Showing posts with label motor. Show all posts
Showing posts with label motor. Show all posts

Friday, March 24, 2017

H Bridge Motor Speed Controller



H Bridge Motor Speed Controller



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Sunday, March 5, 2017

Basic Components of Electric Motor



Basic Components of Electric Motor


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Saturday, January 14, 2017

Carbon a Nonmetal ! But why it is used in Dc motor brushes



Carbon a Nonmetal ! But why it is used in Dc motor brushes



           One reason is the high melting temperature of carbon. 

The inductances of the energized windings, and the mechanics of a brush type motor or generator make arcing and sparking an unavoidable characteristic  of the machine at the brush interface. Electrical arcs produce very high temperatures. High enough to melt metals. 

Carbon has a very high melting point (~3500degC) compared with other conductors. Brushes made with copper or steel would wear out faster because of factors including:
1) The melted metal will break away from, or even be vaporized, leaving the brush with less material to do its job.
2) If the melted material doesnt vaporize or otherwise move away from the interface, it creates a mess for the brush. It can weld together bristles of the brush. It can build up material that interferes with the motion of the rotor.
3) As the metal melts in the presence of an arc, conductive material can be liberated, therby prolonging the arc, exasperating the wearing action.

Carbon is less prone to those high temperature effects and associated impacts to the generator operation.

Source : Dan Church

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Thursday, November 17, 2016

Understand the back emf in a d c motor



Understand the back emf in a d c motor


The back emf in a d.c motor

            In order to understand the idea of back e.m.f in a d.c. motor we will think about an electric car, or milk delivery van, going up and over a hill as shown in Figure 1. 


As soon as the coil in the motor starts rotating, a back e.m.f. will be induced in it due to the flux that it cuts, and this will tend to reduce the current through it.
Let the supply e.m.f. be E, the back e.m.f. be e, the resistance of the coil R and the current through the coil I. Then

I = [E – e]/R since e is proportional to the angular speed (?) the greater ? the smaller I.

For practical motors with E = 100 V, the back e.m.f. may be great as 95 V!

The resistance of the coil R is usually small (less than 1?) and therefore when it is at rest a large current may flow through it. When the coil speeds up this is reduced, since the back e.m.f. is proportional to the rate of rotation of the coil. The starting current can be as large as 1000 A, and a protective resistor must be incorporated in series with the coil during starting. This can be removed when the motor is running. This is why a d.c. motor that is running should never be stopped with the supply connected. If this is done the back e.m.f. will fall to zero, the current will become very large and the coil may burn out.

The diagram shows an electric car run by a 60 V battery going over a hill. It should help to explain what happens when the motor runs at different speeds. As the car climbs the hill AB on the left the motor is running slowly, the back e.m.f. is therefore low (say 5 V) and this means that a large current flows through the motor, giving a large torque. Chemical energy from the battery is converted to potential energy of the car.

The car now goes up section BC. The slope is much shallower, the motor speeds up and so the back e.m.f. rises to say 59 V. The current through the motor is therefore low.

The car now descends the section CD. The speed increases so that the back e.m.f. rises to 60 V, and energy is supplied to just overcome friction. Further down the hill, however, the car is moving faster and the back e.m.f. is greater than 60 V and so the motor acts as a dynamo, storing up energy in the battery. The current flowing produces a torque which tends to oppose the motion and so acts as a brake.

As long as electromagnets are used for the field, a d.c. motor will run on a.c., although very inefficiently owing to the large self-inductance of its coils.

Source : School Physics

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Wednesday, November 9, 2016

Brushless DC Motor How it works



Brushless DC Motor How it works


Brushless DC Motor, How it works ?

                    In order to make the operation more reliable, more efficient, and less noisy the recent trend has been to use brushless D.C motors. They are also lighter compared to brushed motors with the same power output. This article gives an illustrative introduction on the working of BLDC motors.
                    

Why BLDC motors ?

The brushes in conventional D.C motors wear out over the time and may cause sparking. This is illustrated in the Fig.1. As a result the conventional D.C motors require occasional maintainance. Controlling the brush sparking in them is also a difficult affair.
power flow in automobile
Fig.1 The brushes in a conventional D.C motor might cause sparking as shown
Thus the brushed D.C motor should never be used for operations that demand long life and reliability. Fort this reason and the other reasons listed in the introduction, BLDC motors are used in most of the modern devices. Efficiency of a BLDC motor is typically around 85-90%, whereas the conventional brushed motors are only 75-80% efficient. BLDC motors are also suitable for high speed applications ( 10000 rpm or above). The BLDC motors are also well known for their better speed control.

The Basic working

The rotor and stator of a BLDC motor are shown in the Fig.2. It is clear that, the rotor of a BLDC motor is a permanent magnet.
power flow in automobile
Fig.2 The Rotor of a BLDC is a permanent magnet; the stator has a winding arrangment
The stator has a coil arrangement, as illustrated; The internal winding of the rotor is illustrated in the Fig.3 (core of the rotor is hidden here). The rotor has 3 coils, named A, B and C.
power flow in automobile
Fig.3 The coil arrangement in a BLDC is shown here, with different color for different coils
Out of these 3 coils, only one coil is illustrated in the Fig.4 for simplicity. By applying DC power to the coil, the coil will energize and become an electromagnet.
power flow in automobile
Fig.4 The coil energized by a DC power source becomes an electromagnet
The operation of a BLDC is based on the simple force interaction between the permanent magnet and the electromagnet. In this condition, when the coil A is energized, the opposite poles of the rotor and stator are attracted to each other (The attractive force is shown in green arrow). As a result the rotor poles move near to the energized stator.
power flow in automobile
Fig.5 The rotor moves towards the energized coil, due to the attractive force
As the rotor nears coil A, coil B is energized. As the rotor nears coil B, coil C is energized. After that, coil A is energized with the opposite polarity (compare the last part of Fig.6 with Fig.5).
power flow in automobile
Fig.6 In a BLDC, as the rotor nears the energized coil, the next coils is energized; this will make the rotor continuously rotate
This process is repeated, and the rotor continues to rotate. The DC current required in the each coil is shown in the following graph.
power flow in automobile
Fig.7 The DC voltage required in each coil is shown in this graph
A humorous analogy help to remember it is to think of BLDC operation like the story of the donkey and the carrot, where the rabbit tries hard to reach the carrot, but the carrot keeps moving out of reach.
power flow in automobile
Fig.8 Just like the donkey runs after the carrot, in a BLDC the rotor runs after the moving magnetic flux

Further improving the BLDC Performance

Even though this motor works, it has one drawback. You can notice that, at any instant only one coil is energized. The 2 dead coils greatly reduce the power output of the motor. Here is the trick to overcome this problem. When the rotor is in this position, along with the first coil, which pulls the rotor, you can energize the coil behind it such a way that, it will push the rotor.
power flow in automobile
Fig.9 One more coil is energized in practical motors; this will result in a push force apart from the pull force
For this instant, a same polarity current is through the second coil. The combined effect produces more torque and power output from the motor. The combined force also makes sure that a BLDC has a beautiful, constant torque nature. Such torque nature is difficult to achieve in any other type of motors.
power flow in automobile
Fig.10 The BLDC has a constant torque nature as shown.
The current form required for the complete 360 degree rotation is shown in the graph below.
power flow in automobile
Fig.11 The voltage form required in each of the coil
With this configuration 2 coils need to be energized separately, but by making a small modification to the stator coil, we can simplify this process. Just connect one free end of the coils together, as shown in the Fig.10.
power flow in automobile
Fig.12 Connecting one free ends of the coil together makes the BLDC voltage regulation much simpler
When the power is applied between coils A and B, let’s note the current flow through the coils. By comparing second part of the Fig.13 with Fig.9, it is clear that, the current flow is just like the separately energized state.
power flow in automobile

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