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Showing posts with label for. Show all posts

Tuesday, May 14, 2013

Special Considerations for Transformer Protections

  Current Transformers
Current transformer ratio selection and efficiency require unique consideration when applying transformer safety. Unique factors related to transformers, including its winding ratios, magnetizing inrush present, and the presence of winding faucets or load tap changers, are supplys of troublesomeies in engineering a loyal and steady protection scheme for the transformer.
Errors attributable to CT saturation and load-tap-changers are in particular very important for differential protection schemes the place the presents from a couple of set of CTs are when compared. To catch up on the saturation=mismatch blunders, overcurrent relays have to be set to function above these error.

CT Current Mismatch
Under normal, non-fault conditions, a transformer differential relay ought to ideally have equivalent presents in the secondaries of all current transformers linked to the relay in order that no present would drift in its working coil. It is tough, on the different hand, to match current transformer ratios exactly to the transformer winding ratios. This activity grow to bes not possible with the presence of transformer off-load and on-load faucets or load tap changers that vary the voltage ratios of the transformer windings depending on machine voltage and transformer loading.
The excessiveest 2ndary current mismatch between all present transformers linked within the differential scheme have to be calculated when selecting the relay operating environment. If time lengthened overcurrent protection is used, the time prolong atmosphere must also be based on the same consideration. The mismatch calculation needs to be performed for maximum load and through-fault stipulations.

CT Saturation
CT saturation can have a poor affect on the power of the transformer safety to function for inner faults (dependability) and to no longer operate for external faults (security).

For internal faults, dependability of the harmonic restraint type relays will be terriblely impacted if current harmonics generated within the CT secondary circuit due to CT saturation are excessive sufficient to restrain the relay. With a saturated CT, 2nd and 3rd harmonics predominate firstly, however the even harmonics progressively disappear with the decay of the DC element of the fault present. The relay may then function sooner or later when the restraining harmonic part is decreased. These relays on an ordinary basis embody an immediate overcurrent point that's now not restrained with the help of harmonics, however is ready very high (typically 20 times transformer rating). This element may operate on severe inside faults.
For exterior faults, safety of the differentially connected transformer safety may be jeopardized if the present transformers’ unequal saturation is extreme sufficient to produce error present above the relay surroundings. Relays geared up with restraint windings in each and every present transformer circuit would be safer.
The safety downside is particularly crucial when the present transformers are connected to bus breakers quite than the transformer itself. External faults on this case will be of very excessive magnitude as they are not restricted by means of the transformer impedance.

Magnetizing Inrush (Initial, Recovery, Sympathetic)

Initial
When a transformer is energized after being de-energized, a transient magnetizing or thrilling present that will reach instantaneous heights of up to 30 instances full load present may just go with the flow.
This can cause operation of overcurrent or differential relays defending the transformer. The magnetizing current flows in just one winding, for this reason it's going to seem to a differentially related relay as an internal fault.
Techniques used to prevent differential relays from operating on inrush embody discoverion of present harmonics and 0 present intervals, each being traits of the magnetizing inrush current. The former takes advantage of the presence of harmonics, particularly the second harmonic, within the magnetizing inrush present to restrain the relay from operation. The latter differentiates between the fault and inrush currents by way of measuring the zero current periods, with the intention to be for a lot longer for the inrush than for the fault present.

Recovery Inrush
A magnetizing inrush current may additionally waft if a voltage dip is followed by restoration to standard voltage.
Typically, this happens upon elimination of an exterior fault. The magnetizing inrush is frequently less severe on this case than in preliminary energization as the transformer was to no longertally de-energized previous to voltage recovery.

Sympathetic Inrush
A magnetizing inrush present can float in an energized transformer when a nearby transformer is energized. The offset inrush current of the financial institution being energized will discover a parallel path within the energized bank. Again, the magnitude is regularly less than the case of initial inrush. Both the recovery and sympathetic inrush phenomena recommend that restraining the transformer protection on magnetizing inrush current is required at all instances, not most effective when switching the transformer in carrier after a interval of de-energization.

Primary-Secondary Phase-Shift
For transformers with usual delta-wye connections, the presents on the delta and wye sides will have
a  308phase shift relative to one another. Current transformers used for traditional differential relays must
be linked in wye-delta (opposite of the transformer winding connections) to catch up on the
transformer section shift.
Phase correction is regularly insidely equipped in microprocessor transformer protection relays via
software virtual interposing CTs for every transformer winding and, as with the ratio correction, will
depend upon the selected configuration for the restrained inputs. This permits the primary current
transformers to all be related in wye.

Turn-to-Turn Faults
Fault currents on account of a turn-to-turn fault have low magnitudes and are laborious to discover. Typically, the fault must evolve and have an effect on a just right section of the winding or arc over to other sections of the transformer ahead of being noticeed by means of overcurrent or differential protection relays.
For early noticeion, reliance is usually made on tools that can measure the ensuing accumulation of fuel or changes in power within the transformer tank.

Through Faults
Through faults could have an effect on each the transformer and its protection scheme. Depending on their severity, frequency, and duration, via fault presents can result in mechanical transformer harm, even though the fault is just a little limited through the transformer impedance.
For transformer differential protection, present transformer mismatch and saturation could produce operating currents on through faults. This need to be taken into consideration when choosing the scheme, current transformer ratio, relay sensitivity, and running time. Differential protection schemes geared up with restraining windings offer better security for these via faults.

Backup Protection
Backup safety, generally overcurrent or impedance relays applied to at least one or either facet of the transformer, carry out two performs. One perform is to againup the principle safety, most likely a differential relay, and operate in adventure of its failure to commute.
The second operate is safety for thermal or mechanical injury to the transformer. Protection that may become mindful of these external faults and operate in time to prevent transformer harm needs to be considered. The protection must be set to operate ahead of the thru-fault stand up to capability of the transformer is reached.If, on account of its large measurement or significance, most effective differential protection is applied to a transformer, clearing of external faults earlier than transformer damage can occur by other protective tools have to be ensured
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LED Flasher for RC Planes

This is so useful circuit for Rc lovers.Because you can use this circuit simply for your Rc plane or RC car.Here I have used common IC NE 555.So easily you can find it.

Note

* This circuit operates with 6V power supply.

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Sunday, April 21, 2013

Vocal Adaptor for Bass Guitar Amp

These days, music is a major hobby for the young and not-so-young. Lots of people  enjoy  making  music,  and  more  and  more dream of showing off their talents on stage. But one of the major problems often encountered is the cost of musical equipment. How many amateur music groups sing  through an amp borrowed from a guitarist or bass player?
This is where the technical problems arise not in terms of the .25” (6.3 mm)  jack, but in terms of the sound quality (the words  are barely understandable) and volume (the amp  seems to produce fewer decibels than for a guitar). What’s more, unpredictable feedback may cause damage to the speakers and is very unpleasant on the ear. This cheap little  easy-to-build project can help solve these technical  problems.
Circuit diagram :
Vocal Adaptor for Bass-Guitar Amp-Circuit Diagram
A guitar (or bass guitar) amplifier is designed first and foremost to reproduce the sound of the guitar or bass as faithfully as  possible. The frequency response of the amp doesn’t need to be as wide or as flat as in hi-fi (particularly at the high end), and so this sort of amplifier won’t permit faithful reproduction of the voice. If you build an adaptor to compensate for the amp’s limited frequency response by amplifying in advance the frequencies that are  then attenuated by the amp, it’s possible to  improve the quality of the vocal sound. That’s  just what this circuit attempts to do.
The adaptor is built around the TL072CN low-noise dual FET op-amp, which offers good value for money. The NE5532 can be used with almost the same sound quality, but at (slightly) higher cost. The circuit breaks  down into two stages. The first stage is used to match the input impedance and amplify the microphone signal. For a small 15 W guitar or bass amplifier, the achievable gain is  about 100 (gain = P1/R1). For more powerful amplifiers, the gain can be reduced to  around 50 by adjusting P1. The second stage amplifies the band of frequencies (adjustable using P2 and P3) that are attenuated by the guitar amp, so as to be able to reproduce the (lead)  singer ’s voice as clearly, distinctly, and  accurately as possible. To refine the adaptor and tailor it to your amplifier and speaker, don’t be afraid to experiment with the component values and the type  of capacitors.
The circuit can readily be powered using a 9 V battery, thanks to the voltage divider R4/R5 which converts it into a symmetrical  ±4.5 V supply.

Author : Jérémie Hinterreiter
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Wednesday, April 10, 2013

Voltage Tester for Model Batteries

With a suitable load, the terminal voltage of a NiCd or lithium-ion battery is proportional to the amount of stored energy. This relationship, which is linear over a wide range, can be used to build a simple battery capacity meter. 

Circuit Image :
 Voltage Tester for Model Batteries Image
Voltage Tester for Model Batteries Circuit Image 

This model battery tester has two functions: it provides a load for the battery, and at the same time it measures the terminal voltage. In addition, both functions can be switched on or off via a model remote-control receiver, to avoid draining the battery when it is not necessary to make a measurement. The load network, which consists of a BC517 Darlington transistor (T2) and load resistor R11 (15 Ω /5 W), is readily evident. When the load is active, the base of T1 lies practically at ground level. Consequently, T1 conducts and allows one of the LEDs to be illuminated. 

Circuit Diagram :
Voltage Tester for Model Batteries-Circuit Diagram
Voltage Tester for Model Batteries Circuit Diagram

The thoroughly familiar voltmeter circuit, which is based on the LM3914 LED driver, determines which LED is lit. The values of R6 and R7 depend on the type and number of cells in the battery. The objective here is not to measure the entire voltage range from 0 V, but rather to display the portion of the range between the fully charged voltage and the fully discharged voltage. Since a total of ten LEDs are used, the display is very precise. For a NiCd battery with four cells, the scale runs from 4.8 V to 5.5 V when R6 = R7 = 2 kΩ. The measurement scale for a lithium-ion battery with two cells ranges from 7.2 V to 8.0 V if R6 = 2 kΩ and R7 = 1 kΩ. 

For remote-control operation, both jumpers should be placed in the upper position (between pin 1 and the middle pin). In this configuration, either a positive or negative signal edge will start the measurement process. A positive edge triggers IC1a, whose output goes High and triggers IC1b. A negative edge has no effect on IC1a, but it triggers IC1b directly. In any case, the load will be activated for the duration of the pulse from monostable IC1b. Use P12 to set the pulse width of IC1a to an adequate value, taking care that it is shorter than the pulse width of IC1b. 

If the voltage tester is fitted into a remote-controlled model, you can replace the jumpers with simple wire bridges. However, if you want to use it for other purposes, such as measuring the amount of charge left in a video camera battery, it is recommended to connect double-throw push-button switches in place of JP1 and JP2. The normally closed contact corresponds to the upper jumper position,while the normally open contact corresponds to the lower position.

Parts :
Resistors:
R1,R2 = 47kΩ
R3 = 100kΩ
R4 = 500kΩ
R5 = 1kΩ
R6,R7 = see text (1% resistors!)
R8 = 1kΩ5
R9 = 1kΩ2
R10 = 330Ω
R11 = 15Ω 5W
R12 = 15kΩ
P1 = 100kΩ preset
Capacitors:
C1 = 10nF
C2 = 100nF
Semiconductors:
D1-D10 = LED, red, high effi-ciency
T1 = BC557
T2 = BC517
IC1 = 74HC123
IC2 = LM3914AN
Miscellaneous:
PC1,PC2,PC3 = solder pin
JP1,JP2 = jumper or pushbutton

PCB Layout :
B. PCB Laout
Voltage Tester for Model Batteries PCB Layout
 
 
Streampowers
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