Ω load, the idle dissipation is in excess of 4 Watts/channel. The total harmonic distortion (THD) is above 0.1 % at 10kHz at all levels above 10 Watts output and rises dramatically at higher output levels-and even these figures are an underestimate of the actual distortion due to the use of an AES17 filter to remove the effect of the residual switching frequency components on the measuring equipment. The intermodulation distortion (IMD) performance is much worse than a well-designed linear amplifier. The output inductors also generally must be large, in order that they do not saturate or introduce further distortion, and typically measure 4 to 5 cubic centimeters, which is a barrier to overall circuit and package miniaturization.

[0013] There remains a need therefore for an amplifier topology that can be readily miniaturized while providing low power dissipation. There further is a need for an amplifier that is capable of providing low idle and dynamic power dissipation levels, requires no bias setting, and no inductors for EMI or filtering. There further is a need for an amplifier that delivers very low distortion levels.

[0014] US 3 970 953 A describes a distortion-free amplifier for electric signals that has a high-quality low-power amplifier-section.

SUMMARY OF THE INVENTION



[0015] The invention relates to an amplification system as set forth in the claims.

[0016] Further embodiments, alternatives and variations are also described herein or illustrated in the accompanying figures.

BRIEF DESCRIPTION OF THE DRAWINGS



[0017] 

FIG. 1 is a generic schematic diagram of a conventional linear amplifier as known in the prior art.

FIG. 2 is a schematic diagram of an amplifier showing, among other things, an arrangement of impedance.

FIG. 3 is a schematic diagram of embodiment of an amplifier similar to that of FIG. 2, but having an additional feedback loop.

FIG. 4 is a graph showing an example of distortion performance that can be achieved by an amplifier built according to the principles disclosed herein, under certain load parameters.

FIG. 5 is a block diagram of another amplifier design using an amplifier cascading technique.

FIG. 6 is a block diagram illustrating another example of an amplifier design in accordance with various embodiments as disclosed herein.

FIG. 7a is a schematic diagram of a current limiting circuit as known in the prior art, while 7b is a schematic diagram of an alternative current limiting circuit as may be used in connection with various embodiments as disclosed herein.

FIGS. 8a and 8b are diagrams comparing the frequency responses of different amplifier designs.


DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS



[0018] According to one or more embodiments, a low power amplifier is provided having at least a first amplifier configured as or including a driver stage and a second amplifier configured as or including a main output stage, biased into operating modes in which they draw very little idle power, yet also consume very little dynamic power when active. A plurality of impedance networks provide, among other things, feedback paths from the outputs of the first amplifier and the second amplifier to the first amplifier, enabling in part the ability of the low amplifier to combat distortion. The impedance networks also provide a coupling path from the output of the second amplifier including the main output stage to the load, and another coupling path from the output of the first amplifier including the driver stage amplifier to the load. The impedance networks are preferably resistors, capacitors, or network combinations thereof.

[0019] An additional feedback path may also be provided from the load to the input of the first amplifier. The additional feedback path may include a low pass filter and more specifically a T-network of two resistors and a capacitor, and may help flatten out the frequency response of the amplifier at low frequencies. An intermediate amplifier stage may also be added between the driver stage amplifier and the main output stage to provide additional versatility and distortion reduction.

[0020] The first and second amplifiers are both preferably operated in low power dissipation modes, although in some embodiments where power dissipation is not as critical, one or both of the amplifiers can be operated in a higher power dissipation mode in order to, e.g., simplify the design, further reduce distortion (if necessary), or for other reasons. As used herein a low power dissipation mode or low dissipation mode generally includes those operating modes in which standing or idle current dissipation is kept low, and thus would generally include Class B, G and H modes, and potentially Class AB mode in certain configurations.

[0021] As one example, the first amplifier including the driver amplifier stage may be operated in a Class AB mode, while the second amplifier including the main output stage may be operated in a Class B and/or Class G or H mode. Thus, the overall power draw of the amplifier may be kept very low. The second amplifier may alternatively be operated in Class AB mode at the expense of increased power dissipation, which may lower distortion even further. As another example, both the first and second amplifiers can be operated in Class G mode, or both operated in Class H mode, or one in Class G mode and the other in Class H mode. The novel amplifier designs disclosed and taught herein therefore provide a great deal of flexibility and versatility in terms of operating mode selection and overall design configuration. The amplifier design can be tailored for specific purposes including extremely low power dissipation, very low distortion, compact structure, etc., or combinations thereof.

[0022] Figure 1 is a generic schematic diagram of an example of a conventional linear amplifier 100 as known in the prior art. As shown in Figure 1, the linear amplifier 100 includes an input stage 110, a driver stage 120, and an output stage 150 that may include, for example, a pair of transistors 131 and 132 (also labeled as Q1 and Q2 in Figure 1) coupled to positive and negative voltage rails 130, 135 (also labeled as +V and -V in Figure 1). The input stage 110, driver stage 120, and output stage 150 are connected in a serial arrangement. The input stage 110 receives an input signal 106 from an input signal source 105. The output stage transistors Q1, Q2 are normally biased by a voltage source 128 (also labeled Vb) into either Class B or Class AB operation. While shown in Figure 1 as single transistors, the output stage transistors Q1 and Q2 may be embodied as different types of circuit such as single transistors, compound transistor arrangements or FETs. The output stage 150 provides an amplified output signal 140 to a load 145 (represented as an impedance in Figure 1).

[0023] Also in Figure 1, a feedback capacitor 124 (also labeled as Z2 in Figure 1) applies local feedback around the driver stage 120 whilst ensuring stability by introducing a 6dB/octave roll-off to the open loop frequency response of the amplifier 100. Driver stage 120 is typically biased into Class A operation. Input stage 110 is typically implemented as a transconductance stage. Additional resistors 115 and 112 (also labeled as R4 and Rg in Figure 1) provide overall negative feedback around the complete amplifier.

[0024] As mentioned earlier, an amplifier of this generic type generally suffers from poor idle and dynamic dissipation performance when biased into Class AB operation, and poor distortion performance when biased into Class B operation. Dissipation can be reduced by operating in Class G mode, but then more distortion mechanisms are introduced which are difficult to address by means of conventional negative feedback.

[0025] As explained for example in connection with Figure 2, distortion is significantly reduced over the conventional linear amplifier of Figure 1 by providing a signal path from the gain/driver stage X1 to the output by means of an impedance network Z3 whilst also introducing another impedance network Z1. Figure 2 is a schematic diagram of a novel amplifier design, illustrating a useful arrangement of impedance networks and other amplifier circuitry by way of one example. In Figure 2, an amplifier 200 includes, among other things, a gain/driver stage 210 (also labeled as X1 in Figure 2) and an output stage 250 that may include, for example, a pair of transistors 231 and 232 (also labeled as Q1 and Q2 in Figure 2) coupled, similar to Figure 1, to positive and negative voltage rails +V and -V (not shown in Figure 2). The gain/driver stage 210 receives an input signal 206 from an input signal source 205. While shown in Figure 2 as single transistors, as with Figure 1 and all other embodiments that will be described herein, the output stage transistors Q1 and Q2 may be embodied as different types of circuit such as single transistors, compound transistor arrangements or FETs. The output stage 250 provides an amplified output signal 240 to a load 245 (represented as an impedance in Figure 2).

[0026] More generally, the gain/stage 210, while conceptually shown as a single amplifier in Figure 2, may be constructed from multiple amplifier stages or may be included as part of a larger amplifier block. Likewise, the output stage 250, while shown as primarily consisting of transistors Q1 and Q2, may be included as part of a larger amplifier block which may contain one or more stages, and would also be understood to include bias components, protection elements, and other conventional features that are not shown in detail in Figure 2 for the sake of simplicity. Those skilled in the art will appreciate that there are many different ways to implement the gain/driver stage 210 and output stage 250 of amplifier 200.

[0027] As noted above, an impedance network 290 (also labeled as Z3 in Figure 2) is provided between the output of the gain/driver stage 210 and the load 245. Another impedance network 280 (also labeled as Z1 in Figure 2) is provided between the output stage 250 and the load 240. Another impedance network 270 (also labeled as Z2 in Figure 2) is provided from the output of the gain/driver stage 210 to one of the differential inputs of the gain/driver stage 210. A fourth impedance network 260 (also labeled as Z4 in Figure 2) is provided from the output stage 250 to the same differential input of the gain/driver stage 210. Impedance networks 260 and 270 are coupled to ground (or some other reference potential) by another impedance network 212 (also labeled as Zg in Figure 2).

[0028] In the example of Figure 2, impedance network 290 is embodied as a capacitor 291 and resistor 292 connected in parallel. Impedance network 280 is embodied as a resistor 281. Impedance network 270 is also embodied as a resistor 271. Impedance network 260 is embodied as a resistor 262 and capacitor 261 connected in series.

[0029] Choosing the values of the impedance networks Z1, Z2, Z3, Z4 such that they satisfy the relationship Z1(s)•Z2(s) = Z3(s)•Z4(s), the distortion on the amplifier 200 can be significantly reduced compared to a standard feedback amplifier of the type shown in Figure 1. As noted above, in this example impedance network Z1 is preferably embodied as a resistor, impedance network Z2 is preferably embodied as a capacitor, impedance network Z3 is preferably embodied as a parallel combination of resistor and capacitor, and impedance network Z4 is preferably embodied as a series combination of resistor and capacitor, although other equivalent impedance networks may be used. The time constant of the impedance network Z3 preferably matches that of impedance network Z4. At low frequencies, below the frequency at which the impedance of Z3 become capacitive, impedance network Z3 appears resistive in nature and impedance network Z4 appears to be capacitive. The presence of impedance network Z3 softens the crossover knee of the output stage 250 by virtue of the driver stage to load output connection through impedance network Z3.

[0030] In order to gain maximum distortion reduction, impedance network Z4 is preferably capacitive in nature so that the ratio of impedances of Z2:Z4 equals Z3:Z1. However, this means that the open loop gain of the feedback loop around the output stage 250 no longer falls off with frequency. Incorporating a series resistor within Z4 reinstates the fall in gain with frequency above the breakpoint at which Z4 stops appearing capacitive and becomes resistive in nature. The resistor 262 in impedance network Z4 is chosen to set a unity loop gain frequency that ensures stability.

[0031] To retain full distortion reduction, impedance network Z3 should be made to appear capacitive in nature at high frequencies; hence the matching of the time constants of impedance networks Z3 and Z4. There is generally a free choice of time constant for the components of impedance networks Z3 and Z4. However, the larger the time constant, the larger the capacitor has to be in impedance network Z3, and the greater the current that will be drawn from the gain/driver stage 210 (i.e., X1) at high frequencies. To minimize size of the amplifier 200, the time constant for impedance networks Z3 and Z4 should be kept low.

[0032] The balancing of the impedance networks will work even in the presence of parasitic elements in the impedance networks. For instance, a parasitic inductance in series with resistor 281 can be balanced by placing a suitable value resistor in series with capacitor 291. As reflected by the example of Figure 2, all of the components of impedance networks Z1 - Z4 are realized as resistors, capacitors or combinations thereof (excluding parasitic elements). This design approach can lead to a very compact amplifier package. The term "resistor" in this context includes any resistive element that displays a substantially constant impedance relationship over the applicable operating frequency range, and will typically, but not necessarily, involve a conventional discrete resistor component.

[0033] By itself, the choice and arrangement of impedance networks in Figure 2 works adequately but can be improved. For example, the incorporation of the series capacitor 262 within impedance network Z4 means that below the break frequency formed by its series resistor/ capacitor combination of elements 261 and 262, the closed loop gain of the complete amplifier 200 increases at 6dB/octave as frequency decreases. Additionally, the open loop gain around transistors Q1, Q2 due to the arrangement of impedance networks Z2 and Z4 and gain/driver stage 210 becomes constant at low frequencies rather than rising at 6dB/octave with decreasing frequency as with a conventional feedback amplifier. Thus, the distortion reduction around transistors Q1 and Q2 by means of negative feedback will be lowered as compared to a conventional amplifier with this choice of impedance networks. Additional distortion reduction will still be achieved by virtue of the incorporation of impedance network Z3 into the amplifier 20, but there is still room for improvement, as will be explained in more detail below. Also, the output resistance of the amplifier 200 is approximately equal to the parallel combination of the impedance networks Z1 and Z3. In the case where the first impedance network Z1 is embodied as a resistor, the output resistance of the amplifier 200 at low frequencies is generally higher than would be the case for a purely conventional feedback amplifier such as illustrated in Figure 1.

[0034] Figure 3 illustrates how further improvements can be made to distortion performance and closed loop response in the foundational amplifier design of Figure 2. In Figure 3, elements labeled 3xx generally correspond to the similar elements labeled 2xx in Figure 2. In Figure 3, an amplifier 300 receives an input signal 306 from an input signal source 305. Similar to the amplifier 200 of Figure 2, the amplifier 300 of Figure 3 includes a gain/driver stage 310, an output stage 350 comprising transistors 331 and 332 (also labeled as Q1 and Q2), and impedance networks 360, 370, 380 and 390 (also respectively labeled as Z4, Z2, Z1 and Z3 in Figure 3). A network 356 comprising resistors 352, 353 (also labeled as R5, R6 in Figure 3) and a capacitor 354 (also labeled as C7 in Figure 3) has been added to the amplifier 300 to form an additional feedback loop. The feedback is taken from the final output 340 of the amplifier 300 rather than the output stage 350 directly although it is then fed into the same feedback input terminal of gain/driver stage 310 as the existing feedback loop that is based upon impedance networks Z2 and Z4. Notwithstanding this, this connection of the extra feedback loop does not upset the conditions required for maximum distortion reduction.

[0035] Simply adding another resistive feedback path to the amplifier arrangement of Figure 2 would generally result in a non-flat frequency response because extra feedback loop is placed around the closed loop system of Figure 2, and the closed loop gain is not large enough to ensure that the final closed loop response of the amplifier is independent of the value of the Figure 2 closed loop gain. However, by designing the extra feedback network 356 to have a low pass filter response with a cut-off frequency that matches the breakpoint frequency of impedance networks Z3 and Z4 and with an appropriate gain, then the overall amplifier 300 can be designed to have a flat response. Thus the rising low frequency response of the amplifier system of Figure 2 is perfectly compensated by the design additions of Figure 3.

[0036] The extra feedback loop of Figure 3 provided by the addition of feedback network 356 also additionally reduces distortion at low frequencies, compensating for the compromised low frequency distortion performance of the Figure 2 amplifier implementation. Furthermore, this extra feedback loop also reduces the output impedance of the amplifier at low frequencies since the feedback is taken from directly across the load 345 and hence impedance network Z1 is within this feedback loop.

[0037] Having the extra overall frequency dependent feedback loop to lower the output impedance of the amplifier 300 allows the bridge impedance network Z1 to have a higher impedance than would otherwise be possible, within the constraints of power losses within the resistor 381 of the impedance network Z1; thus, the impedance of element Z3 can be similarly increased to lower the value of the parallel capacitance and with it the high frequency current that must be sourced from the gain/driver stage 310.

[0038] The available choices of capacitor and resistor values for impedance networks Z1-Z4 means that balancing at high frequency ranges can be more accurately attained, since capacitors and resistors of the values used for the amplifier design of Figure 3 can be readily obtained with close manufacturing tolerances. The voltage that appears across the capacitor 391 within impedance network Z3 is quite small (it is only the gain/error loss in the output stage plus the product of the output current times the impedance of Z1) and so its package size, given the low voltage requirements of the capacitor 391, is also commensurately small, allowing for miniaturization of the amplifier 300. Multiple amplifiers using the design shown in Figure 3 can be placed in close proximity with little interaction between the impedance networks, because the lack of balancing inductors means that there is less possibility of magnetic coupling among the amplifiers.

[0039] The use of the additional impedance networks Z1, Z3 and Z4 and the extra feedback loop provided by the addition of feedback network 356 allows the high frequency distortion of the amplifier 300 to be significantly lower than a conventional feedback amplifier and so the output stage 350 could potentially be operated, for example, in Class B mode whilst still avoiding crossover distortion. Thus, idle power dissipation that normally occurs due to the quiescent current required to bias a conventional amplifier output stage into Class AB mode is eliminated by the design of Figure 3. This might be of limited use if the gain/driver stage 310 of amplifier 300 were required to have a high idle current drain. However, the gain/driver stage 310 in this example operates at much lower power than the main output stage 350 based around transistors Q1 and Q2, and so the gain/driver stage 310 can be configured with a Class AB output stage 350 having linear, fast output devices (transistors Q1 and Q2) and so still operate with low distortion compared to the main output stage 350. Thus the dissipation in the gain/driver stage 310 can also be very low.

[0040] By incorporating a low power Class AB output stage internally within the gain/driver stage 310, the distortion introduced into the error signal by the Class AB operation of the gain/driver stage 310 can be made exceedingly small. Typically, for an audio power amplifier according to the design shown in Figure 3 capable of delivering 100 Watts nominal output power into a 16 ohm load, the gain/driver stage 310 can be configured to operate for instance with only 1-2 milliamps of quiescent current, which is quite low.

[0041] Given the significant reduction in high frequency distortion of the output stage 350, the dynamic power dissipation of the amplifier 300 can also be reduced by employing a Class G or Class H architecture. Unlike with a conventional feedback amplifier, the high frequency distortion components introduced by the Class G rail switching transitions or Class H tracking scheme will be reduced by using the amplifier feedback configurations of some of the embodiments disclosed herein so that a very low distortion, very low idle power dissipation, low dynamic power dissipation amplifier can be realized. One example of a tracking power supply that can be used in conjunction with the amplifier designs disclosed herein to provide additional power savings is described in co-pending U.S. Patent Application Ser. No. 12/253,047 filed on October 16, 2008, assigned to the assignee of the present invention. The use of a Class G or H architecture for the first amplifier containing the gain/input stage may have the potential to introduce non-linearities into the system, which could need to be controlled or otherwise taken account of.

[0042] Where a Class G or H architecture is applied to both the first and second amplifiers, different power rails (with different voltage levels) may be provided to the first amplifier and the second amplifier to, e.g., help isolation, reduce non-linearities, and minimize power dissipation.

[0043] Figure 4 shows an example of the distortion performance that can be achieved by an amplifier built according to the principles outlined above, when capable of driving a 56 Volt peak signal into a 16 ohm load using an amplifier design constructed according to Figure 3. As shown in Figure 4, the total harmonic distortion is quite low at relatively low frequencies (generally ranging from about 0.0003 to 0.0010 percent distortion level at 1 kHz), and remains low even at higher frequencies (generally ranging from about 0.0020 to 0.0050 percent distortion level at 10 kHz).

[0044] Figures 8a and 8b are idealized frequency response graphs showing the effect of the additional feedback loop 356 in the embodiment of Figure 3. Figure 8a shows that at relatively low frequencies, the overall amplifier gain drops off, then flattens out at a shelf region, and then later drops off again with increasing frequency. By using the additional feedback loop of Figure 3, this frequency response can be altered as shown in Figure 8b. The low frequency response is perfectly compensated by the outer feedback loop, resulting in a flat frequency response out to relatively high frequencies. The outer frequency loop can also be used for additional purposes, such as to extend the operating range of the amplifier through the introduction of an additional zero and pole at high frequencies.

[0045] Further modifications or enhancements can also be made to the amplifier architectures described above. For example, although the distortion of the Class AB gain/driver stage 310 can be made to be low compared to that of the output stage 350, it will still generate some residual distortion. To overcome this, the Class AB gain/driver stage 310 can itself employ the same distortion reduction technique as used around the output stage 250 as previously outlined in connection with Figure 2.

[0046] This "cascaded" approach is illustrated in the amplifier design shown in Figure 5. Elements in Figure 5 labeled "5xx" generally correspond to the similar elements labeled "3xx" in Figure 3. In Figure 5, an amplifier 500 receives an input signal 506 from an input signal source 505. Similar to the design of Figure 3, the amplifier 500 includes a gain/driver stage 510, an output stage 550 comprising transistors 531 and 532 (also labeled as Q1 and Q2), and impedance networks 560, 570, 580 and 590 (also respectively labeled as Z4, Z2, Z1 and Z3 in Figure 5). An additional feedback network 556 comprising resistors 552, 553 (also labeled as R5, R6 in Figure 5) and a capacitor 554 (also labeled as C7 in Figure 5) is included in the amplifier 500, having the same general purpose as in Figure 3, with feedback being taken from the final output 540 of the amplifier 500 and fed into the feedback input terminal of gain/driver stage 350. Also added in Figure 5 is an intermediate stage 542, which in one aspect may act as a second or supplemental driver stage, comprising transistors 543 and 544 (also labeled as Q3 and Q4) and voltage bias components 546 and 547. The transistors 543 and 544 and coupled to the positive voltage rail +V and negative voltage rail -V respectively, and may be biased into Class AB operating mode by bias components 546 and 547

[0047] The output of the intermediate stage 542 is coupled to the input of the output stage 550 via a resistor 529 (also labeled as Z1i in Figure 5). An additional resistor 528 (also labeled as Z3i) is connected from the input of the output stage 550 to the input of the intermediate stage 542. The feedback taken from impedance network 590 (Z3) thus passes through resistor 528 for purposes of intermediate stage 542, although it is still applied directly to the input of the output stage 550. An additional capacitor 548 (also labeled Z2i in Figure 5) is provided from the output of the gain/driver stage 510 to the feedback input terminal thereof. The feedback derived from impedance network 570 (Z2) is taken from the output of the intermediate stage 542 instead of the output of the gain/driver stage 510. The additional elements 529, 548 and 528 (Z1i, Z2i and Z3i) form part of an inner feedback loop, while impedance network 570 (Z2) shares its operation between the inner and outer feedback loops.

[0048] Both the gain/driver stage 510 and the intermediate stage 542 provide some aspect of feed-forward operation, in that both provide current to the load when the main output stage 550 is relatively idle, and hence both may be viewed as having a driver function to some degree. Both stages may also supply gain. In this respect, the designation of particular stages as "gain" or "driver" stages is not intended to be limiting.

[0049] In the example shown in Figure 5, the inner loop components 529, 548 and 528 (Z1i, Z2i and Z3i) have been chosen, along with impedance network 570 (Z2), such that the inner loop realizes the distortion reduction condition described for the Figure 3 amplifier design, with the Class AB stage (i.e., the internal output stage of gain/drive stage 510, in certain embodiments) retaining an integrator type response in respect of the action seen by the outer loop. A resistor 572 (R2) has been added to impedance network 570 (Z2) to help ensure stability of the inner feedback loop around transistors Q3 and Q4, while another resistor 592 (R3i) has been added to impedance network 590 (Z3) to compensate the outer feedback loop for the zero introduced into the integrator response by resistor 572. This arrangement makes it possible for the other outer loop components of impedance networks Z1 - Z4 to remain the same as the example illustrated in Figure 3. The retention of the high frequency roll-off of the improved driver stage comprising gain/driver stage 510 and intermediate stage 542 allows stability of the feedback loop around the output stage 550, and the final overall feedback loop still allows for low output impedance of the amplifier 500 at audio frequencies.

[0050] Other arrangements of the inner loop impedance networks are also possible. For example, if an extra gain stage is introduced before gain/driver stage 510, then capacitor 571 (C2) in impedance network 570 (Z2) could be dispensed with and resistor 528 (Z3i) replaced with a capacitor. The gain of this inner loop would then be flat with frequency, so the extra gain stage could be given an integrator response and the outer bridge and loop components Z4, R5, R6, C7, Zg could be connected to the input of the additional integrator gain stage.

[0051] Such an arrangement is detailed in Figure 6. Elements in Figure 6 labeled "6xx" generally correspond to the similar elements labeled "5xx" in Figure 5. In Figure 6, an amplifier 600 receives an input signal 606 from an input signal source 605. Similar to Figure 5, the amplifier 600 includes a gain/driver stage 610B, an intermediate stage 642 comprising transistors 643 and 644 (also labeled as Q3 and Q4) and voltage bias components 646 and 647, and an output stage 650 comprising transistors 631 and 632 (also labeled as Q1 and Q2), along with impedance networks 660, 670, 680 and 690 (also respectively labeled as Z4, Z2, Z1 and Z3 in Figure 6). An additional gain stage 610A (also labeled X2 in Figure 6) has been added before the gain/driver stage 610B. The amplifier 600 further includes an outer feedback network 656 comprising resistors 652, 653 (labeled as R5, R6) and capacitor 654 (labeled as C7), having a similar purpose as in Figures 3 and 5, with feedback being taken from the final output 640 of the amplifier 600 and fed into a feedback input terminal of gain stage 610A. In this case, the impedance network 670 (Z2) is positioned between the output of the gain stage 610A and the feedback input terminal of gain stage 610A. Similarly, the impedance network 660 (Z4) is positioned between the output of the driver stage 650 and the feedback input terminal of gain stage 610A.

[0052] The feedback from the output of gain/driver stage 610B continues to run through capacitor 648 (Z2i) into the feedback input terminal of the gain/driver stage 610B. A feedback connection is also made from the output of the intermediate stage 642 to the feedback input terminal of the gain/driver stage 610B. In this case, the feedback element is a resistor 619 (also labeled as R2), and another resistor 618 (also labeled Rgi) has been added coupling the feedback input terminal of the gain/driver stage 610B to ground (or some other reference potential). Capacitor 628 and resistor 629 (also labeled as Z3i and Z1i respectively) perform similar functions to their counterparts in Figure 5, both of them forming part of the inner feedback loop.

[0053] In the design of Figure 6, the added gain stage 610A is configured with an integrator response (using the capacitor 671 of impedance network Z2), and the outer bridge and loop components Z4, R5, R6, C7, Zg are connected to the feedback input of the added gain stage 610A instead of the gain/driver stage 610B. The gain of the inner feedback loop including resistors 618 and 619 (Rgi and R2) is flat with frequency.

[0054] As with Figure 5, in the example of Figure 6 the other inner loop components 629, 648 and 628 (Z1i, Z2i and Z3i) have been chosen, along with impedance network 670 (Z2), such that the inner loop realizes the distortion reduction condition described for the Figure 3 amplifier design, with the Class AB stage (i.e., the internal output stage of gain/drive stage 510, in some embodiments) retaining an integrator type response in respect of the action seen by the outer loop. The choice of outer loop impedance network values to ensure maximum distortion reduction now has to take account of the gain of the inner loop which increases the effective impedance of Z2 by the ratio [R2+Rgi]/Rgi. A resistor in impedance network 670 (Z2) is not needed for stability of the inner feedback loop around transistors Q3 and Q4. This arrangement again makes it possible for the other outer loop components of impedance networks Z1-Z4 of the Figure 3 amplifier design to remain the same. The retention of the high frequency roll-off of the inner amplifier subsystem comprising gain stage 610A, gain/driver stage 610B, and intermediate stage 642 allows stability of the feedback loop around the output stage 650, and the final overall feedback loop still allows for low output impedance of the amplifier 600 at audio frequencies.

[0055] If the output impedance of the inner amplifier subsystem is an appreciable value in comparison to the impedance of Z3, then impedance network Z3 can be modified (i.e., increased) to ensure correct distortion reduction.

[0056] By utilizing these extra network arrangements in the amplifier designs of Figures 5 and 6, the dissipation of the Class AB driver stage (that is, the internal output stage of the gain/driver stage 510 or 610B, in some embodiments) can be made even lower by reducing the Class AB quiescent current further, since its distortion can be greatly reduced by the techniques described. The Class AB stage of the gain/driver stage 510 or 610B could itself be biased in Class B, resulting in a reduction of idle dissipation.

[0057] A further reduction in idle dissipation can be obtained by operating the gain/driver stage 210, 310, 510 or 610B in Class G or H mode, since the quiescent power supply voltage to the gain/driver stage will be lower than would be the case otherwise. This could be done also without the extra network(s) of Figure 5 or 6, but extra care would be needed in order to eliminate any power supply switching spikes from affecting the output of the gain/driver stage. The extra network circuitry allows any switching distortion introduced into the gain/driver stage to be significantly reduced.

[0058] Amplifiers generally incorporate small current sensing resistors in series with the output transistors in order to provide for current limiting protection circuits. Impedance network Z1 employed in the various amplifier designs of Figures 2, 3, 5 and 6 can be used to replace these current sensing resistors as depicted in Figures 7a and 7b. Figure 7a shows a conventional current limiting circuit arrangement in which a push-pull output stage 700 comprises n-type transistor 711 and p-type transistor 712 (also labeled as Q1 and Q2) that are inter-connected with a combination of circuitry including transistors 721, 722 and 723 (also labeled as Q3, Q4 and Q5 respectively), current source 724 (also labeled as I1), and resistors 714 and 715 through which the output signal passes to reach the final output 720 of the output stage 700. The amount of current that can be output from transistor 711 is limited by the current that passes through resistor 714, and that amount of current is in turn determined by the base-to-emitter voltage of transistor 721. Resistor 715 and transistor 722 operate in a similar fashion to protect transistor 712 from excessive output current.

[0059] Figure 7b, on the other hand, shows a modified current limiting circuit arrangement that takes advantage of the presence of impedance network Z1 to dispense with resistors 714 and 715. In Figure 7b, output stage 750 comprises n-type transistor 731 and p-type transistor 732 (also labeled as Q1 and Q2) that are again inter-connected with a combination of circuitry including transistors 751, 752 and 753 (also labeled as Q3, Q4 and Q5 respectively), current source 754 (also labeled as I1), and, in this case, resistor 781 which may be the resistor in impedance network Z1 of any of the previous embodiments described herein. In this case, when transistor 731 (Q1) is ON, then resistor 781 serves to limit the output current in the same way as resistor 714, i.e., using the relatively fixed base-to-emitter voltage of n-type transistor 751 to limit the output current, and when transistor 732 (Q2) is ON, then resistor 781 limits the output current in the same way as resistor 715, i.e., using the relatively fixed emitter-to-base voltage of p-type transistor 752 to limit output current.

[0060] The invention has generally been illustrated or discussed with particular reference to an audio power amplifier but is by no means limited to this application area. The disclosed techniques apply also, for example, to low power audio amplifiers, video amplifiers and radio frequency amplifiers, among others.

[0061] According to various embodiments as disclosed herein, a power amplifier is provided having low power dissipation and, more specifically, is capable of having low idle and dynamic power dissipation levels. The power amplifier may not require a bias setting, and further may not require inductors for EMI or filtering. The power amplifier may also deliver very low distortion levels.

[0062] In certain embodiments described herein, a low-power, low-distortion amplifier includes a gain/driver stage, an optional intermediate stage, and an output stage in a cascaded arrangement. A coupling path, which may in one aspect be viewed as a feed-forward path, is provided from the output of the gain/driver stage to the load, via a feed-forward impedance network that may include a capacitor and a resistor connected in parallel. The output stage may be coupled to the load by another impedance network such as a resistor. The output stage may also be coupled to the input of the gain/driver stage by another impedance network, which may take the form of a capacitor and a resistor in a series arrangement. The output of the gain/driver stage may also be coupled to its input by another impedance network, which may take the form of a capacitor.

[0063] In addition, a feedback network is provided from the load to the input of the gain/driver stage for stabilization, which may have the affect of flattening the overall frequency response at low frequencies will leaving the response unchanged at higher frequencies. The additional feedback network may take the form of a low pass filter and, more specifically, a T-network of two series resistors and a capacitor connected between their common node and a reference potential (such as ground). The additional feedback network may be used to counter-act the resistive nature of the frequency response of the feed-forward impedance network at low frequencies. Because the additional feedback network is fed into the negative input of the gain/driver stage, it effectively cancels out the low frequency component of the amplifier's frequency response contributed by the feed-forward impedance network.

[0064] In some embodiments, an additional intermediate amplifier stage may be provided, which functions in certain respects as a driver stage, and has a feed-forward path coupling to the load via the third impedance element.

[0065] In certain embodiments, the main output stage is operated in Class B mode, while the gain/driver stage is operated in Class AB mode, thus leading to low power dissipation configuration. At low signal levels, the gain/driver stage (and/or an intermediate amplifier stage) may provide the drive for the output signal via the feed-forward or coupling between the gain/driver stage (and/or the intermediate amplifier stage) and the load, (through impedance network Z3, while at higher signal levels the main output stage drives the load. In alternative embodiments, one or both of the gain/driver stage and the main output stage may be operated in Class G or H mode, with the addition of an appropriate power supply for the amplifier. In alternative embodiments, the main output stage may be operated in Class AB mode, or else in Class A mode. While doing so may increase power dissipation, this configuration may still take advantage of other benefits provided by the novel designs discussed herein.

[0066] The novel power amplifier embodiments of Figures 2, 3, 5 and 6 may be realized in a very small package and, in particular, may be implemented entirely on a single chip, with the possible exception of the capacitive component of impedance network Z3 which may, in some cases, be large but still relatively small as compared to an inductor, hence allowing smaller overall packaging size. Because of the amplifier's low power dissipation, multiple amplifiers (such as four, eight, or possibly more) may be included on a single chip without the risk of over-heating. Such a chip can be particularly convenient for multi-channel amplifier system such as used in audio applications or for other purposes.

[0067] As noted above, the amplifier designs disclosed herein may be suitable for many different types of applications, including audio or sound reproduction, communications, satellites, and other applications. The novel amplifier designs can potentially have very wide frequency range with substantially flat or constant gain, while maintaining low power dissipation and low distortion. For example, the amplifier may provide relatively flat or constant gain over the range of 20 Hz to 20 KHz for audio applications, but is not so limited, and conceptually may provide flat or constant gain over a much larger pass-band, depending upon the specific application.

[0068] While preferred embodiments of the invention have been described herein, many variations are possible which remain within the concept and scope of the invention. Such variations would become clear to one of ordinary skill in the art after inspection of the specification and the drawings. The invention therefore is not to be restricted except within the scope of any appended claims.


Claims

1. An amplification system, comprising:

a first amplifier (210, 310, 510) operable to receive an input source signal (205, 305, 505);

a second amplifier (250, 350, 550) connected downstream from the first amplifier;

a first impedance network Z1 coupling the second amplifier to a load (245, 345, 545);

a second impedance network Z2 operative to provide negative feedback signal indicative of an output of the first amplifier to an input (Vf) of the first amplifier;

a third impedance network Z3 coupling the output of the first amplifier to the load at a common node with the first impedance network Z1; and

a fourth impedance network Z4 operative to provide a negative feedback signal indicative of an output of the second amplifier to the input of the first amplifier;

wherein all of said impedance networks Z1, Z2, Z3 and Z4 include resistors, capacitors, or network combinations thereof; characterized in that none of the impedance networks Z1, Z2, Z3 and Z4 includes a balancing inductor; and the impedance of the third impedance network is capacitive.


 
2. The amplification system of claim 1, wherein the first impedance network Z1 providing said first coupling path comprises a first resistor (281, 381, 581) connected between the output of said second amplifier and the load.
 
3. The amplification system of claim 2, wherein the second impedance network Z2 comprises a second capacitor (271, 371, 571).
 
4. The amplification system of claim 3, wherein the third impedance network Z3 providing said second coupling path comprises a second resistor (292, 392, 592) connected in parallel with said capacitor (291, 391, 591) between the output of the first amplifier and the load.
 
5. The amplification system of claim 4, wherein the fourth impedance network Z4 comprises a third capacitor (261, 361, 561) and third resistor (262, 362, 562) connected in series.
 
6. The amplification system of claim 1, wherein the third impedance network Z3 includes at least a first capacitor (291, 391, 591).
 
7. The amplification system of claim 1, wherein said second amplifier (250, 350, 550) is configured to operate in Class B mode, Class G mode or Class H mode.
 
8. The amplification system of claim 7, wherein said first amplifier (210, 310, 510) is configured to operate in Class AB mode.
 
9. The amplification system of claim 1, wherein the low pass filter comprises a T-network of two resistors and a capacitor connected between their common node and reference potential.
 
10. The amplification system of claim 1, wherein each of said first, second, third or fourth impedance networks Z1, Z2, Z3 and Z4 consists only of one or more resistors, one or more capacitors, or network combinations thereof.
 
11. The amplification system of claim 1, further comprising a fifth impedance network (356, 556) providing a feedback path from the load to the input of said first amplifier, said fifth impedance network comprising a low pass filter (R6, C7).
 
12. The amplification system of claim 1, wherein the values of the first, second, third and fourth impedance networks Z1, Z2, Z3, and Z4 satisfy the relationship Z1(s)•Z2(s) = Z3(s)•Z4(s).
 
13. The amplification system of claim 1, wherein a time constant of the third impedance network Z3 matches a time constant of the fourth impedance network Z4.
 
14. The amplification system of claim 13, wherein at high frequencies an impedance characteristic of impedance network Z3 appears capacitive in nature.
 
15. The amplification system of claim 14, wherein at low frequencies below which the impedance characteristic of said third impedance network Z3 appears capacitive, the impedance characteristic of the third impedance network Z3 appears resistive.
 
16. The amplification system of claim 1, wherein the fourth impedance network Z4 comprises a series resistor (262, 362, 562) and a series capacitor (261, 361, 561), and wherein a value of the series resistor is selected to provide a unity loop gain frequency to facilitate stability of the amplification system.
 


Ansprüche

1. Verstärkungssystem, umfassend:

einen ersten Verstärker (210, 310, 510), der betriebsfähig ist, ein Eingangsquellensignal (205, 305, 505) zu empfangen;

einen zweiten Verstärker (250, 350, 550), der dem ersten Verstärker nachgeschaltet ist;

ein erstes Impedanznetzwerk Z1, das den zweiten Verstärker an eine Last (245, 345, 545) koppelt;

ein zweites Impedanznetzwerk Z2, das betriebsfähig ist, einem Eingang (Vf) des ersten Verstärkers ein Gegenkopplungssignal bereitzustellen, das auf einen Ausgang des ersten Verstärkers hinweist;

ein drittes Impedanznetzwerk Z3, das an einem gemeinsamen Knoten mit dem ersten Impedanznetzwerk Z1 den Ausgang des ersten Verstärkers an die Last koppelt; und

ein viertes Impedanznetzwerk Z4, das betriebsfähig ist, dem Eingang des ersten Verstärkers ein Gegenkopplungssignal bereitzustellen, das auf einen Ausgang des zweiten Verstärkers hinweist;

wobei alle Impedanznetzwerke Z1, Z2, Z3 und Z4 Widerstände, Kondensatoren oder Netzwerkkombinationen davon beinhalten; dadurch gekennzeichnet, dass keines der Impedanznetzwerke Z1, Z2, Z3 und Z4 eine Ausgleichsinduktivität beinhaltet;

und die Impedanz des dritten Impedanznetzwerks kapazitiv ist.


 
2. Verstärkungssystem nach Anspruch 1, wobei das erste Impedanznetzwerk Z1, das den ersten Kopplungspfad bereitstellt, einen ersten Widerstand (281, 381, 581) umfasst, der zwischen den Ausgang des zweiten Verstärkers und die Last geschaltet ist.
 
3. Verstärkungssystem nach Anspruch 2, wobei das zweite Impedanznetzwerk Z2 einen zweiten Kondensator (271, 371, 571) umfasst.
 
4. Verstärkungssystem nach Anspruch 3, wobei das dritte Impedanznetzwerk Z3, das den zweiten Kopplungspfad bereitstellt, einen zweiten Widerstand (292, 392, 592) umfasst, der zwischen dem Ausgang des ersten Verstärkers und der Last mit dem Kondensator (291, 391, 591) parallel geschaltet ist.
 
5. Verstärkungssystem nach Anspruch 4, wobei das vierte Impedanznetzwerk Z4 einen dritten Kondensator (261, 361, 561) und einen dritten Widerstand (262, 362, 562), die in Reihe geschaltet sind, umfasst.
 
6. Verstärkungssystem nach Anspruch 1, wobei das dritte Impedanznetzwerk Z3 mindestens einen ersten Kondensator (291, 391, 591) beinhaltet.
 
7. Verstärkungssystem nach Anspruch 1, wobei der zweite Verstärker (250, 350, 550) konfigurierst ist, im Klasse-B-Modus, Klasse-G-Modus oder Klasse-H-Modus betrieben zu werden.
 
8. Verstärkungssystem nach Anspruch 7, wobei der erste Verstärker (210, 310, 510) konfiguriert ist, im Klasse-AB-Modus betrieben zu werden.
 
9. Verstärkungssystem nach Anspruch 1, wobei der Tiefpassfilter ein T-Netzwerk aus zwei Widerständen und einem Kondensator, die zwischen ihrem gemeinsamen Knoten und einem Referenzpotenzial verbunden sind, umfasst.
 
10. Verstärkungssystem nach Anspruch 1, wobei jedes von dem ersten, zweiten, dritten und vierten Impedanznetzwerk Z1, Z2, Z3 und Z4 nur aus einem oder mehreren Widerständen, einem oder mehreren Kondensatoren oder Netzwerkkombinationen davon besteht.
 
11. Verstärkungssystem nach Anspruch 1, ferner umfassend ein fünftes Impedanznetzwerk (356, 556), das einen Rückkopplungspfad von der Last zu dem Eingang des ersten Verstärkers bereitstellt, wobei das fünfte Impedanznetzwerk einen Tiefpassfilter (R6, C7) umfasst.
 
12. Verstärkungssystem nach Anspruch 1, wobei die Werte des ersten, zweiten, dritten und vierten Impedanznetzwerks Z1, Z2, Z3 und Z4 die Beziehung Z1(s)•Z2(s) = Z3(s)• Z4(s) erfüllen.
 
13. Verstärkungssystem nach Anspruch 1, wobei eine Zeitkonstante des dritten Impedanznetzwerks Z3 einer Zeitkonstante des vierten Impedanznetzwerks Z4 entspricht.
 
14. Verstärkungssystem nach Anspruch 13, wobei bei Hochfrequenzen eine Impedanzcharakteristik von Impedanznetzwerk Z3 in ihrer Art kapazitiv erscheint.
 
15. Verstärkungssystem nach Anspruch 14, wobei bei Niederfrequenzen, unter denen die Impedanzcharakteristik des dritten Impedanznetzwerks Z3 kapazitiv erscheint, die Impedanzcharakteristik des dritten Impedanznetzwerks Z3 ohmsch erscheint.
 
16. Verstärkungssystem nach Anspruch 1, wobei das vierte Impedanznetzwerk Z4 einen Reihenwiderstand (262, 362, 562) und einen Reihenkondensator (261, 361, 561) umfasst und wobei ein Wert des Reihenwiderstands ausgewählt ist, um eine Eins-Schleifenverstärkungsfrequenz bereitzustellen, um die Stabilität des Verstärkungssystems zu ermöglichen.
 


Revendications

1. Un système d'amplification, comprenant :

un premier amplificateur (210, 310, 510) conçu de façon à recevoir un signal source en entrée (205, 305, 505),

un deuxième amplificateur (250, 350, 550) raccordé en aval du premier amplificateur,

un premier réseau d'impédance Z1 couplant le deuxième amplificateur à une charge (245, 345, 545),

un deuxième réseau d'impédance Z2 conçu de façon à fournir un signal de rétroaction négatif indicatif d'une sortie du premier amplificateur vers une entrée (Vf) du premier amplificateur,

un troisième réseau d'impédance Z3 couplant la sortie du premier amplificateur à la charge au niveau d'un noeud commun avec le premier réseau d'impédance Z1, et

un quatrième réseau d'impédance Z4 conçu de façon à fournir un signal de rétroaction négatif indicatif d'une sortie du deuxième amplificateur vers l'entrée du premier amplificateur,

où la totalité desdits réseaux d'impédance Z1, Z2, Z3 et Z4 comprennent des résistances, des condensateurs, ou des combinaisons de réseau de ceux-ci, caractérisé en ce que

aucun des réseaux d'impédance Z1, Z2, Z3 et Z4 ne comprend un inducteur d'équilibrage,

et l'impédance du troisième réseau d'impédance est capacitive.


 
2. Le système d'amplification selon la Revendication 1, où le premier réseau d'impédance Z1 fournissant ledit premier trajet de couplage comprend une première résistance (281, 381, 581) raccordée entre la sortie dudit deuxième amplificateur et la charge.
 
3. Le système d'amplification selon la Revendication 2, où le deuxième réseau d'impédance Z2 comprend un deuxième condensateur (271, 371, 571).
 
4. Le système d'amplification selon la Revendication 3, où le troisième réseau d'impédance Z3 fournissant ledit deuxième trajet de couplage comprend une deuxième résistance (292, 392, 592) raccordée en parallèle audit condensateur (291, 391, 591) entre la sortie du premier amplificateur et la charge.
 
5. Le système d'amplification selon la Revendication 4, où le quatrième réseau d'impédance Z4 comprend un troisième condensateur (261, 361, 561) et une troisième résistance (262, 362, 562) raccordés en série.
 
6. Le système d'amplification selon la Revendication 1, où le troisième réseau d'impédance Z3 comprend au moins un premier condensateur (291, 391, 591).
 
7. Le système d'amplification selon la Revendication 1, où ledit deuxième amplificateur (250, 350, 550) est configuré de façon à fonctionner en mode Classe B, en mode Classe G ou en mode Classe H.
 
8. Le système d'amplification selon la Revendication 7, où ledit premier amplificateur (210, 310, 510) est configuré de façon à fonctionner en mode Classe AB.
 
9. Le système d'amplification selon la Revendication 1, où le filtre passe-bas comprend un réseau en T de deux résistances et un condensateur raccordés entre leur noeud commun et un potentiel de référence.
 
10. Le système d'amplification selon la Revendication 1, où chacun desdits premier, deuxième, troisième ou quatrième réseaux d'impédance Z1, Z2, Z3 et Z4 se compose uniquement d'une ou de plusieurs résistances, d'un ou de plusieurs condensateurs, ou de combinaisons de réseau de ceux-ci.
 
11. Le système d'amplification selon la Revendication 1, comprenant en outre un cinquième réseau d'impédance (356, 556) fournissant un trajet de rétroaction de la charge vers l'entrée dudit premier amplificateur, ledit cinquième réseau d'impédance comprenant un filtre passe-bas (R6, C7).
 
12. Le système d'amplification selon la Revendication 1, où les valeurs des premier, deuxième, troisième et quatrième réseaux d'impédance Z1, Z2, Z3 et Z4 satisfont la relation Z1(s)•Z2(s) = Z3(s)•Z4(s).
 
13. Le système d'amplification selon la Revendication 1, où une constante temporelle du troisième réseau d'impédance Z3 correspond à une constante temporelle du quatrième réseau d'impédance Z4.
 
14. Le système d'amplification selon la Revendication 13, où, à des fréquences élevées, une caractéristique d'impédance du réseau d'impédance Z3 apparaît capacitive par nature.
 
15. Le système d'amplification selon la Revendication 14, où, à des basses fréquences sous lesquelles la caractéristique d'impédance dudit troisième réseau d'impédance Z3 apparaît capacitive, la caractéristique d'impédance du troisième réseau d'impédance Z3 apparaît résistive.
 
16. Le système d'amplification selon la Revendication 1, où le quatrième réseau d'impédance Z4 comprend une résistance en série (262, 362, 562) et un condensateur en série (261, 361, 561), et où une valeur de la résistance en série est sélectionnée de façon à fournir une fréquence de gain en boucle unitaire destinée à favoriser la stabilité du système d'amplification.
 




Drawing























Cited references

REFERENCES CITED IN THE DESCRIPTION



This list of references cited by the applicant is for the reader's convenience only. It does not form part of the European patent document. Even though great care has been taken in compiling the references, errors or omissions cannot be excluded and the EPO disclaims all liability in this regard.

Patent documents cited in the description




Non-patent literature cited in the description