Background of the Invention
This invention relates to a stepped pulse generator which provides a stepped pulse output in response to the input of a signal of sawtooth form.
In integrated circuit technology it is advantageous to work with step-shaped pulses in order to transmit multiple informations by means of a combined pulse and in order to save connecting points.
Summary of the Invention
The invention seeks to provide a circuit arrangement which is suitable for manufacture in integrated semiconductor technology and which supplies step-shaped pulses.
According to the invention there is provided a stepped pulse generator circuit comprising an input line for a sawtooth waveform, an output line for a stepped pulse waveform, first and second differential amplifiers each comprising first and second transistors, the first transistor of each said differential amplifier having its base electrode coupled to said input line, a common load resistor for the differential amplifiers coupled to the collector electrode of the first transistor of the first differential amplifier, to the collector electrode of the second transistor of the second differential amplifier and said output line, biassing means coupled with the base electrode of the second transistor of the first differential amplifier and the base electrode of the second transistor of the second transistor of the second differential amplifier adapted to provide different bias potentials thereto and current supply means coupled with the emitter electrodes of the transistors of the first and second differential amplifiers.
Further according to the invention, there is provided a circuit arrangement for producing a stepped pulse, characterized in that at least two differential amplifiers are provided each of which has a first and a second transistor; that the bases of the first transistors are connected together and a saw-tooth voltage is supplied to them; that the base potentials of the second transistors are different and are chosen such that they lie between the end potentials of the sawtooth voltage; that the collector of the first transistor of a differential amplifier and the collector of the second transistor of the other differential amplifier have a common collector resistor and that both differential amplifiers obtain the same current.
Brief Description of the Drawings
In order that the invention and its various other preferred features may be understood more easily an embodiment thereof will now be described, by way of example, with reference to the drawings, in which:
FIG. 1 shows a circuit arrangement for a colour television receiver, a negative line flyback pulse being supplied at the input 1 to the circuit arrangement and this circuit arrangement supplies a step-shaped pulse at the output 3, the pulse being synchronous with the line flyback pulse,
FIG. 2a shows a line flyback pulse occurring at the input 1 of FIG. 1,
FIG. 2b shows a sawtooth waveform which occurs at point 2 in the circuit of FIG. 1,
FIG. 2c indicates the voltage waveform occuring at the base electrode of transistor T.sub.10 shown in FIG. 1,
FIG. 2d shows a voltage waveform component occurring across th resistor R.sub.6 due to current flowing through transistor T.sub.12.
FIG. 2e shows a voltage waveform component occuring across the resistor R.sub.6 due to current flowing through the transistor T.sub.13, and
FIG. 2f shows the actual stepped voltage waveform occuring across resistor R.sub.6 which waveform is formed by the combined currents flowing through transistors T.sub.12 and T.sub.13 in FIG. 1.
Description of a Preferred Embodiment
In a preferred embodiment of the invention a circuit arrangement as stated at the outset is proposed in which at least two differential amplifiers are provided each of which has a first transistor and a second transistor; in that bases of the first transistors are connected together and a saw-tooth voltage is supplied to them; that the base potentials of the second transistors are different and such that they lie between the end potentials of the saw-tooth voltage; that the collector of the first transistor of one differential amplifier and the collector of the second transistor of the other differential amplifier have a common collector resistor; and that both differential amplifiers obtain the same current.
Preferably transistors of a current mirror circuit are provided as current sources for the differential amplifiers, these supplying the same current. The saw-tooth voltage is preferably produced by a RC network. As the saw-tooth voltage is only required temporarily a switch is provided which short-circuits the capacitor for the remaining time.
Referring now to the circuit of FIG. 1, this has two differential amplifiers; one differential amplifier comprises the transistors T.sub.15 and T.sub.16 and the other differential amplifier comprises the transistors T.sub.17 and T.sub.18. As is shown in FIG. 1 the bases of the two first transistors T.sub.16 and T.sub.17 of the differential amplifiers obtain the same potential by means of the saw-tooth voltage. The current source for the lefthand differential amplifier is the transistor T.sub.12 and the current source for the right-hand differential amplifier is the transistor T.sub.13. As the transistors T.sub.12 and T.sub.13 are equal and belong to a current mirror circuit together with the transistor T.sub.10 connected as a diode, the transistors T.sub.12 and T.sub.13 supply the same current.
The supply of current is effected into the directly connected emitters of the first and second transistor of each differential amplifier. The bases of the second transistors T.sub.15 and T.sub.18 receive different bias voltages which are supplied by a voltage divider. This voltage divider comprises the resistors R.sub.9, R.sub.11 and R.sub.12. The bias for the base of the transistor T.sub.15 is the tapped voltage between the resistors R.sub.9 and R.sub.11 reduced by the base-emitter voltage of the emitter follower transistor T.sub.19. The bias for the base of the transistor T.sub.18 is obtained from the tapped voltage between the resistors R.sub.11 and R.sub.12 deducting the base-emitter voltage of the emitter follower transistor T.sub.20.
The collector of the first transistor T.sub.16 of the left-hand differential amplifier and the collector of the second transistor T.sub.18 of the right-hand differential amplifier have the common collector-resistor R.sub.6 while the collectors of the transistors T.sub.15 and T.sub.17 are connected to the reference potential.
The transistors T.sub.12 and T.sub.13 are conductive only as long as the negatively directed line flyback pulse is present at input 1. In the remaining time during the line scan the transistors T.sub.12 and T.sub.13 are blocked. Similarly the saw-tooth voltage (FIG. 2b) which occurs at point 2 and is supplied to the bases of T.sub.16 and T.sub.17 via the emitter follower comprising the transistor T.sub.14 and the resistor R.sub.5, is only present during the duration of the line flyback pulse (FIG. 2a).
According to FIG. 2b the saw-tooth voltage runs synchronously in terms of time with the input pulse and in fact it runs from the point A, which corresponds to the supply voltage reduced by the saturation voltage of transistor T.sub.4, up to point B, which corresponds to the end of the input pulse. The sawtooth voltage runs from fairly high to fairly low voltage values in the embodiment.
If the transistor T.sub.12 is conductive then the current flows away from t.sub.12 either via the transistor T.sub.15 or via the transistor T.sub.16, according to which of the two transistors is conductive at the time. At the beginning of the saw-tooth voltage the transistor T.sub.15 is conductive. This stage changes if the saw-tooth voltage applied to the base of T.sub.16 falls below the base bias of the transistor T.sub.15 (point C in FIG. 2b) so that the transistor T.sub.15 is changed from the conductive to the blocking state and T.sub.16 is now conductive. As a voltage drop coming from the current of the transistor T.sub.12 only occurs at the resistor R.sub.6 when the transistor T.sub.16 is conductive then the pulse according to FIG. 2d is produced at the resistor R.sub.6 because of the current of T.sub.12.
However, besides the voltage which results from the current of the transistor T.sub.12 yet another voltage drop occurs across resistor R.sub.6 in accordance with FIG. 2e, which results from the current of the transistor T.sub.13. As FIG. 2e shows this voltage drop occurs immediately with the input pulse, wherein the current resulting from the transistor T.sub.13 flows through the conductive transistor T.sub.18. Only if the saw-tooth voltage has reached the point D in FIG. 2b does the transistor T.sub.17 become conductive instead of transistor T.sub.18 so that the voltage drop at R.sub.6, which results from the current of the transistor T.sub.13 stops.
The addition of the voltage curves of FIGS. 2d and 2e gives the desired step-shaped pulse of FIG. 2f. The stepped pulse reaches output 3, where it is available with low source resistance, via the emitter follower comprising the transistor T.sub.21 and the resistors R.sub.10 and R.sub.13.
The saw-tooth voltage occurs at the RC network which is connected to the point 2 externally, and is formed from a resistor R.sub.14 and a capacitor C. As the saw-tooth voltage should be available synchronously in terms of time with the input pulse, an electronic switch is provided which short-circuits the capacitor C during lines scanning. This switch is formed by a transistor T.sub.4. If T.sub.4 is conductive then a current flow from T.sub.4 to the point 2 and to earth via the resistor R.sub.14. R.sub.14 is so dimensioned that the voltage drop at R.sub.14 is sufficient to drive the transistor T.sub.4 into saturation. During the scanning of the line there is a voltage at point 2 which is equal to the difference between the supply voltage and the saturated voltage of the transistor T.sub.4.
As the transistor T.sub.4 becomes conductive or blockes so becomes the transistor T.sub.5 also conductive or blocked in time therewith, since the transistors T.sub.4 and T.sub.5 together with the transistor T.sub.3, which is connected as a diode, form a current mirror circuit. The current through the switching transistor T.sub.5 flows away to earth via the resistor R.sub.4. The resistor R.sub.4 is so dimensioned that the transistor T.sub.5 is driven into saturation by the voltage drop at R.sub.4. This is the case during the scanning of the line. In this condition no current flow through the transistor T.sub.10, which is connected as a diode, during scanning of the line. During the line flyback pulse the transistors T.sub.5 is blocked and the current through R.sub.4 flows via the transistor T.sub.10 which is connected as a diode. The course shown in FIG. 2c then takes place at the basecollector connection of T.sub.10, wherein the voltage during the pulse is the difference between the supply voltage and the base-emitter voltage from T.sub.10 . As the transistor T.sub.10 belongs to a current mirror circuit together with the transistors T.sub.12 and T.sub.13 then T.sub.12 and T.sub.13 supply current only during the line flyback pulse.
The negatively directed line flyback pulse which is applied at input 1 reaches the base of transistor T.sub.6 via the transistor T.sub.1 which is connected as a diode. The transistors T.sub.6 and T.sub.7 form a differential amplifier. The bias of the transistor T.sub.7 is equal to the tapped voltage between resistor R.sub.2 and R.sub.3 of a voltage divider formed from the resistors r.sub.2 and r.sub.3 and from a transistor T.sub.9 which is conncted as a diode. The transistor T.sub.8 and the transistor T.sub.9 form a current mirror circuit so that the same currents flow through T.sub.8 and through T.sub.9.
During the scanning of the line the potential at the base of the transistor T.sub.6 must be above the base bias of the transistor T.sub.7 so that the current supplied by the current source transistor T.sub.8 flows via T.sub.6 and the transistor T.sub.3 which is connected as a diode. As T.sub.3, T.sub.4 and T.sub.5 belong to a current mirror circuit current also flows through T.sub.4 and T.sub.5 at the same time as the current through T.sub.3, wherein T.sub.4 and T.sub.5 are driven to saturation, as already mentioned.
In order that during the scanning of the line the base potential of the transistor T.sub.6 is above the base potential of the transistor T.sub.7 the potential at input 1 must be greater than the base bias of transistor T.sub.7 plus the voltage of the base-collector diode of the transistor T.sub.1 which is connected as a diode. The transistors T.sub.1 and T.sub.2, which are connected as diodes, together with the resistor R.sub.1 form a series circuit wherein the tapping between the collector of T.sub.1 and the resistor R.sub.1 is connected to the base of the transistor T.sub.6.
As a result of the negatively directed line flyback pulse the base potential of the transistor T.sub.6 is brought below the base bias of the transistor T.sub.7 so that T.sub.6 is now blocked and thus T.sub.7 is conductive. At the same time the current stops flowing through the transistor T.sub.3, which is connected as a diode, and this has the result that also the transistors T.sub.4 and T.sub.5 belonging to the current mirror circuit are switched from the conductive into the blocked state.
Instead of the normally used base-emitter diode the base-collector diode of the input transistor T.sub.1 is used in order to obtain a high blocking voltage and in order to be able to supply the line flyback pulse with an amplitude the value of which is higher than the supply voltage by a multiple.
It will be understood that the above description of the present invention is susceptible to various modification changes and adaptations.