Abstract:
A telecommunication system has a telecommunication line for communicating a combined signal and a splitter that is coupled to the telecommunication line. The splitter has a high-pass filter, a low-pass filter, and a current limiter. The high-pass filter is configured to transmit a first component signal of the combined signal, and the low-pass filter is configured to transmit a second component signal of the combined signal. The current limiter is configured to limit a current of the second component signal thereby preventing at least one inductor in the low-pass filter from saturating.

Description:
FIELD OF THE DISCLOSURE 
     This disclosure generally relates to splitters used to combine and separate signals in a frequency-division communication system, such as a digital subscriber line operating in a frequency band above a conventional telephone signal. 
     RELATED ART 
     For frequency division communications systems, various signal splitters are available for combining and separating a broadband signal, such as an asymmetric digital subscriber line-2+(ADSL2+) signal or other digital subscriber line (DSL) signal, and a plain old telephone service (POTS) signal wherein the signals have been combined for transmission over a twisted wire pair of a telephone cable. Such splitters generally comprise a low-pass filter for passing the low frequency components of the POTS signal to telephone equipment and a high-pass filter for passing the high frequencies of the broadband signal to a data transceiver. 
     In general, a conventional splitter isolates the voice and data services so that they do not interfere with one another. However, during certain events associated with normal POTS service such as ring trip, the conventional splitter may fail to provide sufficient isolation, leading to errors in the broadband data. In some applications, a higher-level communications protocol can cope with the errors by various means, such as requesting a retransmission. Other time sensitive applications are less tolerant of errors. For example, errors in a streaming video signal delivered over a DSL circuit may be observed on a video display device before retransmission can occur. In such applications, there is a need for a robust splitter that provides sufficient isolation between the POTS and DSL service under all normal loop conditions. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWING 
       The disclosure can be better understood with reference to the following drawings. The elements of the drawings are not necessarily to scale relative to each other, emphasis instead being placed upon clearly illustrating the principles of the disclosure. Furthermore, like reference numerals designate corresponding parts throughout the figures. 
         FIG. 1  is a block diagram illustrating a conventional frequency-division communication system using conventional splitters for separating telecommunication signals. 
         FIG. 2  is a diagram illustrating a typical instantiation of the xDSL-over-POTS system depicted in  FIG. 1 . 
         FIG. 3  is a block diagram illustrating a frequency-division communication system having a current-limited splitter in accordance with an exemplary embodiment of the present disclosure. 
         FIG. 4  is a block diagram illustrating a frequency-division communication system having a current-limited splitter in accordance with an exemplary embodiment of the present disclosure. 
         FIG. 5  is a circuit diagram illustrating an embodiment of a current limiter depicted in  FIG. 3  or  FIG. 4  using depletion-mode metal-oxide field effect transistors (MOSFET). 
         FIG. 6  is a block diagram illustrating an exemplary current limiter, such as is depicted in  FIG. 3  or  FIG. 4 . 
         FIG. 7  is a circuit diagram illustrating an exemplary embodiment of a current limiter, such as is depicted in  FIG. 3  or  FIG. 4 , using enhancement-mode MOSFETs. 
         FIG. 8  is a circuit diagram illustrating an exemplary embodiment of a current limiter, such as is depicted in  FIG. 3 , using depletion-mode MOSFETs. 
         FIG. 9  is a circuit diagram illustrating an exemplary embodiment of a current limiter, such as is depicted in  FIG. 3 , using depletion-mode MOSFETs. 
         FIG. 10  is a circuit diagram illustrating an exemplary embodiment of a current limiter, such as is depicted in  FIG. 3 , using enhancement-mode MOSFETs. 
     
    
    
     DETAILED DESCRIPTION 
     In general, embodiments of the present disclosure pertain to signal splitting systems and methods having improved robustness against large-signal transients in a frequency-division communication system, such as when broadband data is transported on the same pair of wires as a POTS signal. Without sufficient large-signal immunity, the isolation typically provided by a conventional splitter could degrade to the point that the services interfere with one another. Audible noise may become present on the telephone, and broadband data may be lost. This disclosure focuses on the impact to the broadband service, though the POTS service will receive some benefits as well. While some broadband applications such as web surfing can easily recover from lost data, other applications, such as streaming video, operate in real time or near real time and are much less tolerant of data loss. 
       FIG. 1  shows a block diagram of an exemplary frequency division communication system  50  wherein a broadband signal, such as an ADSL2+ signal or other type of DSL signal, and a conventional phone signal (a voiceband signal or VB signal) are transported together over a common medium  23 , such as a twisted wire pair. A broadband transceiver (TX/RX)  6 , which comprises a data transmitter and data receiver, at a Central Office (CO) communicates with a broadband transceiver  12 , which comprises a data transmitter and data receiver, at a customer premise in a high frequency band. The transceivers  6 ,  12  are configured to communicate DSL signals (e.g., ADSL2+). In other examples, the transceivers  6 ,  12  can be configured to communicate other types of data signals (e.g. VDSL2). 
     Many DSL signals start around 25 kHz and extend into the MHz realm. Equipment  19  at the CO comprises POTS switch  8  communicates with a telephone  10  in a low frequency band. POTS communication typically occurs in the 200 Hz to 4000 Hz band, often referred to as the voice band (VB), but supervisory signaling may produce spurious noise at higher frequencies. At the CO, a signal splitter  18  serves to isolate the POTS and DSL services from one another by feeding the appropriate frequency band to the termination equipment  6 ,  8  via a low-pass filter (LPF)  2  and a high-pass filter (HPF)  1  as shown. Similarly, customer premise equipment (CPE)  21  comprises a DSL transceiver  12  and a telephone  10  connected to the line  23  via a CPE splitter  22 , which comprises a LPF  30  and a HPF  24 , similar to the CO splitter  18 . 
       FIG. 2  shows more detail of how a conventional DSL over POTS communication system is typically implemented in practice. During an initial learning phase known as “training,” the CO transceiver  6  and the CPE transceiver  12  probe the communication channel over line  23  to learn its transfer function, which is affected by things like the impedance Zco of the CO LPF  2 , the characteristics of cable  20 , and the impedance Zcpe of the CPE LPF  30 , as well as the HPF  1 ,  24  associated with each modem transceiver  6 ,  12 . While many DSL implementations can adapt to slow changes in the transfer function, it is assumed for simplicity that there will be no rapid deviations in the communication channel. 
     For historical reasons, POTS service employs large signals and various impedance conditions to indicate supervisory states to the far end. Neither of these mechanisms is friendly to broadband and can pose serious problems as broadband applications, such as DSL, continue to evolve. While the actual POTS voice signal is intended to be band limited from roughly 200 Hz to 4 kHz, supervisory state changes can create transient signals containing spectral content in the band employed by the broadband service. Of particular concern is the condition in which a person answers a ringing telephone  10 . The circuit  8  applying the ringing requires an interval to detect the off-hook condition of the phone  10 , during which time large ringing voltages are applied to a low-impedance off-hook telephone  10 . Beyond just the spectral noise created by the transients associated with change from high impedance to low impedance of the phone, the resulting currents can be much larger than during other operating states. 
     In fact, the currents can be so large as to impair the operation of the LPFs  2 ,  30 . Conventional splitters are passive in nature, consisting of resistors, inductors, capacitors, and perhaps protection devices. The inductors are the elements that primarily set the impedance of the LPF (Zco or Zcpe) in the DSL band. When current flows through an inductor, it creates a magnetic field proportional to the current. However, as known to those in the art, real inductors have limitations on the magnetic field intensity (also known as flux density) that they can support, beyond which the device saturates and ceases to behave inductively. If enough current flows through the inductors to cause them to saturate, isolation between the POTS and DSL service will likely be degraded and the impedance of the LPF (Zco and/or Zcpe) will likely change, disturbing the transfer function of the DSL system and ultimately causing bit errors. 
     While particular construction details affect the maximum flux density that an inductor can handle without saturating, physical size is the primary limiting factor. It is possible to build inductors that can withstand ring trip currents without saturating, but they are generally large and do not generally minimize the energy associated with supervisory state changes. By combining a current limiter (CL)  200  with a conventional LPF  30 , a current-limited LPF (CL-LPF)  100  can be realized as indicated in  FIG. 3 . With a CL-LPF  100 , transient energy from POTS supervisory signals is reduced and inductors in both the CO LPF  2  and the CPE LPF  30  are simultaneously protected from saturation. Moreover, by reducing impedance fluctuations in the LPFs that would otherwise occur due to high current transients, the current limiter  200  reduces disturbances to the transfer function between the transceivers  6 ,  12  as compared to a system that does not employ a current limiter  200  as described. Further, a single CL  200 , whether used at the CO or CPE, allows the use of relatively small inductors in both the CO LPF  2  and the CPE LPF  30 , which is in itself a significant advantage to telecommunications providers and equipment manufacturers as space is at a premium. Note that a CL-LPF could alternatively be created at the CO by placing a CL  200  between the CO LPF  2  and the POTS switch  8 , as shown by  FIG. 4 , though longitudinal balance would be more critical in this configuration. 
       FIG. 5  illustrates a conceptual embodiment of a current-limited LPF (CL-LPF)  100  in accordance with the present disclosure. The LPF  30 , shown in a representative ladder arrangement of inductors (L) and capacitors (C), is coupled in series with the current limiter  200 . The phone  10  is represented by load impedance, Z L . The current limiter  200  has characteristics illustrated by the voltage-current curve  202  in  FIG. 5 . An examination of curve  202  shows that for small values of current, the limiter  200  has a fixed value of resistance shown by the slope  203  of curve  202 . When the current reaches a threshold value, I max  (positive or negative), then the current is clamped to that value. A maximum current value of around 110 mA (milliamperes) will allow normal delivery of POTS while allowing relatively small inductors to be used with the LPFs  2 ,  30  of both the CO and CPE. Although 110 mA is a preferred value for one embodiment of the present disclosure, other values may be used for I max . 
     Known or future-developed current limiters may be used to implement the current limiter  200 , though conventional current limiters may interfere with POTS service in some way. An exemplary embodiment of a current limiter (CL)  200  is disclosed herein, with a block diagram of such a limiter  200  shown in  FIG. 6 . Conceptually, the limiter  200  comprises several elements, the first of which is a limiting element  601 , also known as a pass device, which acts to restrict the flow of current. The limiting element  601  is modulated by a feedback control element  603  such that it presents the impedance necessary to achieve the desired limiting function. The current sensing element  602  monitors the current actually flowing through the current limiter  200  at any given time as the input to the feedback control element  603 . 
     Exemplary embodiments of the current limiter  200  are shown in  FIG. 7  through  FIG. 10 . The embodiments of the current limiter  200  described herein utilize metal-oxide field effect transistors (MOSFETs or FETs) as the limiting element, a resistor as the current sensing element, and a Bipolar Junction Transistor (BJT) for feedback control, although other types of components may be used in other embodiments. 
       FIG. 7  shows a CL  200  based on enhancement mode FETs M 1  and M 2  as the limiting elements  601 . A voltage source Vx supplies gate-to-source voltage (Vgs) for the FETs M 1  and M 2 , placing them in a normally conductive, low-impedance state. Resistors RL 1  and RL 2  form the current sensing element  602 , while BJTs Q 1  and Q 2  close the feedback control loop  603 . Consider the case where node Ain is at a positive potential with respect to node Bin such that conventional current flows from Ain to Bin. When the current through the sensing element  602  develops enough voltage to turn on the base-emitter junction (Vbe(on)) of Q 1 , Q 1  begins to conduct, stealing gate drive from the FET M 1 . This increases the impedance of FET M 1 , decreasing the current that flows. Q 1  continues to steal M 1 &#39;s gate drive until the voltage developed across the current sensing element  602  reaches exactly Vbe(on) of Q 1 , completing the feedback control  603  to M 1 , the limiting element  601 . For this polarity of current flow, Q 2  remains off, leaving M 2  in its low-impedance state. M 1  and Q 1  are the active limiting element  601  and feedback control element  603 , respectively, for this polarity. When the voltage across the sensing element  602  drops below Vbe(on) of Q 1 , Q 1  quits conducting, restoring gate drive to the FET M 1  and placing it back in a low-impedance state. Due to the symmetry of the circuitry, for the opposite polarity of input such that current flows from Bin to Ain, the principles of the circuit&#39;s operation are exactly the same with M 2  serving as the limiting element  601  and Q 2  serving as the feedback control element  603 . 
     In the normally conductive state, this embodiment of a CL  200  has a total insertion resistance of (RL 1 +RL 2 +RMOS 1 +RMOS 2 ) where RMOS 1  and RMOS 2  are the drain-to-source on resistance of FETs M 1  and M 2  respectively. The maximum current (Imax) allowed by the device (Imax) is Vbe(on)/(RL 1 +RL 2 ). For a current limit of 110 mA, a reasonable value, RL 1 +RL 2  would be about 4.53 ohms as Vbe(on) will be approximately 0.5 Volts for small collector currents. Typical FET devices such as International Rectifier&#39;s IRF 730  put RMOS 1  and RMOS 2  at roughly 1 ohm each. This makes for a total insertion resistance of less than 7 ohms. 
     Low insertion resistance is highly desirable, as additional resistance decreases the supervisory range of the POTS service and adds additional attenuation to the voiceband (VB) signals. The architecture of  FIG. 7  has no deadband in the pass function that would otherwise add crossover distortion to the VB signal. As known in the art, crossover distortion generally refers to distortion caused by line voltages close to zero when the line voltage is transitioning from a positive voltage to a negative voltage or vice versa. Such distortion is typically cause by transistors turning off when the line voltage falls below the critical biasing value (Vbe(on) for BJT, Vgs for FET). 
     The symmetry of the instant embodiment ensures that it will perform equally well for either polarity of input signal. The action of the feedback control element  603  makes the current limit independent of various characteristics of the limiting element  601 , such as the gate-to-source threshold voltage of the FETs used to implement the element  601 . 
       FIG. 8  shows an alternative embodiment based on depletion-mode MOSFETs M 1  and M 2  as the limiting element  601 . This embodiment removes the need for voltage source Vx of  FIG. 7 , as depletion-mode FETs are in their low-impedance conductive state when there is no gate-to-source voltage. Rload represents the load, such as a telephone  10 , and is not part of the current limiter  200 . Considering the scenario where current is flowing from Ain to Bin, M 1  serves as the limiting element  601 , a resistor RL 1  serves as the current sensing element  602 , and a BJT Q 1  serves as the feedback control element  603 . For small currents, BJTs Q 1  and Q 2  are both off and resistors R 1  and R 2  ensure that there is no voltage drop between the gate and source of either M 1  or M 2 . Thus, M 1  and M 2 , being depletion-mode devices, are in their low-impedance conductive state. When sufficient current flows through RL 1  to develop enough voltage to turn on the base-emitter junction (Vbe(on)) of Q 1 , Q 1  conducts, pulling the gate of M 1  negative with respect to its source. This increases the impedance of the FET M 1 , decreasing the current that flows until the feedback loop reaches a steady state condition. For this embodiment, it is desirable for Imax*(Rload+RMOS 2 +RL 1 )&gt;=Vgs(M 1 ), where Vgs(M 1 ) is the threshold voltage of M 1  and RMOS 2  is the drain-to-source resistance of M 2  in its fully conductive state (Vgs=0). This condition ensures that there is sufficient gate drive available for M 1  to reach a high enough impedance to limit the current for any input voltage. For this polarity of current flow, BJT Q 2  remains off, leaving M 2  in its low-impedance state. M 1  and Q 1  are the active limiting element  601  and feedback control element  603  for this polarity. When the voltage across the RL 1  sensing element  602  drops below Vbe(on) of Q 1 , Q 1  quits conducting, placing M 1  back in a low-impedance state. Due to the symmetry of the circuitry, for the opposite polarity of input such that current flows from Bin to Ain, the principles of the circuit&#39;s operation are exactly the same with M 2  serving as the limiting element  601 , resistor RL 2  serving as the current sensing element,  602  and BJT Q 2  serving as the feedback control element  603 . 
     In the normally conductive state, this embodiment of a CL  200  has a total insertion resistance of (RL 1 +RL 2 +RMOS 1 +RMOS 2 ) where RMOS 1  and RMOS 2  are the drain-to-source on resistance of FETs M 1  and M 2  respectively. The maximum current (Imax) allowed by the device is Vbe(on)/(RLx), where x is 1 or 2 depending on the polarity. For the representative case of Imax=110 mA, RLx would be about 4.53 ohms as Vbe(on) will be approximately 0.5 Volts for small collector currents. Typical depletion-mode FET devices such as Supertex DN3535 put RMOS 1  and RMOS 2  have roughly 10 ohms each. This makes for a total insertion resistance of approximately 30 ohms. When Ain is positive with respect to Bin, diode D 2  ensures that no current bypasses the load via the base-collector junction of Q 2 . Diode D 1  serves the same function for Q 1  for the opposite polarity of input signal. 
     Additional modifications to the current limiter  200  are possible. For the embodiment of  FIG. 8 , the feedback control element  603  is implemented via a BJT transistor. As known to those in the art, Vbe(on) of a BJT varies with temperature at a rate of approximately—2 mV/degree Centigrade, causing Imax to vary with temperature as well. Other feedback control instantiations may not have a temperature dependence, but in this case,  FIG. 9  shows an exemplary configuration that compensates for temperature variance such that Imax does not vary with temperature. By choosing appropriate values, the voltage divider feeding the base-emitter junction of BJT Q 1 , formed by resistor R 10  and Rtherm 1 , varies at an effective rate of +2 mV/degree Centigrade, where Rtherm 1  is a negative temperature coefficient (NTC) thermistor. The net result is that the current required, Imax, to activate the feedback control element  603  is independent of temperature. Similar compensation is accomplished for BJT Q 2  by the addition of resistor R 20  and Rtherm 2 , which is an NTC thermistor. Compensation can be accomplished for the CL  200  based on enhancement-mode FETs via similar changes to the embodiment shown in  FIG. 7 . 
       FIG. 9  also shows an additional modification that protects the CL  200  from large AC over-voltage conditions such as those that might be experienced during a 60 Hz power fault. During normal operation, nodes Ain and Aout are connected via a low impedance (RL 2 +RMOS 1 ), and are, therefore, at very nearly the same potential for small signal operation. During a fault condition, though, large voltages could potentially be forced across the Ain to Aout nodes. Should the voltage at node Ain become sufficiently negative relative to Aout, capacitor C 1  charges via resistor R 11 , zener diode DZ 1 , and diode Dbypass 1 . During the half-cycle of the AC fault where Ain is positive with respect to Aout, the stored charge on C 1  shuts off M 1  so that M 1  is not dissipating large amounts of power, thereby protecting the current-limiter  200  from component failure. The charge on C 1  is replenished every negative half-cycle, keeping M 1  turned off for the duration of the fault. In this way, M 1  is not exposed to abusive amounts of power during a fault condition. When the fault is removed, C 1  discharges, M 1  returns to a low-impedance state, and normal operation resumes. Capacitor C 2 , zener diode DZ 2 , and diode Dbypass 2  provide similar protection to M 2  that can be understood via the symmetry of the circuit. 
     Diode Dbypass 1  sits in parallel with the integrated source-to-drain diode of M 1 . The integrated FET diode in many readily available parts is small and not intended to carry large currents. As Dbypass 1  is larger, it turns on at a lower voltage, thus carrying the majority of the current and protecting such integrated diodes from damage. Dz 1  protects the gate-to-source junction of M 1  from damaging voltages, and also provides a path to charge capacitor C 1 . Diode D 10  protects the base-to-emitter junction of Q 1  from excessive reverse voltages. 
     Diode Dbypass 2  sits in parallel with the integrated source-to-drain diode of M 2 . As Dbypass 2  is larger, it turns on at a lower voltage, thus carrying the majority of the current and protecting such integrated diodes from damage. Dz 2  protects the gate-to-source junction of M 2  from damaging voltages, and also provides a path to charge capacitor C 2 . Diode D 20  protects the base-to-emitter junction of Q 2  from excessive reverse voltages. 
       FIG. 10  is an exemplary configuration using enhancement-mode FETs. The embodiment shown by  FIG. 10  is identical to that shown by  FIG. 7  except that various components have been added for providing circuit protection and compensating for temperature fluctuations as described above for the embodiment depicted by  FIG. 9 . In particular, temperature dependent thermistors Rtherm 1 , Rtherm 2  have been added to compensate for temperature fluctuations, and zener diodes D 3 , D 7  have been added to protect the circuit from damaging voltages. 
     In the embodiments shown by  FIGS. 7-10 , it can be observed that the components of the current limiter  200  are not connected to a reference voltage (e.g., the load&#39;s ground). Indeed, the voltages of the current limiter components float with the line voltage enabling the current limiter to handle a wide range of voltages. 
     While the embodiments of the present disclosure have been described in detail, it is to be expressly understood that it will be apparent to persons skilled in the relevant art that the embodiments may be modified without departing from the spirit of the disclosure. Various changes of form, design or arrangement may be made to the disclosure without departing from the spirit and scope of the disclosure.