A bipolar electric motor is an electric motor with only two (hence bi-) poles to its stationary field. [1] They are an example of the simple brushed DC motor, with a commutator. This field may be generated by either a permanent magnet or a field coil.
The 'bipolar' term refers to the stationary field of the motor, not the rotor. [1] The rotors often have more than two poles, three for a simple motor and potentially more for a high-power motor. A two-pole rotor has the disadvantage that it is not self-starting in all positions and so requires to be flicked to start.
The first DC electrical motors, from the Gramme motor of the 1870s onwards, used bipolar fields. These early machines used crudely designed field pole pieces with long magnetic circuits, wide pole gaps and narrow pole pieces that gave only a limited flux through the armature. These fields were usually horseshoe-shaped, with either permanent horseshoe magnets or else either one or two field coils at some distance from the poles.
Early insulated wire was insulated, if at all, [notes 1] with wrappings of cotton thread. These coils could only handle a low temperature rise before overheating and burning out with a short circuit. The coils were thus long and shallow, sometimes of only a single layer of wire, which required a long core simply to contain their size. Single small coils could be mounted horizontally, but the most common arrangement used two tall coils side by side.
To improve the efficiency of the magnetic circuit, it was realised that multiple magnetic paths could be provided through the same armature. The two coils were now separated and placed at the sides of the motor, with their iron core as a sideways figure-8 circuit and the armature in a central pole gap. Flux from both coils passed through this gap. This gave a magnetic circuit that was shorter overall and thus had fewer magnetic losses. The more compact coil windings were made possible by the use of shellac for impregnating the windings and improving the reliability of their insulation.
Later designs, from around 1900, became more compact with shorter, more efficient magnetic circuits. The field coils now moved into short, squat internal coils around the pole pieces themselves. [1] The remainder of the magnetic circuit was a double-sided circular path around the casing of the motor. Whilst primarily designed to be more efficient, this also gave a far more compact layout in terms of space.
This circular layout also represented the end of the bipolar motor as an industrial power source. It was possible to place a second set of field coils and pole pieces within the same size of casing, giving a four-pole arrangement. Because of the more efficient provision of field flux around the entire circumference of the armature, this give a motor of almost twice the power, for the same armature current. [1] Armature current, and the associated commutator and brushgear, represented one of the most expensive parts of the motor to manufacture.
One of the last industrial uses for large bipolar motors was for the Milwaukee Road's class EP-2 electric locomotives of 1917. [2] The line had chosen to electrify its Coast Division route, using a voltage of 3,000 V DC. These were not the first electric locomotives produced and incorporated lessons learned from previous practice. Many early locomotives had used one or two large motors mounted on the locomotive frame, with drive to the wheels by traditional steam locomotive practice of coupling rods. Where AC motors were used, requiring many poles and thus large diameters, these frame-mounted motors appeared inevitable even though they required this maintenance-intensive mechanical drive to the wheels. An alternative system of nose-hung traction motors used small high-speed motors alongside each axle, driving through a reduction gearbox. This system would eventually predominate across both electric and diesel locomotives, but at this time it was difficult to produce a reliable high-power gearbox.
The "bi-polar" design used axle-mounted motors, driving each wheel directly. The axle formed the spindle of not only the wheels, but also the motor armature itself. This obviously simple system had been used before, but only for low-powered locomotives with lightweight motors. As the wheels and axle, and in this case the motor too, are unsprung by the suspension, any extra weight here would lead to poor riding qualities. To permit its use for these extremely powerful new locomotives, the motor was split in two. The armature was formed as part of the axle, but the much heavier field poles and coils were carried on the suspended frame of the locomotive. This gave an acceptable ride.
The complexity of this system was that the armature must now be free to move up and down relative to the field, as the suspension moves. With a contemporary four-pole motor, this would vary the pole gap at the upper and lower poles, probably to the extent that the armature hit the pole pieces (suspension travel being far larger than typical pole gaps). The solution was to return to the relatively antiquated bipolar motor. By placing the poles at the side of the armature and giving them flat vertical faces, the armature was free to move up and down between them. The motor design was relatively inefficient, even by the standards of the day, but these locomotives were designed for their power and haulage capacity with a generous supply of cheap hydro-electricity, rather than designed for efficiency.
Early "bi-polar" designs included the New York Central's pioneering S-Motor of 1904 and later T-Motor of 1913, however the Milwaukee Road's class EP-2 became the class most associated with the bi-polar motor, even garnering the name "Bi-Polar" for the class.
The EP-2 locomotives operated reliably and successfully for 35 years. They were eventually withdrawn owing to a general decline in US railroads in the late 1950s, the advent of cheap diesel power, and in particular to a rebuilding of the class that was poorly carried out and left the rebuilt locomotives with reliability problems.
The bipolar motor is still in widespread use today, in medium-power, low-cost applications such as the universal motors used in home appliances such as food mixers, vacuum cleaners and electric drills.
These motors are broadly the design of the brushed DC motor with series-connected field windings. They also work well on AC supplies and are now most commonly found on such. They offer greater torque and speed than induction motors and so have many applications where their capital cost and light weight are more important than their electrical efficiency.
The simple bipolar motor has been widely used in electric toys, since the early days of tinplate toys.
The first such motors used a simple horseshoe permanent magnet. More modern 'can' motors, from the 1960s onwards, have remained bipolar but have, like the industrial motors, used a more efficient pair of C-shaped magnets within a circular steel can case.
Owing to their additional cost and complexity, motors with field coils have only rarely been used for models. One well-known exception to this was the 'Taycol' range of motors, primarily aimed at larger model boats. [3] These had their heyday in the 1950s and 1960s, becoming obsolete and uncompetitive in price as more powerful materials for permanent magnets, specifically ferrite, became available.
Taycol began with simple horseshoe magnet motors, [4] but their real speciality was with wound fields. [5] Most of these used a single transverse field coil mounted above the rotor. Their larger 'Marine' and 'Double Special' ranges used a dual-coil layout, with two vertical field coils mounted at the sides. [3]
A similar, although smaller and far less powerful motor, was the Meccano E15R motor. [6] [7]
Construction of a simple bipolar motor, usually with a bipolar rotor as well, remains a popular basic science project for children. [8] [9]
An electromagnetic coil is an electrical conductor such as a wire in the shape of a coil, spiral or helix. Electromagnetic coils are used in electrical engineering, in applications where electric currents interact with magnetic fields, in devices such as electric motors, generators, inductors, electromagnets, transformers, and sensor coils. Either an electric current is passed through the wire of the coil to generate a magnetic field, or conversely an external time-varying magnetic field through the interior of the coil generates an EMF (voltage) in the conductor.
An electric motor is an electrical machine that converts electrical energy into mechanical energy. Most electric motors operate through the interaction between the motor's magnetic field and electric current in a wire winding to generate force in the form of torque applied on the motor's shaft. Electric motors can be powered by direct current (DC) sources, such as from batteries, motor vehicles or rectifiers, or by alternating current (AC) sources, such as a power grid, inverters or electrical generators. An electric generator is mechanically identical to an electric motor, but operates with a reversed flow of power, converting mechanical energy into electrical energy.
In electricity generation, a generator is a device that converts motive power into electrical power for use in an external circuit. Sources of mechanical energy include steam turbines, gas turbines, water turbines, internal combustion engines, wind turbines and even hand cranks. The first electromagnetic generator, the Faraday disk, was invented in 1831 by British scientist Michael Faraday. Generators provide nearly all of the power for electric power grids.
An alternator is an electrical generator that converts mechanical energy to electrical energy in the form of alternating current. For reasons of cost and simplicity, most alternators use a rotating magnetic field with a stationary armature. Occasionally, a linear alternator or a rotating armature with a stationary magnetic field is used. In principle, any AC electrical generator can be called an alternator, but usually the term refers to small rotating machines driven by automotive and other internal combustion engines.
A synchronous electric motor is an AC motor in which, at steady state, the rotation of the shaft is synchronized with the frequency of the supply current; the rotation period is exactly equal to an integral number of AC cycles. Synchronous motors contain multiphase AC electromagnets on the stator of the motor that create a magnetic field which rotates in time with the oscillations of the line current. The rotor with permanent magnets or electromagnets turns in step with the stator field at the same rate and as a result, provides the second synchronized rotating magnet field of any AC motor. A synchronous motor is termed doubly fed if it is supplied with independently excited multiphase AC electromagnets on both the rotor and stator.
A DC motor is any of a class of rotary electrical motors that converts direct current electrical energy into mechanical energy. The most common types rely on the forces produced by magnetic fields. Nearly all types of DC motors have some internal mechanism, either electromechanical or electronic, to periodically change the direction of current in part of the motor.
A traction motor is an electric motor used for propulsion of a vehicle, such as locomotives, electric or hydrogen vehicles, elevators or electric multiple unit.
In electrical engineering, an armature is the component of an electric machine which carries alternating current. The armature windings conduct AC even on DC machines, due to the commutator action or due to electronic commutation, as in brushless DC motors. The armature can be on either the rotor or the stator, depending on the type of electric machine.
The universal motor is a type of electric motor that can operate on either AC or DC power and uses an electromagnet as its stator to create its magnetic field. It is a commutated series-wound motor where the stator's field coils are connected in series with the rotor windings through a commutator. It is often referred to as an AC series motor. The universal motor is very similar to a DC series motor in construction, but is modified slightly to allow the motor to operate properly on AC power. This type of electric motor can operate well on AC because the current in both the field coils and the armature will alternate synchronously with the supply. Hence the resulting mechanical force will occur in a consistent direction of rotation, independent of the direction of applied voltage, but determined by the commutator and polarity of the field coils.
A field coil is an electromagnet used to generate a magnetic field in an electro-magnetic machine, typically a rotating electrical machine such as a motor or generator. It consists of a coil of wire through which a current flows.
A repulsion motor is a type of electric motor which runs on alternating current (AC). It was formerly used as a traction motor for electric trains but has been superseded by other types of motors. Repulsion motors are classified under single phase motors. In repulsion motors the stator windings are connected directly to the AC power supply and the rotor is connected to a commutator and brush assembly, similar to that of a direct current (DC) motor.
A Gramme machine, Gramme ring, Gramme magneto, or Gramme dynamo is an electrical generator that produces direct current, named for its Belgian inventor, Zénobe Gramme, and was built as either a dynamo or a magneto. It was the first generator to produce power on a commercial scale for industry. Inspired by a machine invented by Antonio Pacinotti in 1860, Gramme was the developer of a new induced rotor in form of a wire-wrapped ring and demonstrated this apparatus to the Academy of Sciences in Paris in 1871. Although popular in 19th century electrical machines, the Gramme winding principle is no longer used since it makes inefficient use of the conductors. The portion of the winding on the interior of the ring cuts no flux and does not contribute to energy conversion in the machine. The winding requires twice the number of turns and twice the number of commutator bars as an equivalent drum-wound armature.
An AC motor is an electric motor driven by an alternating current (AC). The AC motor commonly consists of two basic parts, an outside stator having coils supplied with alternating current to produce a rotating magnetic field, and an inside rotor attached to the output shaft producing a second rotating magnetic field. The rotor magnetic field may be produced by permanent magnets, reluctance saliency, or DC or AC electrical windings.
The rotor is a moving component of an electromagnetic system in the electric motor, electric generator, or alternator. Its rotation is due to the interaction between the windings and magnetic fields which produces a torque around the rotor's axis.
A brushed DC electric motor is an internally commutated electric motor designed to be run from a direct current power source. Brushed motors were the first commercially important application of electric power to driving mechanical energy, and DC distribution systems were used for more than 100 years to operate motors in commercial and industrial buildings. Brushed DC motors can be varied in speed by changing the operating voltage or the strength of the magnetic field. Depending on the connections of the field to the power supply, the speed and torque characteristics of a brushed motor can be altered to provide steady speed or speed inversely proportional to the mechanical load. Brushed motors continue to be used for electrical propulsion, cranes, paper machines and steel rolling mills. Since the brushes wear down and require replacement, brushless DC motors using power electronic devices have displaced brushed motors from many applications.
A dynamo is an electrical generator that creates direct current using a commutator. Dynamos were the first electrical generators capable of delivering power for industry, and the foundation upon which many other later electric-power conversion devices were based, including the electric motor, the alternating-current alternator, and the rotary converter.
In electrical engineering, electric machine is a general term for machines using electromagnetic forces, such as electric motors, electric generators, and others. They are electromechanical energy converters: an electric motor converts electricity to mechanical power while an electric generator converts mechanical power to electricity. The moving parts in a machine can be rotating or linear. Besides motors and generators, a third category often included is transformers, which although they do not have any moving parts are also energy converters, changing the voltage level of an alternating current.
A magneto is an electrical generator that uses permanent magnets to produce periodic pulses of alternating current. Unlike a dynamo, a magneto does not contain a commutator to produce direct current. It is categorized as a form of alternator, although it is usually considered distinct from most other alternators, which use field coils rather than permanent magnets.
A flux switching alternator is a form of high-speed alternator, an AC electrical generator, intended for direct drive by a turbine. They are simple in design with the rotor containing no coils or magnets, making them rugged and capable of high rotation speeds. This makes them suitable for their only widespread use, in guided missiles.
An alternator is a type of electric generator used in modern automobiles to charge the battery and to power the electrical system when its engine is running.
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