Wednesday, 30 December 2015

Introduction of Electric Car

You need the following to get started:
- Detailed pre-plans on how to construct your own electric car.
- You can use any vehicle- gas, diesel 
- A garage, shop or barn is nice, but not necessary 
- Simple tools every home workshop has- wrenches, drills etc. 
- A large DC motor (9 inches or larger) and a source of  batteries. Note that AC motors can be used as well but they are a bit more expensive so we went with DC. They are easier to install too. 
- You can, of course buy all these parts brand new but this is the heaviest cost of the whole project so we suggest using the sources of free DC motors and free industrial batteries listed in the plans. 
- They’re not hard to find either and since a DC motor will run for probably longer than you will own your car, using salvaged motors makes sense.
- After obtaining your DC motor and batteries you have to remove your gas engine from your car. 
- Leave the clutch and flywheel assembly and detach the rest. That will leave you room for batteries and DC motor mounting. 
- It is imperative that you only use a standard transmission vehicle for your conversion as automatic transmissions simply won’t work. 
- Don’t worry, you won’t even have to shift gears in traffic once the conversion is done. It will drive just like an automatic transmission, which is nice. Put it in gear and go. When you stop the engine simply stops too. It doesn’t keep idling, requiring clutching like a gas engine. 





Learning how to build your own electric car is a lot of fun too. Putting together the controller and motor assembly is not that difficult either. 

Your new Electric car will be able to go 50 mph and travel up to 200 miles on a single charge too. Isn’t it amazing. Try it!!

Monday, 21 December 2015

WORKING PRINCIPLE OF STEPPER MOTOR


Stepper motors consist of a permanent magnetic rotating shaft, called the rotor, and electromagnets on the stationary portion that surrounds the motor, called the stator. Figure 1 illustrates one complete rotation of a stepper motor. At position 1, we can see that the rotor is beginning at the upper electromagnet, which is currently active (has voltage applied to it). To move the rotor clockwise (CW), the upper electromagnet is deactivated and the right electromagnet is activated, causing the rotor to move 90 degrees CW, aligning itself with the active magnet. This process is repeated in the same manner at the south and west electromagnets until we once again reach the starting position.



Figure 1
In the above example, we used a motor with a resolution of 90 degrees or demonstration purposes. In reality, this would not be a very practical motor for most applications. The average stepper motor's resolution -- the amount of degrees rotated per pulse -- is much higher than this. For example, a motor with a resolution of 5 degrees would move its rotor 5 degrees per step, thereby requiring 72 pulses (steps) to complete a full 360 degree rotation.
You may double the resolution of some motors by a process known as "half-stepping". Instead of switching the next electromagnet in the rotation on one at a time, with half stepping you turn on both electromagnets, causing an equal attraction between, thereby doubling the resolution. As you can see in Figure 2, in the first position only the upper electromagnet is active, and the rotor is drawn completely to it. In position 2, both the top and right electromagnets are active, causing the rotor to position itself between the two active poles. Finally, in position 3, the top magnet is deactivated and the rotor is drawn all the way right. This process can then be repeated for the entire rotation.



Figure 2
There are several types of stepper motors. 4-wire stepper motors contain only two electromagnets, however the operation is more complicated than those with three or four magnets, because the driving circuit must be able to reverse the current after each step. For our purposes, we will be using a 6-wire motor.
Unlike our example motors which rotated 90 degrees per step, real-world motors employ a series of mini-poles on the stator and rotor to increase resolution. Although this may seem to add more complexity to the process of driving the motors, the operation is identical to the simple 90 degree motor we used in our example. An example of a multipole motor can be seen in Figure 3. In position 1, the north pole of the rotor's permanent magnet is aligned with the south pole of the stator's electromagnet. Note that multiple positions are aligned at once. In position 2, the upper electromagnet is deactivated and the next one to its immediate left is activated, causing the rotor to rotate a precise amount of degrees. In this example, after eight steps the sequence repeats.



Figure 3
The specific stepper motor we are using for our experiments (ST-02: 5VDC, 5 degrees per step) has 6 wires coming out of the casing. If we follow Figure 5, the electrical equivalent of the stepper motor, we can see that 3 wires go to each half of the coils, and that the coil windings are connected in pairs. This is true for all four-phase stepper motors.



Figure 4
However, if you do not have an equivalent diagram for the motor you want to use, you can make a resistance chart to decipher the mystery connections. There is a 13 ohm resistance between the center-tap wire and each end lead, and 26 ohms between the two end leads. Wires originating from separate coils are not connected, and therefore would not read on the ohm meter.

                              CLICK HERE FOR MORE DETAILS


Auto Transformers basics.....

auto transformer

  An auto transformer is an electrical transformer having only one winding. The winding has at least three terminals which is explained in the construction details below.



Some of the advantages of auto-transformer are that,

  • they are smaller in size, 
  • cheap in cost, 
  • low leakage reactance,
  • increased kVA rating, 
  • low exciting current etc. 
An example of application of auto transformer is, using an US electrical equipment rated for 115 V supply (they use 115 V as standard) with higher Indian voltages. Another example could be in starting method of three phase induction motors

Construction Of Auto Transformer

 An auto transformer consists of a single copper wire, which is common in both primary as well as secondary circuit. The copper wire is wound a laminated silicon steel core, with at least three tappings taken out. Secondary and primary circuit share the same neutral point of the winding. The construction is well explained in the diagram. Variable turns ratio at secondary can be obtained by the tappings of the winding (as shown in the figure), or by providing a smooth sliding brush over the winding. Primary terminals are fixed.
Thus, in an auto transformer, you may say, primary and secondary windings are connected magnetically as well as electrically.

Working Of Auto Transformer

As I have described just above, an auto transformer has only one winding which is shared by both primary and secondary circuit, where number of turns shared by secondary are variable. EMF induced in the winding is proportional to the number of turns. Therefore, the secondary voltage can be varied by just varying secondary number of turns.
As winding is common in both circuits, most of the energy is transferred by means of electrical conduction and a small part is transferred through induction.



The considerable disadvantages of an auto transformer are,

  • any undesirable condition at primary will affect the equipment at secondary (as windings are not electrically isolated),
  • due to low impedance of auto transformer, secondary short circuit currents are very high,
  • harmonics generated in the connected equipment will be passed to the supply.

Unity Power Factor AC–DC Power Converter

·          This article presents a power converter and its control circuit for high-frequency-fed ac to dc conversion.
·        Based on the resonant technique, the input current is shaped to be sinusoidal and is forced to follow the high-frequency sinusoidal input voltage so as to achieve unity power factor.

·        With the proper selection of the characteristic impedance of the resonant tank, the converter is able to perform the function of a buck, boost, or buck–boost converter.
·         The initial condition of the resonant tank is used to control the output voltage gain of the converter.


fFOR MORE DETAILS: CLICK HERE

Saturday, 19 December 2015

CURRENT-FED PUSH–PULL CONVERTER TRIGGERING USING SOFT-SWITCHING

 A push–pull converter is suitable for low-voltage photovoltaic ac module systems, because the step-up ratio of the high-frequency transformer is high, and the number of primary-side switches is relatively small. 



However, the conventional push–pull converter does not have high efficiency because of high-switching losses due to hard switching and transformer losses (copper and iron losses) as a result of the high turn ratio of the transformer. In the proposed converter, primary-side switches are turned ON at the zero-voltage switching condition and turned OFF at the zero-current switching condition through parallel resonance between the secondary leakage inductance of the transformer and a resonant capacitor. The proposed push–pull converter decreases the switching loss using soft switching of the primary switches. In addition, the turn ratio of the transformer can be reduced by half using a voltage-doubler of secondary side. 

Saturday, 12 December 2015

ZETA CONVERTER



  • A  non isolated power factor corrected (PFC) converter is being proposed to be used at the front end to improve the power quality of an SMPS for a PC. 
  • The front end converter is able to reduce the 100 Hz ripple in its output that is being fed to the second stage isolated converter. 
  • The performance of the front-end Zeta converter is evaluated in three different operating conditions to select the best operating condition for the proposed SMPS system.


  • The zeta converter is a dc to dc converter .It can be operated at buck and boost modes.
  • we can able to step down either step up of the output voltage.




FOR  MORE DETAILS: CLICK HERE......



HPF CONVERTER WITH ZVS TRANSITION

  • This article presents a single-phase high-power factor ac/dc converter with soft-switching characteristic. The boost converter performs the function of power-factor correction (PFC) to obtain high power factor and low current harmonics at the input line.
  • The buck converter further regulates the dc-link voltage to provide a stable dc output voltage.

                        


  • Without using any active-clamp circuit or snubber circuit, the active switches of the proposed converter can achieve zero-voltage switching-on (ZVS) transition together with high power factor that satisfies the IEC 61000-3- 2 standards over a wide load range from 30% to 100% rated power.
  • The steady-state analysis is developed and a design example is provided. A prototype circuit of 60 W was built and tested.
  • Experimental results verify the feasibility of the proposed circuit with satisfactory performance

FOR MORE DETAILS: CLICK HERE.....