Abstract:
An X-radiation protection circuit in a television receiver is responsive to both high voltage and high beam current conditions. A first detector is interconnected with an electron beam power source and monitors the beam current therefrom. The first detector produces a first voltage proportional in magnitude to the electron beam current. A second detector monitors a high voltage transformer that produces a potential for operating on the electron beam and the second detector produces a second voltage that is proportional in magnitude to the high voltage potential. A monitoring circuit constantly monitors both the first and second voltages and produces a trigger signal whenever the additive sum of the first and second voltages exceeds a selected magnitude. In this manner, a trigger signal indicates an excessively high combination of electron beam current and high voltage. This circuit is constantly responsive to both high voltage and electrom beam current, and substantially independent of power supply voltage changes. In addition, a hold down circuit operates independently of the first and second detectors to produce the trigger signal whenever the high voltage potential exceeds a predetermined magnitude.

Description:
RELATED APPLICATIONS 
     This is a continuation-in-part application of Ser. No. 101,878, filed Sept. 28, 1987 U.S. Pat. No. 4,841,406. 
    
    
     FIELD OF THE INVENTION 
     The present invention relates to X-radiation protection systems in a television receiver and in particular relates to a protection circuit that is constantly responsive to both high voltage and electron beam current in the television receiver. 
     BACKGROUND OF THE INVENTION 
     In many modern televisions, a high voltage accelerator potential is developed by a flyback transformer for accelerating an electron beam in a cathode-ray tube. This potential is generally referred to as the high voltage and will be on the order of 25 to 30 kilovolts for most color televisions. Screen brightness is proportional to the electron beam intensity (electron beam current) which is generally proportional to the high voltage. Thus, to increase screen brightness as might be desired, one must increase the high voltage and beam current. However, a television receiver is designed to operate at a particular high voltage and beam current, and exceeding such design criteria may cause the production of X-radiation. 
     While the electron beam current is generally proportional to the high voltage, the actual relationship between these two parameters varies depending upon operating conditions of the receiver. Also, while the production of X-radiation is generally associated with excessive high voltage, in fact, the production of X-radiation is affected by a combination of both high voltage and beam current. In general, as the beam current is lowered, a greater high voltage is allowable without producing harmful amounts of X-radiation. 
     To protect against the production of X-radiation, protective circuitry is commonly used to disable the television when favorable conditions exist for the production of X-radiation. Early designs of such protective circuitry simply monitored the high voltage and disabled the television set whenever a threshold was exceeded. In this configuration, the design of the protection circuit must assume a worst case electron beam current and thus, the threshold must be set lower than necessary for most beam currents. This design requirement often resulted in an unnecessary disablement of the television set when the magnitude of the high voltage went high, but the electron beam current remained sufficiently low to negate any danger of X-radiation production. 
     Various protection circuits have been designed to avoid so called nuisance shutoffs during periods where low electron beam current negates the potential of producing X-radiation. For example, Willis in U.S. Pat. No. 4,126,816 discloses a circuit that monitors only high voltage during normal operating conditions. However, at a predetermined low beam current, a second circuit imposes a new bias on the protective circuit which raises the magnitude of the high voltage required to trigger protection of the television set. In essence, Willis discloses a high voltage monitor or protection circuit that operates in two modes: a low beam current mode and a high beam current mode. However, this monitor is not fully responsive to beam current since the monitor is decoupled from the beam current circuit except during periods of low beam current. If a malfunction occurred which caused a very high beam current with the magnitude of the high voltage remaining normal, this circuit would not respond to the extremely high beam current and would not trigger protection. 
     Another example of a high voltage protection circuit is disclosed in U.S. Pat. No. 4,287,535 to Vakil in which high voltage is monitored and a latch circuit is triggered when the high voltage magnitude is considered excessive. Vakil monitors a high voltage horizontal sweep transformer and connected to the transformer are a rectifier circuit and a Zener diode circuit. So long as the high voltage is below a predetermined threshold, the Zener diode decouples the latch circuit from the sweep transformer and rectifier circuit. However, when the high voltage exceeds the first threshold, the Zener diode breaks down and the latch circuit is coupled to the rectified voltage from the transformer. However, the latch circuit is not necessarily actuated by the aforementioned coupling. Instead, the current flow from the transformer through the rectifier and latch circuit must exceed a second threshold before the latch circuit will be actuated. This second threshold is variable depending upon input from a feedback circuit that is also connected to the high voltage sweep transformer and the cathode-ray tube anode. According to the patent, the second threshold is proportional in magnitude to the beam current. Thus, according to the patent, once the first and second thresholds have been exceeded, in that order, the latch circuit is permanently triggered. Regardless of the magnitude of the high voltage or the electron beam current, the latch will remain triggered until the television is turned off. Again, Vakil is not fully monitoring beam current since the high voltage monitor is decoupled from the latch except during periods when the magnitude of the high voltage exceeds the first threshold. 
     As a further example of a protection circuit, U.S. Pat. No. 4,213,166 describes a system in which beam current and high voltage are monitored to determine a condition for enabling operation of a high voltage shutdown circuit. A high voltage transformer winding generates a voltage proportional to the high voltage applied to the cathode ray tube. A second voltage is generated proportional to the beam current and is combined with the winding generated voltage. When the combined voltage exceeds a reference potential, the shutdown circuitry is enabled. 
     The foregoing techniques must remain stable during operation of the television receiver. Changes in voltages not specifically related to the generation of the X-ray conditions must not influence the operation of the protection circuit. Thus, variations in low voltage power supply voltage which occur over time must not alter the operation of the protective circuit. 
     The above circuits are but a few examples of numerous protection circuits for television receivers designed to protect against X-radiation. Many others exist but they are generally more complicated and expensive than necessary. Also, due to their complexity, they have an excessive number of failure modes. Finally, many of the protective circuits have been outmoded or made obsolete by changes in television design. For example, many televisions use a horizontal sweep transformer which was the signal source in the Vakil patent. 
     SUMMARY OF THE INVENTION 
     In accordance with the present invention, a protection circuit is provided for a television that constantly monitors both beam current and high voltage. A threshold curve is established for the combination of these two parameters, and if the combination of a beam current and high voltage exceeds the threshold a trigger signal is produced. 
     This protection circuit is used in a television having a cathode ray tube producing an electron beam. In the television, a high voltage transformer provides a high voltage potential that operates on the electron beam, and an electron beam power source provides an electron beam current to the tube. The protection circuit includes a first detector that is interconnected with the electron beam power source which monitors the electron beam current from the source. This beam current is advantageously monitored in a preferred embodiment of the invention with a beam current detecting circuit which provides a voltage proportional to beam current and substantially independent of any low voltage circuit operating potential. A second detector monitors the high voltage transformer and produces a second voltage proportional in magnitude to the high voltage potential. A monitoring circuit constantly monitors both the first and second voltages and produces a trigger signal when the additive sum of said first and second voltages exceeds a selected magnitude. In this configuration, a reliable trigger signal indicates an excessively high combination of electron beam current and high voltage potential. 
     The preferred embodiment of the invention accomplishes the object of providing a voltage proportional to beam current which avoids the consequences of low voltage power supply variations. Thus, over the course of time, such power supply fluctuations do not adversely effect the trigger signal magnitude which is used to provide an indication of an X-ray condition. A transistor is used to amplify the change in voltage of a DAG connection independent of the television low voltage power supply voltage as an indication of beam current. This difference in potential generates a collector current through a load resistor. The corresponding voltage drop across the load resistor is an accurate beam current indication independent of changes in the low voltage power supply voltage. 
     In accordance with a second embodiment of the invention, a hold down circuit is provided for independently generating the trigger signal in response only to the high voltage potential whenever the potential exceeds a predetermined magnitude. In this manner, the trigger signal is also generated from the high voltage potential totally independently of the electron beam current, but at all times both beam current and high voltage are monitored by the first and second detectors. 
    
    
     BRIEF DESCRIPTION OF THE FIGURES 
     FIG. 1 illustrates an embodiment of the invention incorporating a hold down circuit for independently generating the trigger signal. 
     FIG. 2 illustrates a preferred embodiment of the invention. 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT 
     Referring now to FIG. 1, a protection circuit 10 includes circuitry for monitoring both the beam current and the high voltage of a television. The protection circuit 10 includes a power source 12 whose output is connected to resistors 14 and 16 that are connected in series through a junction 18 to another junction 20. At the junction 20, resistor 16 is connected to the cathode-ray tube DAG 21 which has a conductive coating on the outside of the tube. Junction 20 is also connected to the standard beam limiting circuitry 23 of the television set and is connected through a capacitor 22 to ground. 
     The beam current of the cathode ray tube passes entirely through the power source 12, the resistors 14 and 16 and through the junction 20. In conventional television sets, the beam limiting circuitry 23 uses a resistor to provide it with a timing constant. As shown in the drawing, the resistors 14 and 16 are performing the function of the single resistor needed by the beam limiting circuitry 23 to provide its timing constant. However, for purposes of the present circuit, the needed single resistor has been broken into a pair of series connected resistors, namely resistors 14 and 16. Since the beam current must pass entirely through resistor 14, there will be a voltage drop from the power source across the resistor 14 that is proportional to the beam current. As the beam current increases, the voltage drop across the resistor 14 increases and the voltage appearing at junction 18 will decrease with increasing beam current. 
     The voltage at junction 18 is applied through a resistor 24 to the base PNP transistor 26. The emitter of the transistor 26 is connected to ground through a resistor 28 and is connected through resistor 30 to a rectifier circuit 32 which consists of a diode 34 and a capacitor 36. The rectifier circuit 32 receives power from coil 38 that consists of about 1 to 3 turns on a flyback transformer 40. The flyback transformer 40 is the transformer that provides the accelerating high voltage potential for the electron beam of the cathode ray tube. The voltage produced by the coil 38 will be an alternating current in the form of spikes as are conventionally produced by flyback transformers in televisions. This alternating current is applied to the rectifier current 32 which will produce a DC voltage that is proportional in magnitude to the AC voltage produced by the coil 38. Thus, the magnitude of the voltage of rectifier 32 is proportional in magnitude to the high voltage alternating current produced by the flyback transformer 40. The DC voltage of the rectifier circuit 32 is applied through resistors 30 and 28 which function as a voltage divider and thus, the voltage appearing at the emitter of the transistor 26 will be proportional to the magnitude of the high voltage on the flyback transformer 40. 
     It is desired to apply a voltage to the emitter of transistor 26 that is proportional to the high voltage, and the function of resistors 30 and 28 is to appropriately scale the voltage applied to the emitter. In like manner, the design criteria in choosing the size of resistor 14 was to produce a voltage of appropriate scale at junction 18 that is proportional in magnitude to the beam current, and the design criteria for choosing resistor 16 is to provide a time constant to the beam limiting circuitry. That is, the series resistance of resistors 14 and 16 is chosen to provide an appropriate resistance for the beam limiting circuitry 23. 
     The collector of transistor 26 is connected through a diode 42 and a resistor 44 to ground. A capacitor 46 is also connected between the diode 42 and ground. A trigger responsive device 48 is connected to the resistor 44 so that the voltage appearing across resistor 44 provides an input to device 48. When a voltage does appear across the resistor 44, this is the trigger signal and the trigger responsive device 48 will respond to such trigger signal and protect the television in a conventional manner. For example, the trigger responsive device 48 may disable the power supply for the entire television set or just the horizontal oscillator. 
     A pair of Zener diodes 50 and 52 are connected in a reverse bias direction between the output of the rectifier circuit 32 and the diode 42. Thus, a series connection is formed by the output of the rectifier 32, the Zener diodes 50 and 52, the diode 42 and the resistor 44. 
     The function of diode 42 is for protection and capacitors 22 and 46 function as filters for high frequency components that may appear on the circuit. 
     OPERATION 
     In operation, the circuit 10 constantly monitors both the beam current and the high voltage and produces a trigger signal in response to a combination thereof. As previously mentioned, the voltage applied to the base of transistor 26 is proportional in magnitude to the magnitude of the beam current. Also, the voltage applied to the emitter of transistor 26 is proportional to the magnitude of the high voltage on the flyback transformer 40. As long as the television is operating within normal magnitudes of high voltage and beam current, the circuit is designed so that the voltage on the base of transistor 26 is significantly greater than the voltage on the emitter of transistor 26 to prevent the transistor 26 from turning on. Under these conditions, no current flows through transistor 26, and thus no voltage drop is produced across resistor 44. Therefore, the input to the trigger responsive device 48 is zero volts or ground (common). The relative magnitudes of the voltages appearing on the base and emitter of transistor 26 are controlled by resistors 14, 28 and 30 so that the transistor 26 will not turn on during normal operations of the television with beam current and high voltage falling within safe ranges. 
     However, if the beam current begins to rise, the voltage drop across resistor 14 will increase, and the voltage applied to the base of resistor 26 will decrease. If the high voltage magnitude remains constant and the beam current continues to increase, eventually the voltage appearing at the base of transistor 26 will drop below Veb of the transistor (approximately 0.6 volts) and the transistor turns on. When the transistor 26 turns on, current will flow from the recitifier circuit 32, through resistor 30, through transistor 26, through diode 42 and through resistor 44 to ground. This current flow will cause a voltage drop across the resistor 44 creating a trigger signal for the device 48 and a shutoff will occur. 
     In like manner, the circuit is responsive to increases in magnitude of the high voltage. If the magnitude of the high voltage on the flyback transformer 40 began to increase, the output of the rectifier circuit 32 would increase, and after the voltage division produced by resistors 30 and 28, the voltage appearing at the emitter of the transistor 26 would likewise increase. If the beam current remains constant and the magnitude of the high voltage continues to rise, the voltage appearing at the emitter of transistor 26 will eventually rise until it approaches the voltage appearing at the base of transistor 26. When the emitter voltage increases approximately 0.6 of a volt greater than the base voltage, the transistor will again turn on and a current will flow through resistor 44, providing a trigger signal to the device 48. 
     The transistor 26 operates in this mode as a comparator. AS the high voltage sample appearing on the emitter of transistor 26 increases to a level equal to the potential on the transistor 26 base constituting a reference level, the transistor 26 switches generating a trigger signal. The threshold voltage representing the level of beam current for the cathode ray tube varies, changing the switching voltage level for transistor 26. 
     From the discussion above, it will be appreciated that the protection circuit 10 will turn on and create a trigger signal in response to an infinite number of combinations of beam current and high voltage magnitude. When the sum of the voltages appearing at the base and emitter of transistor 26 exceed a predetermined threshold, the transistor will turn on and a trigger signal will be produced. 
     The Zener diodes 45 and 47 provide a hold down function at zero or low beam current and these diodes, in combination with the components with which they function. Basically, the Zener diodes 45 and 47 provide for a shutoff whenever the magnitude of the high voltage exceeds a predetermined amount regardless of the beam current magnitude. As the high voltage magnitude begins to rise, the magnitude at the output of the rectifier circuit 32 will also rise. Eventually, the magnitude of the voltage produced by the rectifier circuit 32 will exceed the breakdown voltages of the Zener diodes 45 and 47, and a current will flow from the rectifier 32, through the Zener diodes 45 and 47, through diode 42 and through resistor 44 to ground. When the Zener diodes 45 and 47 break down, a voltage is produced across resistor 44 and a trigger signal is provided to the device 48. The purpose of the hold down circuit 45 and 47 is to provide a high voltage magnitude that may never be exceeded at zero or very low beam current. It should be noted that the Zener diodes 50 and 52 are inserted into the circuit without any resistors between the diodes and the coils 38. Thus, the voltages sensed by the Zener diodes 45 and 47 are not subject to errors that might be created by a voltage division circuit, and since so few components are disposed between the diodes 45 and 47 and the coil 38, the number of failure modes is minimized. 
     In the embodiment of FIG. 1, the resistors 14, 28 and 30 are chosen so that the hold down circuit is basically a redundant circuit that would provide an alternate shutdown in the event that the transistor 26 or the components operating in association with transistor 26 failed. However, it should be appreciated that the circuit 20 could be designed so that the hold down circuit provided by Zener diodes 45 and 47 would dominate under certain operating conditions. For example, the circuit 10 could be designed so that the protection function is provided by the transistor 26 whenever beam currents and high voltage magnitudes are within normal operating ranges. But, if the beam current drops to an abnormally low magnitude, the circuit 10 could be designed so that the Zener diodes 45 and 47 would break down before transistor 26 turned on. 
     In an alternate embodiment, a Zener diode 56 could be placed across transistor 26 as shown in dashed lines in the drawing. The Zener diode 43 is not normally present, but if it were, it would protect against the possibility of a failure of transistor 26. The Zener diode 43 would function similarly to diodes 45 and 47, except that the voltage applied to it would be controlled by the voltage division circuit formed by the resistors 30 and 28. This voltage would be proportional to the high voltage on the flyback transformer 40, but it is not the preferred embodiment since diode 43 would be subject to the effects of the tolerances in the magnitudes of resistors 28 and 30. In most circuits of this type, the resistors will have a tolerance of plus or minus five percent. 
     The circuit of FIG. 2 represents a further preferred embodiment of the concept for monitoring both CRT current and television receiver high voltage, and using the result as an indication of an X-radiation generating condition. The circuit of FIG. 2 is advantageous in that variations in the low voltage power supply 54 of the television receiver do not influence the reliable detection of an X-radiation condition. The circuit comprises a transistor 50 which includes in the base circuit a voltage divider comprising resistors 63 and 64. The transistor 50 includes an emitter resistor 62. Changes in the DAG potential are expressed as a change in current through resistors 63 and 64. As will be obvious to those skilled in the art, the transistor 50 will conduct when the voltage output from voltage divider 63 and 64 is less than the potential V s  applied by the low voltage power supply 54 to the emitter resistor 62. 
     It can be seen that changes in the power supply voltage 54 will effect the voltage at the emitter of transistor 50, as well as that produced by the voltage divider 63 and 64. 
     The current in the emitter collector circuit of transistor 50 is proportional to the voltage supplied to the base by voltage divider 63, 64 and the emitter resistor 62. As the beam current increases, the voltage drop across resistor 63 increases, thus increasing the collector emitter current. 
     The potential developed across collector resistor 61 is therefore proportional to the beam current through resistors 63 and 64. This potential is summed with the potential generated from the tertiary winding 60 on the high voltage transformer. The high voltage transformer tertiary winding 60 and collector resistor 61 form a composite voltage. This composite voltage, when it exceeds the Zener breakdown of Zener diode 58, will be indicative of an X-radiation condition. Diode 59 is familiar to those skilled in the art as being merely a rectifier for rectifying the pulses appearing on transformer tertiary winding 60 into a DC voltage. 
     Capacitor 68 reduces the effect of ripple from rectifying the pulse to transformer current. Additionally, a load resistor 57 is connected across the Zener diode, providing a limit to the voltage magnitude produced on terminal 55. 
     A capacitor 66 is shown between the DAG winding and negative supply of the low voltage power supply. 
     The circuit represented in FIG. 2 generates a trip voltage VX proportional to ##EQU1## This equation includes the sum of two terms comprising the term I× (R 57  +R 61 ), representing the high voltage term, and the remaining term ##EQU2## representing the beam current element. When these two terms combine to exceed the Zener potential, V 58 , a trigger signal is developed. 
     As can be seen by the foregoing equation, the trigger voltage is independent of the power supply voltage V s . Thus, as the power supply voltage within the television receiver, changes the X-ray condition is still reliably detected. 
     It therefore can be seen that the foregoing principles of detecting beam current as well as excessive high voltage as an indication of X-radiation generating conditions can be applied by a circuit which is substantially insensitive to changes in power supply voltage. 
     Although preferred embodiments have been described in the foregoing detailed description, it will be understood that the invention is capable of numerous rearrangements, modifications and substitutions of parts without departing from the scope of the invention as defined by the appended claims.