The present invention relates to an amplifier whose gain changes depending on the change of a power source voltage and more particularly to an angular velocity sensor apparatus incorporating this amplifier.
Although various amplifiers, such as DC amplifiers and high-frequency amplifiers, are used for electronic devices, it is general that the voltage of the DC power source of such an amplifier is stabilized and maintained constant. The amplifier can have stable characteristics by maintaining the voltage of the power source constant.
However, electronic devices mounted on mobile bodies, such as automobiles, and used in severe environmental conditions have a problem wherein the power source voltage having been stabilized once varies owing to load variation and external noise. In recent automobiles, many sensors are used for automobile body control and safety devices, such as an attitude control system and an antilock brake system (ABS). The output signals of the most of these sensors are analog signals. Such an analog signal is required to be converted into a digital signal by using an AD converter so that data processing is performed by using a microcomputer on the basis of the analog signal and predetermined judgments and control are carried out.
A reference voltage (VREF) is usually required in the case when AD conversion is carried out. The same reference voltage as VREF is also required on the side of a sensor outputting a signal to be AD converted. Hence, in the case when an AD converter is away from the sensor, a wire connected to a reference voltage source is required in addition to a power source wire, a grounding wire and a signal output transmission wire. However, the number of wires in electronic devices for automobiles and the like is required to be decreased in view of cost and reliability. Hence, it is general that no reference voltage source is provided and that the voltage of the DC power source is used as the reference voltage.
In this kind of electronic device, when the power source voltage rises while the detection output of the sensor is constant, the AD converter carries out AD conversion on the basis of the raised power source voltage. As a result, the digital output obtained after the AD conversion lowers as if the detection output of the sensor is decreased. Hence, if the AD conversion is carried out in this way, no correct detection data is obtainable. The correct detection data is obtainable by increasing the power source voltage by 10% for example, so that the detection output of the sensor is increased by 10%, and the increased detection output is then input to the AD converter. With this measure the variation of power source voltage is cancelled, whereby the converted digital output properly corresponds to the analog detection output of the sensor.
As described above, a sensor mounted on an automobile or the like is required to have a characteristic wherein its output varies in proportion to the power source voltage.
Since it was difficult to attain a highly accurate amplifier having this kind of characteristic in conventional electronic devices for automobiles and the like, the sensitivity itself of the sensor has been made proportional to the power source voltage.
As an example of conventional electronic devices for automobiles, an angular velocity sensor apparatus for detecting the rocking of an automobile body has been used to control the attitude of an automobile. The configuration and operation of a conventional angular velocity sensor apparatus will be described below referring to
Referring to
A terminal 133 connected to the level detection element 102 of the angular velocity sensor 10 is connected to the input terminal of a first amplifier 111. An input signal Vin owing to the charge generated on the surface of the level detection element 102 is input to the first amplifier 111. The output voltage Vm of the first amplifier 111 is input to a rectifier 122, a variable gain amplifier 125 and a phase detector 127. The output voltage Vm is rectified by the rectifier 122, smoothened by a smoothing circuit 123 comprising a resistor 143 and a capacitor 144 and input to the negative input terminal of the adder 125a of the variable gain amplifier 125. The comparison voltage Vr of a comparison voltage generation circuit 114 is applied to the positive input terminal of the adder 125a. The comparison voltage generation circuit 114 comprises two resistors 141 and 142 having the same resistance value and connected in series. The resistors 141 and 142 connected in series are further connected between a power source VDD and a circuit ground Gr. Half of the power source voltage is output as the comparison voltage Vr. The adder 125a applies the voltage difference between the output voltage of the smoothing circuit 123 and the comparison voltage Vr to an amplifier 125b that is capable of changing its gain by virtue of voltage control in the variable gain amplifier 125. The gain of the amplifier 125b is controlled by the voltage difference between the two voltages input to the adder 125a. An output signal obtained by this control is applied from the drive terminal 130 of the angular velocity sensor 10 to the drive element 101 and drives this element.
Since the output of the first amplifier 111 is amplified by the variable gain amplifier 125 and applied from the terminal 130 of the angular velocity sensor 10 to the drive element 101, the loop circuit circuit including the first amplifier 111, the rectifier 122, the smoothing circuit 123, the variable gain amplifier 125 and the angular velocity sensor 10 forms a sinusoidal oscillation circuit having an automatic gain control function. This loop circuit circuit is hereafter referred to as an “AGC loop circuit circuit.” The amplitude of the output voltage Vm of the first amplifier 111 is controlled so as to become constant by the AGC loop circuit circuit.
With the above-mentioned configuration, the angular velocity sensor 10 carries out tuning-fork vibration with a constant amplitude without being affected by variations in the characteristics of the elements and changes in temperature. In addition, the angular velocity sensor 10 attains high angular velocity detection sensitivity without being affected by variations in the characteristics of the elements and changes in temperature.
The comparison voltage Vr of the comparison voltage generation circuit 114 shown in
Hence, the amplitude of the output voltage Vm always becomes a sinusoidal voltage having an amplitude proportional to the power source voltage Vdd. When the first amplifier 111 and the rectifier 122 are configured so as not to depend on the power source voltage Vdd, the output signal of the level detection element 102 of the angular velocity sensor 10, that is, the input signal Vin of the first amplifier 111, also becomes a voltage proportional to the power source voltage Vdd as the output voltage Vm does. The level variation of the voltage of each of the detection elements 103 and 104 is proportional to the amplitude of the sinusoidal wave output from the level detection element 102. Hence, an angular velocity output signal, which is obtained when signal of the level variation is detected by the phase detector 127, amplified by a DC amplifier 118 and output to an output terminal 119, also becomes proportional to the power source voltage Vdd. As a result, it is possible to obtain an amplifier device whose gain changes in proportion to the power source voltage Vdd.
The operation of the amplifier device shown in
Since the angular velocity sensor 10 is an element generating mechanical vibration, it has a characteristic of functioning as a mechanical filter, a relatively larger time constant, and a relatively slow response speed. In addition, the smoothing circuit comprising the resistor 143 and the capacitor 144 is a low-pass filter having a large time constant. Hence, the response speed of the AGC loop circuit circuit including the angular velocity sensor 10, the amplifier 111, the rectifier 122, the smoothing circuit 123 and the variable gain amplifier 125 to disturbance is relatively low. In other words, its response frequency is relatively low. An example of the response characteristic is shown in the graph of
In the graph of
The response speed of the AGC loop circuit circuit is increased by raising the gain of the AGC loop circuit circuit. However, when the gain is raised, the variation ratio of the input voltage Vin with respect to the power source voltage Vdd increases, whereby the voltage variation ratio at the resonance frequency fr increases further.
In the conventional circuit shown in
The present invention is intended to provide an amplifier whose response speed is high and whose gain is proportional to a power source voltage such that even when the power source voltage varies abruptly, the gain changes so as to follow the variation of the power source voltage, and an output voltage depending on the variation of the power source voltage is obtained.
An amplifier in accordance with the present invention whose gain is proportional to a power source voltage comprises first and second P-channel MOS field-effect transistors (hereafter abbreviated to MOS-FETs) whose respective back gates are formed so as to be electrically isolated from a semiconductor substrate and whose respective sources are connected in common, a first voltage source for outputting a voltage obtained by dividing a power source voltage, a second voltage source for generating a positive voltage having a potential difference almost identical to the threshold voltages of the above-mentioned first and second MOS-FETs with reference to the output voltage of the above-mentioned first voltage source, a third voltage source for generating a predetermined negative voltage with reference to the output voltage of the above-mentioned first voltage source, and an operational amplifier, to the positive input terminal of which the output of the above-mentioned second voltage source is applied as a bias voltage. The sources of the above-mentioned first and second MOS-FETs, connected in common, are connected to the negative input terminal of the above-mentioned operational amplifier, and the respective back gates of the above-mentioned first and second MOS-FETs are connected to either their respective sources or the above-mentioned second voltage source. The gate of the above-mentioned first MOS-FET is biased at the potential of a circuit ground, and its drain is connected to an input terminal to which a signal with no DC component is input. The gate of the above-mentioned second MOS-FET is connected to the above-mentioned third voltage source, and its drain is connected to the output terminal of the above-mentioned operational amplifier, which leads to the output terminal of the above-mentioned amplifier.
In accordance with the present invention, the gain of the amplifier changes in proportion to a power source voltage. Therefore, when each of analog detection outputs of various sensors is amplified by using this amplifier, the amplified detection output changes depending on the change of the power source voltage. Hence, even when the power source voltage is used as a reference voltage when an analog detection output is AD converted, it is possible to obtain a digital output properly corresponding to the above-mentioned analog detection output. Since the frequency characteristic of the amplifier is sufficiently high (extending to a high frequency range), particularly when the amplifier is used for various sensors mounted on vehicles, the amplifier has a sufficient response speed, thereby being applicable to various high-speed operation sensors.
An amplifier in accordance with another aspect of the present invention whose gain is proportional to a power source voltage comprises first and second N-channel MOS-FETs whose respective back gates are formed so as to be electrically isolated from a semiconductor substrate and whose respective sources are connected in common, a first voltage source for outputting a voltage obtained by dividing a power source voltage, a second voltage source for generating a negative voltage having a potential difference almost identical to the threshold voltages of the above-mentioned first and second MOS-FETs with reference to the output voltage of the above-mentioned first voltage source, a third voltage source for generating a predetermined positive voltage with reference to the output voltage of the above-mentioned first voltage source, and an operational amplifier, to the positive input terminal of which the output of the above-mentioned second voltage source is applied as a bias voltage. The sources of the above-mentioned first and second MOS-FETs, connected in common, are connected to the negative input terminal of the above-mentioned operational amplifier. The respective back gates of the above-mentioned first and second MOS-FETs are connected to either their respective sources or the output terminal of the above-mentioned second voltage source, the gate of the above-mentioned first MOS-FET is connected to the above-mentioned positive power source voltage, and its drain is connected to an input terminal to which a signal with no DC component is input. The gate of the above-mentioned second MOS-FET is connected to the above-mentioned third voltage source, and its drain is connected to the output terminal of the above-mentioned operational amplifier, which leads to the output terminal of the above-mentioned amplifier.
In accordance with the present invention, the gain of the amplifier changes in proportion to a power source voltage. Therefore, when each of analog detection outputs of various sensors is amplified by using this amplifier, the amplified detection output changes depending on the change of the power source voltage. Hence, even when the power source voltage is used as a reference voltage when an analog detection output is AD converted, it is possible to obtain a digital output properly corresponding to the above-mentioned analog detection output. Since the frequency characteristic of the amplifier is sufficiently high, particularly when the amplifier is used for various sensors mounted on vehicles, the amplifier has a sufficient response speed, thereby being applicable to various high-speed operation sensors.
An amplifier in accordance with another aspect of the present invention whose gain is proportional to a power source voltage comprises first and second P-channel MOS-FETs whose respective back gates are formed so as to be electrically isolated from a semiconductor substrate and whose respective sources are connected in common, a first voltage source for outputting a voltage obtained by dividing a power source voltage, a second voltage source for generating a positive voltage having a potential difference almost identical to the threshold voltages of the above-mentioned first and second MOS-FETs with reference to the output voltage of the above-mentioned first voltage source, a third voltage source for generating a predetermined negative voltage with reference to the output voltage of the above-mentioned first voltage source, and first and second operational amplifiers whose respective positive input terminals are connected to the above-mentioned second voltage source. The sources of the above-mentioned first and second MOS-FETs, connected in common, are connected to the output terminal of the above-mentioned first operational amplifier, and the respective back gates of the above-mentioned first and second MOS-FETs are connected to either their respective sources or the above-mentioned second voltage source. The gate of the above-mentioned first MOS-FET is connected to the above-mentioned third voltage source, and its drain is connected to the negative input terminal of the above-mentioned first operational amplifier and to an input terminal to which a signal with no DC component is input. The gate of the above-mentioned second MOS-FET is connected to a circuit ground, and its drain is connected to the negative input terminal of the above-mentioned second operational amplifier. A resistor is connected between the negative input terminal of the above-mentioned second operational amplifier and the output terminal of the above-mentioned second operational amplifier, which leads to the output terminal of the above-mentioned amplifier.
In accordance with the present invention, the gain of the amplifier changes in proportion to a power source voltage. Therefore, when each of analog detection outputs of various sensors is amplified by using this amplifier, the amplified detection output changes depending on the change of the power source voltage. Hence, even if the power source voltage is used as a reference voltage when an analog detection output is AD converted, it is possible to obtain a digital output properly corresponding to the above-mentioned analog detection output. In the case when an input signal is a current signal, the first operational amplifier and the first MOS-FET serving as its feedback resistor operate as a current-voltage converter. In addition, the second operational amplifier, the second MOS-FET and the resistor form an ordinary inverting amplifier. Hence, the gain between the input terminal and the output terminal is the product of the gain of the current-voltage converter and the gain of inverting amplifier, allowing to obtain a large gain.
An amplifier in accordance with another aspect of the present invention whose gain is proportional to a power source voltage comprises first and second P-channel MOS-FETs whose respective back gates are formed so as to be electrically isolated from a semiconductor substrate and whose respective sources are connected in common, third and fourth P-channel MOS-FETs whose respective sources are connected in common, a first voltage source for outputting a voltage obtained by dividing a power source voltage, a second voltage source for generating a positive voltage having a potential difference almost identical to the threshold voltages of the above-mentioned first, second, third and fourth MOS-FETs with reference to the output voltage of the above-mentioned first voltage source, a third voltage source for generating a predetermined negative voltage with reference to the output voltage of the above-mentioned first voltage source, first and second operational amplifiers whose positive input terminals are connected in common and biased by the above-mentioned second voltage source, the first and second P-channel MOS-FETs whose respective sources are connected in common and further connected to the output terminal of the above-mentioned first operational amplifier, and the third and fourth P-channel MOS-FETs whose respective sources are connected in common and further connected to the output terminal of the above-mentioned second operational amplifier. The respective back gates of the above-mentioned first, second, third and fourth MOS-FETs are connected to either their respective sources or the above-mentioned second voltage source, and the gates of the above-mentioned first and third MOS-FETs are connected to the above-mentioned third voltage source. The drain of the above-mentioned first MOS-FET is connected to the negative input terminal of the above-mentioned first operational amplifier and to a first input terminal to which a signal with no DC component is input. The drain of the above-mentioned third MOS-FET is connected to the negative input terminal of the above-mentioned second operational amplifier and to a second input terminal to which a signal with no DC component is input. The gates of the above-mentioned second and fourth MOS-FETs are connected to a circuit ground, and the drain of the above-mentioned second MOS-FET is connected to the positive input terminal of the above-mentioned third operational amplifier. The drain of the above-mentioned fourth MOS-FET is connected to the negative input terminal of the above-mentioned third operational amplifier, the above-mentioned second voltage source is connected to the positive input terminal of the above-mentioned third operational amplifier via a first resistor, and a second resistor is connected between the negative input terminal of the above-mentioned third operational amplifier and the output terminal of the above-mentioned third operational amplifier, which leads to the output terminal of the above-mentioned amplifier.
In accordance with the present invention, the gain of the amplifier changes in proportion to a power source voltage. When each of analog detection outputs of various sensors is amplified by using this amplifier, the amplified detection output changes depending on the change of the power source voltage. Hence, even if the power source voltage is used as a reference voltage when an analog detection output is AD converted, it is possible to obtain a digital output properly corresponding to the above-mentioned analog detection output. Since the frequency characteristic of the amplifier is sufficiently high, particularly when the amplifier is used for various sensors mounted on vehicles, the amplifier has a sufficient response speed, thereby being applicable to various high-speed operation sensors. Further, the amplifier has two input terminals of a first input terminal and a second input terminal, thereby being applicable also to sensors having two output terminals such as angular velocity sensors.
An angular velocity sensor apparatus in accordance with the present invention comprises a drive section for vibrating vibration elements, a vibration level detection section for detecting the vibration levels of the above-mentioned vibration elements, Coriolis force detection sections for detecting a Coriolis force generating depending on an angular velocity, a first amplifier for amplifying the output signal of the above-mentioned vibration level detection section, a rectifying circuit for rectifying the output signal of the above-mentioned first amplifier to obtain a DC voltage, a variable gain amplifier, receiving the output signal of the above-mentioned first amplifier, for changing its amplification degree depending on the output value of the above-mentioned rectifying circuit, a second amplifier for amplifying the output signals of the above-mentioned Coriolis force detection sections, a phase detector for detecting the phase of the output voltage of the above-mentioned second amplifier on the basis of the vibration frequencies of the above-mentioned vibration elements, and a DC amplifier for DC amplifying the output of the above-mentioned phase detector. The above-mentioned second amplifier comprises at least two operational amplifiers, and at least two MOS-FETs in which the drain-source voltage is biased at 0 V, wherein one of the above-mentioned MOS-FETs is biased so that the gate-source voltage becomes constant, and the other MOS-FET is biased so that the gate-source voltage changes depending on the variation of a power source voltage, and the gains of the above-mentioned operational amplifiers are determined by the ratio of the channel resistances of the above-mentioned at least two MOS-FETs biased by the above-mentioned voltages different from each other.
An angular velocity sensor apparatus in accordance with another aspect of the present invention comprises a drive section for vibrating vibration elements, a vibration level detection section for detecting the vibration levels of the above-mentioned vibration elements, Coriolis force detection sections for detecting a Coriolis force generating depending on an angular velocity, a first amplifier for amplifying the output signal of the above-mentioned vibration level detection section, a rectifying circuit for rectifying the output signal of the above-mentioned first amplifier to obtain a DC voltage, a variable gain amplifier, receiving the output signal of the above-mentioned first amplifier, for changing its amplification degree depending on the output value of the above-mentioned rectifying circuit, a second amplifier for amplifying the output signals of the above-mentioned Coriolis force detection sections, a phase detector for detecting the phase of the output voltage of the above-mentioned second amplifier on the basis of the vibration frequencies of the above-mentioned vibration elements, and a DC amplifier for DC amplifying the output of the above-mentioned phase detector.
The above-mentioned second amplifier whose respective back gates are formed so as to be electrically isolated from a semiconductor substrate and whose respective sources are connected in common, third and fourth P-channel MOS-FETs whose respective sources are connected in common, a first voltage source for outputting a voltage obtained by dividing a power source voltage, a second voltage source for generating a positive voltage having a potential difference almost identical to the threshold voltages of the above-mentioned first, second, third and fourth MOS-FETs with reference to the output voltage of the above-mentioned first voltage source, a third voltage source for generating a predetermined negative voltage with reference to the output voltage of the above-mentioned first voltage source, first and second operational amplifiers whose positive input terminals are connected in common and biased by the above-mentioned second voltage source, the first and second P-channel MOS-FETs whose respective sources are connected in common and further connected to the output terminal of the above-mentioned first operational amplifier, and the third and fourth P-channel MOS-FETs whose respective sources are connected in common and further connected to the output terminal of the above-mentioned second operational amplifier. The respective back gates of the above-mentioned first, second, third and fourth MOS-FETs are connected to either their respective sources or the above-mentioned second voltage source, and the gates of the above-mentioned first and third MOS-FETs are connected to the above-mentioned third voltage source. The drain of the above-mentioned first MOS-FET is connected to the negative input terminal of the above-mentioned first operational amplifier and to a first input terminal to which a signal with no DC component is input. The drain of the above-mentioned third MOS-FET is connected to the negative input terminal of the above-mentioned second operational amplifier and to a second input terminal to which a signal with no DC component is input. The gates of the above-mentioned second and fourth MOS-FETs are connected to a circuit ground, the drain of the above-mentioned second MOS-FET is connected to the positive input terminal of the above-mentioned third operational amplifier, and the drain of the above-mentioned fourth MOS-FET is connected to the negative input terminal of the above-mentioned third operational amplifier. The above-mentioned second voltage source is connected to the positive input terminal of the above-mentioned third operational amplifier via a first resistor, and a second resistor is connected between the negative input terminal of the above-mentioned third operational amplifier and the output terminal of the above-mentioned third operational amplifier, which leads to the output terminal of the above-mentioned amplifier. According to the present invention, an amplifier having a sufficiently high frequency characteristics and whose gain changes in proportion to a power source voltage is used as the second amplifier, thereby making it possible to provide an angle velocity sensor having a high response speed.
a is a graph showing the relationship between the power source voltage and time in the angular velocity sensor apparatus shown in
b is a graph showing the relationship between the output voltage (Vm) of the amplifier and time in the angular velocity sensor apparatus shown in
c is a graph showing the relationship between the output voltage (Vout) indicating an angular velocity and time in the angular velocity sensor apparatus shown in
a is the graph showing the relationship between the power source voltage and time in the conventional angular velocity sensor apparatus shown in
b is the graph showing the relationship between the output voltage of the amplifier and time in the conventional angular velocity sensor apparatus shown in
c is the graph showing the relationship between the output voltage indicating an angular velocity and time in the conventional angular velocity sensor apparatus shown in
Preferred embodiments in accordance with the present invention will be described below referring to
<<First Embodiment>>
An amplifier whose gain is proportional to a power source voltage (hereafter referred to as a power source voltage proportional amplifier) in accordance with a first embodiment of the present invention will be described below referring to
In
The operation of the power source voltage proportional amplifier in accordance with this embodiment configured as described above will be described below. Since no DC current flows into the drain of the MOS-FET 21, the negative input terminal (−), the output terminal 52 and the positive input terminal (+) of the operational amplifier 61 have the same potential.
While an MOS-FET, such as the MOS-FETs 21 and 22, operates in an unsaturated state, its drain current Ids is generally represented by the following equation (1).
Ids=β·{(Vgs−Vth)·Vds−(Vds)2/2} (1)
wherein β is a mutual conductance per unit gate voltage, Vgs is a gate-source voltage, Vth is a gate-source threshold voltage at the time when the MOS-FET turns on, and Vds is a drain-source voltage. In addition, the ON resistance Ron of the MOS-FET is the inverse number of a value obtained by differentiating the drain current Ids obtained according to the equation (1) with respect to the drain-source voltage Vds, and is represented by equation (2).
Ron=1/(dIds/dVds) (2)
From the equations (1) and (2), equation (3) is obtained.
dIds/dVds=β·{(Vgs−Vth)−Vds} (3)
In the case when no bias voltage is applied between the drain and source, that is, in the case of zero bias, the drain-source voltage Vds is zero. Hence, the second term on the right side of the equation (3) disappears. As a result, the equation (2) becomes equation (4).
Ron=1/{β·(Vgs−Vth)} (4)
According to the equation (4), it is found that the ON resistance Ron of the MOS-FET is inversely proportional to the product of the mutual conductance β and the voltage difference (Vgs−Vth) when the drain-source voltage Vds is zero. Since the mutual conductance β is determined by the production process and the size of each of the MOS-FETs 21 and 22, it is a constant value. When the ON resistance Ron of the MOS-FET is used as an input resistance for determining the gain of an operational amplifier, a circuit wherein the voltage difference (Vgs−Vth) serving as a bias voltage is proportional to the power source voltage Vdd is configured, whereby it is found that an amplifier whose gain is proportional to the power source voltage Vdd is obtained.
In the bias circuit 11 shown in
To the source of the MOS-FET 23, a constant minute current (constant current) flows from the constant current source 13 connected to the power source VDD. By this constant current, a bias current corresponding to the threshold voltages Vth of the MOS-FETs 21 and 22 is generated between the output voltage 11a of the operational amplifier 60 and the positive input terminal (+) of the operational amplifier 61, whereby the input DC bias of the, operational amplifier 61 is level-shifted. Hence, the threshold voltages Vth of the MOS-FETs 21 and 22 are cancelled. It is desired that the value of the constant current should be as small as possible. It is also desired that the gate width of the MOS-FET 23 should be as large as possible.
The gate bias voltage of the MOS-FET 22 operating as the feedback resistor of the operational amplifier 61 of the amplifier circuit 20a is made negative with reference to the output voltage of the operational amplifier 60. This negative voltage is applied from the constant voltage source 12. With the above-mentioned configuration, the ON resistance of the MOS-FET 22 does not change even if the bias voltages of the negative input terminal (−) and the positive input terminal (+) of the operational amplifier 61 varies depending on the variation of the power source voltage Vdd. On the other hand, the ON resistance of the MOS-FET 21 decreases in inverse proportion to the power source voltage Vdd. By virtue of the above-mentioned operation, the gain of the amplifier circuit 20a having the MOS-FETs 21 and 22 and the operational amplifier 61 becomes proportional to the power source voltage Vdd.
The source potential Vso of the MOS-FETs 21 and 22 is a bias voltage of the negative input terminal (−) of the operational amplifier 61 with respect to the circuit ground Gr and is represented by the following equation (5).
Vso={R45/(R44+R45)}·Vdd−Vgs23 (5)
wherein R44 and R45 are the resistance values of the resistors 44 and 45, respectively, and Vdd is the power source voltage. Vgs23 is the gate-source voltage of the MOS-FET 23 and its polarity is negative since the FET is a P-channel FET.
Using the gate-source voltage Vgs and the threshold voltage Vth, the drain-source current Ids of the MOS-FET 23 is represented by the following general equation (6) when the operation of the MOS-FET is saturated.
Ids=(β/2)·(Vgs−Vth)2 (6)
When it is assumed that the drain-source current of the MOS-FET 23 is Ids23, that the mutual conductance per unit gate voltage thereof is β23 and that the gate-source voltage thereof is Vgs23, the equation (6) becomes the following equation (6A).
Ids23=(β23/2)·(Vgs23−Vth)2 (6A)
When the equation (6A) is solved with respect to the gate-source voltage Vgs23, equation (7) is obtained.
Vgs23 =√{square root over (2·Ids23/β23)}+Vth (7)
In the case when the ratio 2·Ids23/β23 in the equation (7) is far smaller than the threshold voltage Vth, that is, when 2·Ids23/β23<<Vth, the equation (7) becomes equation (8).
Vgs23≈Vth (8)
In order that the ratio 2·Ids23/β23 is made small, the current supplied from the constant current source 13 is decreased, the channel length of the gate of the MOS-FET 23 is decreased as small as possible and the channel width thereof is increased as large as possible as detailed later. The condition of the equation (8) can thus be attained.
The gate-source voltage Vgs21 of the MOS-FET 21 is represented by equation (9) using the equations (5) and (8).
Vgs21=Vth−{R45/(R44+R45)}·Vdd (9)
When it is assumed that the mutual conductance per unit gate voltage is β21, the ON resistance Ron21 of the MOS-FET 21 is obtained by substituting Vgs21 in Vgs of the equation (4), as represented by equation (10).
Ron21=1/[−β21·{R45/(R44+R45)}·Vdd] (10)
According to the equation (10), it is found that the threshold voltage Vth is eliminated and that the ON resistance Ron is inversely proportional to the power source voltage Vdd. The minus sign is attached to β21 since the MOS-FET 21 is a P-channel FET and β21 itself is negative.
When similar calculations are carried out for the MOS-FET 22, the gate-source voltage Vgs22 can be represented by equation (11).
Vgs22={R45/(R44+R45)}·Vdd−V12−Vso (11)
wherein V12 is the voltage value of the constant voltage source 12. When Vso of the equation (5) is substituted and the equation (11) is arranged, the equation (11) becomes equation (12).
Vgs22=−V12+Vgs23 (12)
In a similar manner to the MOS-FET 21, when a mutual conductance of the MOS-FET 22 per unit gate voltage in β22, the ON resistance Ron22 of the MOS-FET 22 is represented by equation (13) obtained by substituting Vgs22 in Vgs of the equation (4).
Ron22=1/{β22·(−V12+Vgs23−Vth)} (13)
Since Vgs23≈Vth according to the equation (8), Vgs23 and Vth in the equation (13) are offset with each other, whereby the equation (13) becomes equation (14).
Ron22=1/{β22·(−V12)} (14)
Since the voltage V12 of the constant voltage source 12 is constant, it is found according to the equation (14) that the ON resistance of the MOS-FET 22 is constant regardless of the power source voltage Vdd.
In order that the gain G between the input terminal 51a and the output terminal 52 of the amplifier circuit 20a shown in
G=Ron22/Ron21 (15)
G=(β21/β22)·{R45/(R44+R45)}·(Vdd/V12) (16)
When the value of the resistor 44 is the same as that of the resistor 45, that is, when R44=R45, the equation (16) is simplified to equation (17).
G=(β21/β22)·{Vdd/(2·V12)} (17)
Since the power source voltage Vdd is included in the numerator of the equation indicating the gain G as indicated in the equation (16) and the equation (17), the gain G is proportional to the power source voltage Vdd.
In the power source voltage proportional amplifier in accordance with this embodiment described above, the circuit comprising the P-channel MOS-FETs 21, 22 and 23 is explained as an example. However, even when N-channel MOS-FETs are used, the power source voltage proportional amplifier in accordance with this embodiment can be configured similarly.
It can be understood easily that the gain becomes inversely proportional to the power source voltage Vdd when the gate biases of the MOS-FETs 21 and 22 of P-channel are reversed.
In
The P-channel MOS-FETs 21, 22 and 23 for this embodiment are semiconductor devices having a well-known structure. The structure will be described briefly referring to a cross-sectional view in
Since a zero bias is applied between the source and the drain in this embodiment, almost identical characteristics are obtained actually even if the source terminal 76 and the drain terminal 77 are replaced with each other. However, even if the DC bias voltage is 0 V, if the level of a signal to be applied is high, a small potential difference is generated between the source and the drain. When the potential difference is about 0.1 V, for example, no problem occurs. However, as the potential difference becomes larger than this value, errors occur in the above-mentioned calculation equations.
In addition, the size of the channel significantly affects the characteristics of the MOS-FET as explained below. The mutual conductance β per unit gate voltage, used in the above-mentioned equation (1), and the size of the channel have the relationship indicated by the following equation (18).
β∝(W/L) (18)
wherein W/L represents the dimension ratio of the channel region CH in the back gate 71 facing the polysilicon film 75 in
According to the equation (18), it is found that the ON resistance of the MOS-FET, such as the MOS-FETs 21 and 22, configured as shown in
In addition, the calculations in accordance with the above-mentioned calculation equations are carried out on the assumption that the potential of the back gate terminal 79 of each of the MOS-FETs 21, 22 and 23 is identical to that of the source terminal 76 thereof. However, it is not always necessary that the respective back gate terminals 79 are connected in common with their corresponding source terminals 76. The potentials of the back gate terminals 79 of the MOS-FETs 21, 22 and 23 should only be identical to one another. Since the structure of the MOS-FET 23 of the bias circuit 14 is identical to those of the MOS-FETs 21 and 22, the threshold voltages of the MOS-FETs 21, 22 and 23 change similarly at all times. As a result, when the potentials of all the source terminals 76 of the MOS-FETs are the same, the variation of the threshold voltage owing to the back-gate effect is cancelled. However, as the threshold voltage becomes higher owing to the back-gate effect, the accuracy of proportion at the time when the gain is proportional to the power source voltage becomes worse.
<<Second Embodiment>>
A power source voltage proportional amplifier in accordance with a second embodiment of the present invention will be described referring to
As shown in
As indicated in the above-mentioned equation (15), the gain G of the power source voltage proportional amplifier in accordance with the first embodiment is represented by the ratio of the ON resistances of the MOS-FETs 21 and 22, that is, the ratio Ron(22)/Ron(21). Similarly, the gain G of the power source voltage proportional amplifier in accordance with the second embodiment is represented by the ratio of the ON resistances of the MOS-FETs 24 and 25, that is, Ron(25)/Ron(24). In the case when the relationship between the MOS-FETs 21 and 22 are reversed in the first embodiment, that is, when the gate connections of the MOS-FETs 21 and 22 are replaced with each other so that the gate bias voltage of the MOS-FET 21 is fixed and so that the gate bias voltage of the MOS-FET 22 is proportional to the power source voltage Vdd, the ON resistance of the MOS-FET 22 serving as a feedback resistor changes in inversely proportional to the power source voltage Vdd. In the case when the relationship between the MOS-FETs 24 and 25 are reversed in the second embodiment, that is, when the gate connections of the MOS-FETs 24 and 25 are replaced with each other so that the gate bias voltage of the MOS-FET 24 is fixed and so that the gate bias voltage of the MOS-FET 25 is proportional to the power source voltage Vdd, the ON resistance of the MOS-FET 25 serving as a feedback resistor changes in inversely proportional to the power source voltage Vdd. As a result, it is possible to obtain an amplifier whose gain is inversely proportional to the power source voltage Vdd.
<<Third Embodiment>>
A power source voltage proportional amplifier in accordance with a third embodiment of the present invention will be described referring to a circuit diagram shown in
For example, a detection element of an angle velocity sensor having a tuning fork structure is an element of outputting current. When an input current flows into the input terminal 51, the operational amplifier 64 and the MOS-FET 31 serving as the feedback resistor of the operational amplifier 64 operate as a current-voltage converter. In addition, the operational amplifier 65, the MOS-FET 32 and the resistor 46 form an ordinary inverting amplifier. Hence, the gain G between the input terminal 51 and the output terminal 52 is the product of the gain of the current-voltage converter and the gain of inverting amplifier. The gain G is thus obtained by using the following equations (19) to (26).
It is assumed that an input signal is a current signal that is input from, for example, an angular velocity sensor having a tuning-fork structure and serving as a signal source. The dependence of the output voltage V52 of the output terminal 52 on the power source voltage Vdd of the power source VDD is calculated. Assuming that the open loop gains of the operational amplifiers 64 and 65 are very high, the following three equations (19), (20) and (21) are established.
V52=V64·G65 (19)
V64=Iin·Ron31 (20)
G65=R46/Ron32 (21)
wherein V64 is the output voltage of the operational amplifier 64, G65 is the gain of the operational amplifier 65, Iin is the current of the signal from the signal source, Ron31 is the ON resistance of the MOS-FET 31, Ron32 is the ON resistance of the MOS-FET 32, and R46 is the resistance value of the resistor 46. Since the ON resistance of the MOS-FET is as explained before in detail referring to
Ron31=1/{β31·(−V12)} (22)
Ron32=1/[−β32·{R45/(R44+R45)}·Vdd] (23)
wherein β31 and β32 are the mutual conductance values per unit gate voltage of the MOS-FETs 31 and 32, respectively, and V12 is the voltage of the constant voltage source 12.
The following equations (24) and (25) are obtained by substituting the equations (22) and (23) in the equations (20) and (21), respectively.
V64=Iin/{β31·(−V12)} (24)
G65=R46·[−β32·{R45/(R44+R45)}·Vdd] (25)
Furthermore, the output voltage V52 of the amplifier circuit 20d is obtained by multiplying the equation (24) by the equation (25) and represented by equation (26).
V52=(β32/β31)·{R45/(R44+R45)}·(Vdd/V12)·R46·Iin (26)
Since the power source voltage Vdd is included in the equation (26) so as to be multiplied, it is found that the output voltage 52 of the amplifier circuit 20d is proportional to the power source voltage Vdd according to this equation (26). The equation (26) is different from the equation (17) for calculating the gain on the basis of the configuration shown in
<<Fourth Embodiment>>
A fourth embodiment of the present invention relates to a power source voltage proportional amplifier with two inputs, which is configured by applying the circuit shown in
It is found that an amplifier circuit 20e shown in
V55=(β36/β35)·{R45/(R44+R45)}·(Vdd/V12)·R50·(Iin53−Iin54) (27)
In the equation (27), R50 is the resistance value of the resistor 50, and β35 and β36 are the mutual conductance values per unit gate voltage of the MOS-FETs 35 and 36, respectively. In the MOS-FETs 35 and 36, a relationship of β∝(W/L) is established, as explained according to the equation (18) in the descriptions of the above-mentioned third embodiment. It is thus found that the output voltage V55 is proportional to the channel widths W, provided that the channel lengths L are the same. Since the power source voltage Vdd is included in the numerator of the equation (27), the output power source voltage V55 is proportional to the power source voltage Vdd.
The frequency characteristics of the power source voltage proportional amplifiers in accordance with the above-mentioned first to fourth embodiments are determined depending on the fundamental frequency characteristics of the MOS-FETs and operational amplifiers being used. In the case when MOS-FETs and operational amplifiers available at present are used, the maximum amplifiable frequency is about 10 MHz, for example. In other words, it is possible to amplify an input signal having a frequency of about 10 MHz. In addition, the frequency range in which the gain is proportional to the variation of the power source voltage is about 1 MHz, for example.
<<Fifth Embodiment>>
A fifth embodiment of the present invention relates to an angular velocity sensor apparatus incorporating the power source voltage proportional amplifier in accordance with the above-mentioned fourth embodiment.
A terminal 133 connected to the level detection element 102 of the angular velocity sensor 10 is connected to the input terminal of a first amplifier 111. An input signal Vin owing to the charge generated on the surface of the level detection element 102 is input to the first amplifier 111. The output voltage Vm of the first amplifier 111 is input to a rectifier 122, a variable gain amplifier 125 and a phase detector 127. The output voltage Vm is rectified by the rectifier 122, smoothened by a smoothing circuit 123 comprising a resistor 143 and a capacitor 144 and input to the negative input terminal of the adder 125a of the variable gain amplifier 125. The positive comparison voltage Vr of a comparison voltage generation circuit 15 is applied to the positive input terminal of the adder 125b. The comparison voltage generation circuit 15 a constant voltage source, such as a band-gap constant voltage source, whose negative terminal is connected to a circuit ground Gr. The adder 125a applies the voltage difference between the output voltage of the smoothing circuit 123 and the comparison voltage Vr to an amplifier 125b that is capable of changing its gain by virtue of voltage control in the variable gain amplifier 125. The gain of the amplifier 125b is controlled by the voltage difference between the two voltages input to the adder 125a. An output signal obtained by this control is applied from the drive terminal 130 of the angular velocity sensor 10 to the drive element 101 and drives this element.
Since the output of the first amplifier 111 is amplified by the variable gain amplifier 125 and applied from the terminal 130 of the angular velocity sensor 10 to the drive element 101, the loop circuit circuit including the first amplifier 111, the rectifier 122, the smoothing circuit 123, the variable gain amplifier 125 and the angular velocity sensor 10 forms a sinusoidal oscillation circuit having an automatic gain control function. This loop circuit is hereafter referred to as an “AGC loop circuit.” The amplitude of the output voltage Vm of the first amplifier 111 is controlled so as to become constant by the AGC loop circuit. Since the voltage of the comparison voltage generation circuit 15 is fixed, the AGC loop circuit operates on a constant voltage regardless of the variation of the power source voltage Vdd. Hence, the amounts of the charges output from the detection-use piezoelectric elements 103 and 104 are not affected by the power source voltage Vdd either. The phase detector 127 and the DC amplifier 118 following the second amplifier 42 having an amplification degree proportional to the power source voltage Vdd do not depend on the power source voltage. However, the signal output to an angular velocity signal output terminal 119, that is, the output of the angular velocity sensor apparatus, depends on the power source voltage since the second amplifier serving as a power source voltage proportional amplifier depends on the power source voltage.
In
The output detected by the phase detector 127 is DC amplified by the DC amplifier 118 and output from the output terminal 119 as an output signal having a level proportional to the power source voltage Vdd and indicating an angular velocity.
The power source voltage response characteristics of the angular velocity sensor apparatus shown in
a shows a state wherein the power source voltage Vdd is increased unit step by A % while a constant angular velocity is detected.
Although the present invention has been described with respect to its preferred embodiments, the present invention is not limited to these embodiments. It will be understood that various modifications may be made without departing from the technical scope of the present invention. Further, the scope of the application of an amplifier with a gain proportional to source voltage according to the present invention is not limited to angular velocity sensors having the above-mentioned tuning fork structure, but includes velocity sensors having the other structures and other various electronic apparatus.
Number | Date | Country | Kind |
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2002-364865 | Dec 2002 | JP | national |
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Number | Date | Country | |
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20040124923 A1 | Jul 2004 | US |