tbu function

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© 200 5 FultecSe m icondu ctor Inc. 1 ww w.fulte c.com  Introduc ti on to  T B U P r ot e c ti o n By Dr. Richard Harris Ful te c Se m icondu ctor Inc.  J une 2005  _________________________________ ________________________ 1 BACKGROUND 1.1 THE SURGE THREA T Surge prote ction is the proce ss of prote cting e lectron ic system s or equipm ent from voltage s and current which are ou tside th eir sa fe ope rating l im its. The se s urge voltage s and cu rren ts can be gene rated by sh ort circui ts, lightni ng or f au lts from a p ower system and usua lly ente r the electronic system along inte r-eq uipme nt wiring. The surges m ay be galvani call y coupled into the systemas in the cas e of a direct li ghtn ing st ri ke, or through an ina dvertent conne ction of the power system to the wiring, or as a re sult of an e arth pot en tia l rise . The y m ay be ca pa citivel y coupled into the syste m which m ay occur when a data system is us ed in the vicinity of a high volta ge powe r l ine . The y ma y be inductively coupled into the syst em a s m a y occur if the wiring is run in parallel with large currents running in a power circuit feeding ahigh powe r motor.  The s iz e and waveformo f t he t ransients which can o ccur within a syst em are m an y and va ri ed . I n gen eral, however, the following will hold true: 1.  L ightning - Altho ug h direct s trike li gh tning cu rrent can pote ntially gen era te tra nsients in the m illion of  volts an d te ns of thousa nds of am ps, el ectronic eq uipm en t is rarel y expose d to surge s of thi s magn itude . The grea tes t exposure in telecomm uni cation syste m s is through inter- connecting te lecom m unication transm ission lines .  These lines can only ca r ry volt a ges up to 5kV and currents of the order of 1kA . The refore, for the vas t m ajori ty of insta nce s where the ch an ce of lightn ing strike dire ctly to the eq uipm e nt is low, 5kV an d 1kA is the limit of the direct strike or inductively gene rateds urges. 2 .  Powe r I nduc tion - Altho ug h po we r indu ction voltage s can b e qu ite high in voltage an d curren t, they are often a re lim ited in duration. The se voltag es a re caus ed by faults on the powe r system which couple into the system(usuall y inducti vel y as a conseq uence of the surge cau sing a ve ry l a rge fault curre nt). I n virtuall y all m ode rn power transm ission system s, the se fau lts a re very quickly terminat ed b y ci rcuit breake r and re -closer e qui pm ent. This ca n occur in as short as a couple of cycles of power frequ e ncy vol tage an d rarely take longer than a s econd. The se transients a re typicall y mode led as a 600Vrms waveform las ting up to a second . 3 .  Power cross - Alte rna tively, power cross volta ge s are low vol tage eve nts but the exposu re can occur for very long durations. They a re of ten ca use d by m aintenan ce e rror or cabling faults and can result i n m oderate currents (< 25 A) f lowing for a long pe riod of tim e (15 m inute s, for exam ple). The y are predom inate ly at m ains power supp ly voltage leve ls (100-240V rms). 4 .  Earth Potential Rise (EPR) - EPR can be cate gorized into two forms : 1) As a res ult of powe r system faults and 2) lightni ng discharge s. In norm al industry, where faul t curren ts from the p ower system are li m ite d in mag nitude by fuses a nd circuit brea kers, powe r system EPR is not us ua lly a considerable risk. EPR only becomes a significant ri sk when p ower ea rthing sys tem s a re signif ican tly below standa rd or whe re high power transm ission systems a re used such as at power generation and distribution facilities, within high power industry, and in the vicinity of electrical traction systems (electric rail ). I n suc h circum sta nce s, this type of surge ne e ds to be carefully ma nage d an d expe rt predicti ons ne ed to be m a de of the risk an d size of events. Lightn ing EPR can on ly resu lt due to dire ct strike to the buil ding housing the e quipme nt or in its im m ed iat e vicini ty. Such e vents a re uncom m on, unless the installation is particularly vulnerable due to location or e xtreme height (e .g. cell ular phone ba se-station an tenna e). The e qui pm en t exposure a s a resu lt of EPR can be very hi gh, and a t high ea rth resistance locat ions, m ay be com e a significa nt portion of the lightning current. 5.  All othe r forms of transien ts te nd to be lower e nergy forms not posing any additional risk to equipment if  

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©2005 Fultec Semiconductor Inc. 1 www.fultec.com 

I ntroduction to

 TBU P rotection

By Dr. Richard Harris

Fultec Semiconductor Inc.

 June 2005

 ___________________________________________________________________________________________________ 

1 BACKGROUND

1.1 THE SURGE THREAT

Surge protection is the process of protecting electronic

systems or equipment from voltages and current whichare outside their safe operating limits. These surgevoltages and currents can be generated by short circuits,lightning or faults from a power system and usually enterthe electronic system along inter-equipment wiring. Thesurges may be galvanically coupled into the system as inthe case of a direct lightning strike, or through aninadvertent connection of the power system to thewiring, or as a result of an earth potential rise. They maybe capacitively coupled into the system which may occurwhen a data system is used in the vicinity of a highvoltage power line. They may be inductively coupledinto the system as may occur if the wiring is run in

parallel with large currents running in a power circuitfeeding a high power motor.

 The size and waveform of the transients which can occurwithin a system are many and varied. In general,however, the following will hold true:

1.  Lightning - Although direct strike lightning currentcan potentially generate transients in the million of volts and tens of thousands of amps, electronicequipment is rarely exposed to surges of thismagnitude. The greatest exposure intelecommunication systems is through inter-connecting telecommunication transmission lines.

 These lines can only carry voltages up to 5kV andcurrents of the order of 1kA. Therefore, for the vastmajority of instances where the chance of lightningstrike directly to the equipment is low, 5kV and 1kAis the limit of the direct strike or inductivelygenerated surges.

2.  Power Induction - Although power inductionvoltages can be quite high in voltage and current, theyare often are limited in duration. These voltages arecaused by faults on the power system which coupleinto the system (usually inductively as a consequence

of the surge causing a very large fault current). Invirtually all modern power transmission systems,these faults are very quickly terminated by circuitbreaker and re-closer equipment. This can occur in asshort as a couple of cycles of power frequencyvoltage and rarely take longer than a second. These

transients are typically modeled as a 600Vrmswaveform lasting up to a second.

3.  Power cross- Alternatively, power cross voltages arelow voltage events but the exposure can occur forvery long durations. They are often caused bymaintenance error or cabling faults and can result inmoderate currents (<25A) flowing for a long periodof time (15 minutes, for example). They arepredominately at mains power supply voltage levels(100-240V rms).

4.  Earth Potential Rise (EPR) - EPR can becategorized into two forms: 1) As a result of power

system faults and 2) lightning discharges. In normalindustry, where fault currents from the power systemare limited in magnitude by fuses and circuitbreakers, power system EPR is not usually aconsiderable risk. EPR only becomes a significantrisk when power earthing systems are significantlybelow standard or where high power transmissionsystems are used such as at power generation anddistribution facilities, within high power industry, andin the vicinity of electrical traction systems (electricrail). In such circumstances, this type of surge needsto be carefully managed and expert predictions needto be made of the risk and size of events. LightningEPR can only result due to direct strike to thebuilding housing the equipment or in its immediatevicinity. Such events are uncommon, unless theinstallation is particularly vulnerable due to locationor extreme height (e.g. cellular phone base-stationantennae). The equipment exposure as a result of EPRcan be very high, and at high earth resistancelocations, may become a significant portion of thelightning current.

5. All other forms of transients tend to be lower energyforms not posing any additional risk to equipment if 

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protection has been suitably designed for the eventsdetailed above.

1.2 CONVENTIONAL PROTECTION

 There are two primary methods for implementingprotection against surge threats, namely, blocking thesurge or diverting (shunting) the surge. Nearly allconventional protection schemes used today are based onshunting architectures because of two fundamentalassumptions:

1)  Inexpensive devices whichshunt faults of 100sof amperes and 1000s of volts exist

2)  Inexpensive devices which block faults of 100sof amperes and 1000s of volts do not exist

 Therefore, conventional protection relies on the primaryform of protection being shunt device which divertcurrent. However, none of the available shunt devicesare sufficiently perfect to protect electronic equipment bythemselves.

Electronic equipment can be damaged by voltages in the10s of volts and currents in the 100s of milliamps if theypersist for any significant length of time (more thanmicro-seconds). Therefore, equipment protectionrequires a shunt protector that: 1) can react fast enoughto allow less than these values from reaching theequipment, and 2) can subsequently short circuit andprotect the interface from a surge which may peak on theorder of 1000A. Considering that the surge may developin a few micro-seconds, this is quite a difficult task.

Some primary protective devices are fast enough to reactin time, for example, semiconductor-based devices.However these devices tend to have limited currenthandling capability. Also, those semiconductor devicesrated for the primary protection task tend to capacitivelyload a circuit (due to their physically large size) resultingin bandwidth limitations.

Non-semiconductor surge protectors, such as the GasDischarge Tube (GDT), dont capacitively load circuitsand can handle very large current (10s of kilo-amperes).However, these devices are slow to react and dont keepthe voltages sufficiently low to provide successfulprotection by themselves.

 Therefore, conventional protection must be based on a

number of stages of such devices. These stages typicallystart with a GDT as the primary protector - for its currenthandling capability, followed up by a semiconductorthyristor protector for speed the secondary protector.

1.3 COORDINATION PROTECTION

When GDT and thyristor shunt protectors are used asprimary and secondary protectors, the protectioncoordination between them is always complicated in

practice. When a surge event occurs, the fast secondaryprotector will act to limit voltage within the system first(due to its speed). Often this protector will be rated tokeep the circuit voltages quite low in order to protect theequipment. Thus, its action will prevent the high energyprimary protector (GDT), which requires a highervoltage to operate, from working. In this circumstance,

damage is inevitable to the secondary protector beforethe GDT operates.

 This problem is solved by the complex process of inter-stage coordination. Coordination is the process of placing impedance between the primary and secondaryprotectors to ensure that sufficient voltage is generatedacross the primary protector, resulting from currentflowing in the secondary protector, to trigger the primarydevice. Coordination is engineered properly when theprimary protector operates after the secondary protectoroperates, yet before the secondary protector is damaged.

 The coordinating impedance can be resistive, capacitive,

inductive, non-linear or a combination of all of these;proper selection is critical.

Large resistance is the easiest choice to ensure that onlya small current in the secondary device causes asignificant voltage across the primary device causing itto operate. However, large resistance introducesconsiderable loss within the data transmission path whichis often intolerable. Capacitance and inductance are alsouseful, but these impedances are frequency related and socircuits coordinated with such will work only for a bandof surge frequencies. Non-linear resistance can also beused to create different coordinating arrangements basedon the duration of the surge - low level surges for

example which last a long time causing the coordinatingimpedance to change to a high resistance state chokingfurther current flow and triggering the primary protector(the basis of operation of the PTC). A typicalconventional POTS (Plain Old Telephone System)protection design with inter-stage protection is providedinFigure 1.

Figure 1. Conventional Protection - Circled partsindicating the secondary protection and the coordinatingimpedances.

In reality though, the process of selecting the bestcoordinating arrangement requires an in depthunderstanding of :

Interface

GDT Fuse Resistor Thyristor Diodes

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1. the surge threat;

2. the performance of all the protective componentsshunting and coordinating (voltage/current/power/energy/ time) characteristics in addition to theconditions with which they trigger or not;

3. the interfaces resistibility to voltages and currents

(voltage/current/time);4. the transmission system specifications (bandwidth,maximum allowable loss)

5. the interaction between multi-stage protectioncircuits.

And therein is the problem. The time and frequencydependent aspects of the coordination problem makethese circuits difficult to design with any degree of certainly. Consequently, testing must be used to assessthe performance of a protection design within a specificsystem - a requirement which has founded the vast arrayof testing and design standards which operate within the

market place. In addition, virtually all completed designshave inherent weaknesses - a weakness to sneak currents,a weakness to high energy surges, or a weakness tosurges of a particular frequency or at a particular rate of repetition - and these weaknesses cause field failures,replacement cost and lack of reliability.

2 IDEAL PROTECTION

Recall that secondary protection is only required toprevent the let-through energy of the primary protector(the energy of the surge which gets past the primaryprotector) from damaging the load.

By definition, the peak open circuit voltage of the let-through energy past the primary protector must besmaller than that of the initiating surge otherwise bydefinition, it is providing no protection at all. Therefore,a secondary protector which blocks rather than divertsthis lower, manageable and largely predictable voltagewould be very effective.

 The requirements for this ideal blocking device are self-evident:

1. As the device needs to block the let-through energy of the primary protector, it must be a series component (in

series with the transmission line), located just after theprimary protector. As a series component, the device willreact to the current through the device rather than voltageacross the interface.

2. This series device should have a predictable, stableand low trigger current (current at which the devicechanges between its conductive and non-conductivestate) to provide effective protection for sensitivedownstream equipment.

3. It should be very fast acting (less than 10nanoseconds) to protect equipment from surges whichrise to 5kV in a micro-second - as do direct lightningstrikes or lightning EPR;

4. It should be very low impedance (resistive, capacitiveand inductive) so that it does not effect normal circuitoperation;

5. In the blocking mode, it should be a very highimpedance so that it does not dissipate significant energyduring long duration surges;

6. It should be able to block voltages of the order of 1-2kV

7. It should automatically reset after the surge toreinstate the system and continue to allow normal systemoperation.

In addition, for practical and economic reasons it should be small in size and be low in cost. Fultecs TransientBlocking Unit (TBU) protector meets these

requirements.

3 FULTECS TBU

3.1 HOW THE TBU WORKS

3.1.1 General

 TBU protection takes a different approach to that of conventional protection. It is still based broadly on theassumption that a primary shunt protector is needed assurge currents are more manageable than surge voltages.However, it effectively replaces the need for secondaryprotection and coordination considerations, with onecomponent.

Fultec has developed the TBU to meet the requirementsof the ideal protector described in Section 2. In order tounderstand the operation of the TBU, it is useful topicture the TBU as having a current limiting functionalblock and a voltage disconnect functional block.

Figure 2. TBU functional block diagram

 The TBU responds to both over-current and over-voltagefaults as described in the following paragraphs.

LOAD

S

 TBUCURRENT

LIMITVOLTAGE

DISCONNECT LOAD

SS

 TBUCURRENT

LIMITVOLTAGE

DISCONNECT

CURRENTLIMIT

CURRENTLIMIT

VOLTAGE

DISCONNECT

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LOAD

Sshort

 TBU

CURRENTLIMIT

VOLTAGEDISCONNECT LOAD

SSshort

 TBU

CURRENTLIMIT

VOLTAGEDISCONNECT

CURRENTLIMIT

CURRENTLIMIT

VOLTAGEDISCONNECT

3.1.2 Over-current faults

Figure 3. Over-current fault diagram

With a short circuit event occurring at time 1 (see Figure4), the current rises to the current limiting level of Iout

(time 2, ~10 nano-seconds). At this point, the voltagedisconnect portion of the circuit operates and by time 3(~1 micro-second), the load is disconnected from thesurge. During the remainder of the surge (time 4), the

 TBU remains in the protected state of very low current

and voltage at the load.

1

2

3

4

Iout

Iop

Ileak

Vload

Vsource

time

nano-second

reaction time

~1µsec

1

2

3

4

Iout

Iop

Ileak

Vload

Vsource

time

nano-second

reaction time

~1µsec

 

Figure 4. TBU reaction to a over-current fault

3.1.3 Over-voltage faults

LOAD

S

SURGE  TBU

CURRENT

LIMIT

VOLTAGE

DISCONNECT LOAD

SS

SURGE  TBU

CURRENT

LIMIT

VOLTAGE

DISCONNECT

CURRENT

LIMIT

CURRENT

LIMIT

VOLTAGE

DISCONNECT

Figure 5. Over-voltage fault

With a lightning or power cross event at time 1 (seefigure 6), voltage and current rise until the currentlimiting portion of the circuit limits current to the levelof I out (time 2, ~10 nano-seconds). At this point, thevoltage disconnect portion of the circuit operates and by

time 3 (~1 micro-second), the load is disconnected fromthe surge. During the remainder of the surge (time 4),the TBU remains in the protected state of very lowcurrent and voltage at the load.

1

2

4

3

time

nano-second

reaction time

Ileak

Vload

Vsource

~1µsec

Iout

Iop

1

2

4

3

time

nano-second

reaction time

Ileak

Vload

Vsource

~1µsec

Iout

Iop

 

Figure 6. TBU reaction to an over-voltage fault

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3.2 TBU PERFORMANCE

3.2.1 Impulsive Surge Test Results

The following test results show the TBUs response to afast-rising lightning impulse. The test was done using a10/1000µs impulse generator as a voltage source with thepeak voltage set to 1200V. The test was conductedwithout shunt devices (i.e. with no GDT, thyristor orMOV).

LOAD100 ohms

 TBU

SS

Surge 1200V, 10/1000 sec

A B

Figure 7. Lightning impulse test circuit

Figure 8 shows the input waveform on the lower trace inred (voltage on the TBU input, VA) and the voltage at the

 TBU output on the upper trace in blue (VB). The TBUcurrent limited at ~280ma (i.e. 28V across the 100resistor) and then disconnected the load throughout theremainder of the surge. The peak voltage across the TBUwas ~1200 volts, just after it triggered to protect the load.

 The device automatically reset after the surge ended.

Figure 8. Impulse test of TBU device

3.2.2 AC Over-voltage

 The following tests show TBU performance against anAC over-voltage.

Voltage 600Vac

LOAD100 ohms

S

A B TBU

LOAD100 ohms

SS

A B TBU

Figure 9. AC Over-voltage test circuit

ACSource

 TBU triggers

2nd

3rd

4th

VA

VB

Figure 10. TBU blocking a 600Vrms power cross

At the onset of the surge, the TBU reacted to the

increasing current and triggered to protect the load. The TBU remained in the protected state throughout theremainder of the high voltage cycle. At each surge zero-crossing, the TBU reset in a micro-second, and thenretriggered to protect the load for each of the remainingcycles of the test. Once the fault was removed, thedevice reset to its normal, low impedance state.

4 SUMMARY

4.1 BLOCKING, NOT SHUNTING

In designing circuit protection, conventional wisdom hasheld that blocking devices that can cost effectively blockreal world surges do not exist. As a result, most circuitprotection schemes today rely on multiple shunt devicesto protect against surges. However, the currents that canoccur in such surges can be significant (100s of amps)and they can last a very long time (in the order of 1second to hours). This high current coupled withsignificant duration places a very large stress on all typesof shunt protective devices including GDTs, MOVs &thyristors.

Surge1200 V

 TBU triggers at 28 V

VA

VB

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However, a new protection device called the TransientBlocking Unit (TBU) has proven the conventionalwisdom to be out-dated. As a consequence, it is nowpossible to effectively block surges and prevent sensitiveload electronics being subjected to high levels of energyduring surge events.

4.2 CONCLUSION The TBU provides blocking protection for both powercross and lightning. Benefits of the TBU are over-voltage & over-current protection in one device,extremely high speed performance, high blockingvoltages & currents, precise output current and voltagelimiting, very high bandwidth, and a small size. Theseadvantages result in a protection device which exceeds

 Telcordia GR-1089 and ITU K.20/K.21 requirements,provides automatic protection coordination, and is GHzdata rate compatible all within a minimum of printedcircuit board area.

 The TBU protector provides the circuit protection designcommunity with a simple, superior protection device.