Fully Controlled AC to DC Converters

The ac to dc conversion with suitable examples and sketches are discuss here advanced. ac to dc conversion is needed to read as engineer student.

Single phase bridge with inductive load (With source inductance

Real AC sources have an internal impedance.Β  This is basically anΒ  β€œinternal inductance”, because internal resistance is often negligible. We denote this inductance as Ls per phase.

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Full-bridge thyristor converter with inductive load, with source inductance.

Because of 𝐿𝑠, current 𝐼𝑠 at input cannot make step changes at switchover points between  𝑇1,𝑇2  and  𝑇3,𝑇4 .  Current changes take time.  During this brief interval of time, both the outgoing and incoming pairs of thyristors conduct simultaneously.  This is called a β€œconduction overlap”.  The phase angle width of conduction overlap is called β€œconduction overlap angle”.

Conduction overlap angle is denoted by 𝑒.

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Waveforms of output voltage  𝑉 π‘œ , Input current   𝐼𝑠  and Converter input voltage   𝑉𝐴𝐡  

During overlap, all 4 thyristors conduct simultaneously and hence 𝑉 π‘œ = 0.   Let consider the overlap after triggering  𝑇1,𝑇2 pair. Using KVL,

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Reduction  βˆ†π‘‰ π‘œ of mean output voltage due to conduction overlap is,

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Input DisF gets deteriorated when the delay angle is increased.  This is a drawback of fully-controlled thyristor converters

Supply voltage VAB at the point of common coupling (PCC) is distorted with 2 notches per cycle, occurring at angle Ξ± from zero crossing.  These notches go down to zero volt, which is highly undesirable.  This is another drawback of thyristor converters.  Note that VAB is the input voltage for other loads connected to the PCC.

Depth of voltage notches can be reduced to an acceptable level by connecting an external inductor (Lc) at the converter input.  This avoids artificial zero-crossings in the voltage waveform.  Acceptable depth of notches are specified in power-quality standards.

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(Depth of voltage notch with converter inductance) =  (𝐿𝑠/( 𝐿𝑐 +𝐿𝑠)) X(Depth of voltage notch without converter inductance)

Example ac to dc conversion

A single-phase full-bridge converter is operating on 230 V, 50 Hz singlephase supply that has an internal inductance 2 mH. The converter delivers 12 A constant current at a mean voltage of 120 V DC to an inductive load.  Determine,

  • Operating delay angle
  • Conduction overlap angle
  • Input displacement-factor
  • RMS value of the fundamental component of supply current
  • Depth of voltage-notches at the point of common coupling (PCC)
  • Required converter inductance to reduce the depth of notches down to 25% and its influence on the values found in (i) to (iv).
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3-phase full-bridge with inductive load

3-phase full-bridge with inductive load
3-phase full-bridge with inductive load

Three-phase full-bridge thyristor converter with inductive load

Thyristor full-bridge operates quite similar to diode full-bridge but the turn-on points of thyristors are now delayed by angle Ξ±.  For continuous load current, one thyristor from the upper-half and other from the lowerhalf must conduct at any time.  Six line-line voltages at the input decide which pair should conduct at a given point of time.

Wave Patterns

Six line-line voltage waveforms at the converter input for a, b, c standard phase sequence

  1. Upper-half thyristors bear ODD numbers and lower-half thyristors bear EVEN numbers.
  2. Delay angle for a thyristor is measured from its β€œdiode-like” conduction point.
  3. Triggering order of thyristors turns out to be 1, 2, 3, 4, 5, 6, 1, …… 
  4. Consecutive trigger-points are 60Β° apart. 
  5. Once triggered, a thyristor conducts for 120Β° span until the next thyristor in that half takes over. 
  6. Between trigger points, two previously triggered thyristors conduct πΌπ‘œ (they are in upper and lower halves). 
  7. The pair that conducts at a time passes the corresponding line voltage on to 𝑉 π‘œ (eg:  𝑉 π‘œ ≑ 𝑉𝐴𝐡 when (1, 6) pair conducts). 

πΌπ‘Ž =    πΌπ‘œ if 𝑇1 is conducting

βˆ’πΌπ‘œ if 𝑇4 is conducting  

0 otherwise                    

𝑉1 =   0   if 𝑇1 is conducting

𝑉𝐴𝐡 if 𝑇3 is conducting

𝑉𝐴𝐢 if 𝑇5 is conducting

ac to dc conversion

Waveforms of Vo, Ia and V1 at an arbitrary delay angle Ξ±

ac to dc conversion

By varying  𝛼 between 0Β° to 180Β°, we can vary  π‘‰π‘œπ‘šπ‘’π‘Žπ‘› between 3( 2)^1/2 𝑉𝐿/ πœ‹ and βˆ’3 ( 2)^1/2 𝑉𝐿/ πœ‹ . Frequency of superimposed ripple in 𝑉 π‘œ is = 6 𝑓 𝑠 β«½

Fundamental component of input line current  πΌπ‘Ž  waveform is  𝛼 angle shifted forward, relative to the case of diode-bridge.   ∴ Input Displacement angle = 𝛼 β«½     Input Displacement Factor (DisF) = cos𝛼 β«½

ac to dc conversion

When  𝛼 is varied, Peak reverse voltage blocked by a thyristor= 2𝑉𝐿 β«½  Peak forward voltage blocked by a thyristor =  2𝑉𝐿 β«½

Example ac to dc conversion

Sketch Vo waveform for Ξ± = 90Β° and Ξ± = 150Β°.

ac to dc conversion

Output voltage waveform for Ξ± = 90Β°

ac to dc conversion

Output voltage waveform for Ξ± = 150Β°

The ac to dc conversion with suitable examples and sketches are discuss here advanced. ac to dc conversion is needed to read as engineer student.

3-phase full-bridge with inductive load (With source inductance)

a, b, c are supply side poles

A, B, C are converter-input poles

Ls is supply internal inductance per phase

Io is continuous

Input currents  πΌπ‘Ž,𝐼𝑏,𝐼𝑐 cannot make step changes at the points of commutation due to the presence of 𝐿𝑠.  Current changes taking a brief time during which both the outgoing thyristor and the incoming thyristor conduct simultaneously, creating conduction overlap. 

Phase-angle width of conduction overlap is β€œconduction overlap angle”, denoted by β€œu”.  During the brief conduction overlap, the newly triggered thyristor and two already conducting thyristors conduct simultaneously.

During overlap, three recently triggered thyristors conduct. Outside overlap, two recently triggered thyristors conduct.

Waveforms of output-voltage (𝑉 π‘œ), Input current (πΌπ‘Ž), Thyristor-voltage (𝑉1) and Line-line voltage (𝑉𝐴𝐡) at the PCC  

Outside the conduction overlaps, 𝑉 π‘œis not influenced by source inductance 𝐿𝑠, because input currents are constant at πΌπ‘œ or 0.  We want to identify 𝑉 π‘œ during overlaps, and derive an expression for conduction overlap angle 𝑒. Let consider the conduction overlap following the triggering of 𝑇1.  During this overlap  𝑇5,𝑇6,𝑇1 conduct simultaneously.

If we look carefully, 𝑉𝑐𝑏is the output voltage before the overlap, and π‘‰π‘Žπ‘is the output voltage after the overlap.  In general, we can state that β€œduring an overlap, the output voltage takes the mean between β€œpre-overlap 𝑉 π‘œ if continued through the overlap and the post-overlap 𝑉 π‘œ if advanced to the beginning of overlap

Reduction of Volt-radian area from 𝑉 π‘œ due to the conduction overlap is,

ac to dc power converter
ac to dc power converter

Waveform of Voltage  𝑉1across thyristor  𝑇1 indicates frequent step changes, which apply high 𝑑𝑉 𝑑𝑑 stress on the thyristor.  Therefore proper 𝑑𝑉 𝑑𝑑 protection using RC-snubber circuits is very important.  Otherwise, inadvertent triggering can occur, causing serious fault conditions.

Line-line voltage at the point of common coupling (PCC) contains 6 nos. of notches per cycle.  Four of these notches are shallow notches (of volt-radian area πœ”πΏπ‘ πΌπ‘œ) and two are deep notches (of volt-radian area 2πœ”πΏπ‘ πΌπ‘œ ).  Deep-notches occur at angle 𝛼 away from zero crossing points of the line-voltage, with a depth of  2𝑉𝐿 sin 𝛼 + 𝑒 2 .  The six notches are 60Β° spaced, each of width 𝑒 

ac to dc power converter

During overlaps, voltage 𝑉𝐴𝐡is related to 𝑉 π‘œaccording to KVL. Outside overlaps, 𝑉𝐴𝐡is equal to supply voltage π‘‰π‘Žπ‘.

𝑉𝐴𝐡 =     

     π‘‰π‘Žπ‘ outside overlaps                                                       𝑉 π‘œ during overlap after 𝑇1 where 5,6,1 conduct 𝑉 π‘œ during overlap after 𝑇2 where 6,1,2 conduct    0 during overlap after 𝑇3 where 1,2,3 conduct βˆ’π‘‰ π‘œ during overlap after 𝑇4 where 2,3,4 conduct βˆ’π‘‰ π‘œ during overlap after 𝑇5 where 3,4,5 conduct    0 during overlap after 𝑇6 where 4,5,6 conduct

Notches in the voltage at PCC are undesirable. In particular, two deep notches which touch zero-volt are highly undesirable. In practice, we use separate inductors at the converter input to reduce the depth of all notches by a factor, as required.  

ac to dc power converter

Depth of voltage notch with converter inductance =

𝐿𝑠 𝐿𝑐 +𝐿𝑠

  Depth of voltage notch without converter inductance

Example ac to dc conversion

Three-phase, full-bridge thyristor converter is operating on 50 Hz, 400 V threephase supply, that has an internal inductance 2 mH per phase.  The converter delivers 20 kW of power to an inductive load at a mean DC voltage of 380 V.  Load current can be assumed to be constant.    Determine, (i) Delay angle (ii) Conduction overlap angle (iii) Input Displacement Factor (iv) RMS value of the fundamental component of input current (v) Input inductance per phase required to reduce depth of notches of the line voltage at the PCC by 60%.

ac to dc power converter
ac to dc power converter
ac to dc power converter

3-phase full-bridge with Regenerative load (With source inductance)

The ac to dc power supply with suitable examples and sketches are discuss here advanced. ac to dc power supply is needed to read as engineer student.

3-phase full-bridge with Regenerative load

For loads with negative EMF, we can operate the converter as an inverter by making 𝛼 > 90Β°.  Then real power flows from the load back to the AC supply.  This is identified as a load commutated inverter (LCI)

Waveforms of output voltage and thyristor-1 voltage

For successful operation, β€’ Each incoming thyristor should be on forward-bias at the point of triggering. β€’ Each outgoing thyristor should immediately be under reverse-bias for a brief phase angle width, as determined by thyristor-turn-off time .

First condition is normally satisfied without difficulties. Always the conducting thyristor (in a given half) creates a forward bias across the next in line at the point of triggering.   For example, conducting T5 creates a forward bias across T1 at triggering of T1. Second condition, however, should be guaranteed by restricting the maximum delay angle below 180Β°.  Then the outgoing thyristor will be subjected to reverse bias over a brief phase-angle slot.  If this slot is wider than the β€œturn-off angle” specified for the particular thyristor, the commutation will be successful.

For example, in the waveforms, outgoing T1 is subjected to reverse bias for a phase angle span Ξ³.

𝛾 = Extinction angle 𝛾 = 180Β°βˆ’ 𝛼 +𝑒  If 𝛾 is greater than the β€œturn-off-angle”, the commutation will be successful.  In general, about a 15Β° allocation for extinction angle is a reasonable choice, which for 50 Hz AC operation amounts to about 0.8 ms reservation (thyristor turn off times are much shorter than 0.8 ms).

Example ac to dc conversion

A three-phase thyristor full-bridge is operating on 400 V, 50 Hz three-phase AC supply that has internal inductance 2 mH per phase.  Thyristors used in the bridge needs a reservation of 500 ΞΌs for the turn-off time. Determine, (i) Minimum extinction angle required (ii) Peak real power that can be returned back to the AC source at a time when the converter is delivering 30 A current to an inductive load.

ac to dc power supply

Greatest reversal of power occurs when the delay angle is changed stepwise to cause the highest acceptable reverse voltage at the load, because current πΌπ‘œis still continuing due to load inductance. 

Β π‘ƒπ‘šπ‘Žπ‘₯ π‘Ÿπ‘’π‘”π‘’π‘› = 512.2Γ—30 W = 15336 Wβ«½

The ac to dc conversion with suitable examples and sketches are discuss here advanced. ac to dc conversion is needed to read as engineer student.

Reference ac to dc conversion

  1. Page ac to dc conversion
  2. Page ac to dc conversion

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