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  1. Time-division multiplexing is a technique/process that allows a link to be 'sectioned' in time slots, so different signals can be transmitted almost simultaneously using the same link. Each transmission uses the channel for a limited (and fixed) period of time (the time slot). In synchronous TDM, all.:
    The asynchronous nature of induction-motor operation comes from the slip between the rotational speed of the stator field and somewhat slower The self-excited synchronous motor, also called a switched-reluctance motor, contains a rotor cast of steel that includes notches or teeth, dubbed salient blessmerp.comg: pokie. ALARM_ON. KEY_OFF or. BELT _ON =>. END_TIMER_10 or. BELT_ON or. KEY_OFF => ALARM_OFF. If no condition is satisfied, implicit self-loop in the current state .. Synchronous vs. Asynchronous FSMs. • Synchronous (Esterel, StateCharts). – communication by shared variables that are read and written in zero time. Feedback elements are clocked. Asynchronous versus synchronous. Clock. Combinational. Logic. Combinational. Logic. Synchronous. Asynchronous. 4. CSE, Lecture In = 0. In = 1. In = 0. In = 1. Finite-state machines. ◇ States: Possible storage-element values. ◇ Transitions: Changes in  Missing: pokie.
  2. Syt 1 could also suppress asynchronous release by directly competing with the asynchronous Ca2+ sensor for the release machinery (11, 16). Whether Ca2+ binding to Syt 1 is required for these distinct roles in synchronous versus asynchronous release is unclear. To date, Ca2+ binding mutations in the.:
    Slots l4 thru l6 are for the autodial /autoanswer modem boards. Slot l3, the synchronous channel, can be used for a choice of boards; the RM l2.l2, RM-2OlB or RM-2OlC. Slots l4 and l5 contain RM-8OlA ACU dialer boards used to establish calls through the telephone circuits. Slot l6, the asynchronous channel, also uses a. The small air gap may result mechanical problems in addition to the noise and losses at the slot tooth faces. This reactive power is a function of the air-gap and a larger air-gap or low synchronous / magnetising reactance allows the synchronous machine to deliver and absorb higher levels of reactive power. This is very. Asynchronous Slot Multiplexing Taking the analogy of the cakes flowing on a conveyor belt with workers removing the cakes and packing them into boxes, there is an intuitive conservation of rate. The average rate at which the cakes are removed from the belt must equal the input cake rate (is the SI unit for cake rate, cps, or.
  3. Fractional-slot concentrated-windings (FSCW) have been gaining a lot of interest in Permanent Magnet (PM) synchronous machines. efficiency, higher power density, higher slot fill factor, lower manufacturing cost, better flux-weakening capability resulting in wider constant power vs. speed range, and fault-tolerance.:
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The University of Faisalabad. Induction motor air gap is less:. To avoide the noise. To improve the power factor. To avoide the leakage flux. Induction motor is operated in induction principal so. Islamic Azad University, Najafabad Branch.

Thanks for your valuable responses, but why air gap in synchronous machines is large with respect to induction ones? Private University Consortium Ltd. It is well known that due to being self-excited a synchronous machine is a source of reactive power.

This is very important as reactive power is required for establishing and maintaining the EM fields in a power system network and voltage stability. Also as power transfer along a transmission line is inversely proportional to the synchronous reactance it is desirable to have a low value to allow for higher active power transfer and a larger air-gap also allows for this. The IM machine on the other hand is self excited and must draw its reactive power from the supply. To limit the reactive power drawn from the supply one requires a high magnetising reactance which is achieved by using a smaller air-gap.

That is why transformers draw considerably less reactive power than IM's as Akhilesh points out above. Thus the SM has a large air gap for low magnetising reactance to allow higher reactive and active power to be delivered whereas the IM has a small air gap for higher magnetising reactance to limit the reactive power drawn.

It certainly is true and a very good, interesting and important question to have asked. Dear Diana very thanks for your comprehensive response. The magnetizing field in an IM has to jump the gap, the bigger the gap, the harder it is to get the flux induced in the rotor cage, and the more current it takes to get the job done i. Synchronous machines have a separately excited field in the rotor, it is fed through other means and does not have to jump across the air gap, so the gap is bigger to facilitate manufacturing.

According to me the stability of synchronous machine is indirectly related to air gap length. So to improve stability air gap is more for sync machines. Checkout the relations between short circuit ratio, airgap length, sync power coeficient.. And there is no problem of power factor in sync machines ,we can overexcite the machine.

Sri Jagadguru Chandrasekaranathaswamiji Institute of Technology. I think that short circuit protection is a factor. In the case of generator I suppose it is. Even as a sync motor an external fault would be fed. In an induction motor the rotor resistance being high. Islamic Azad University Mashhad Branch. In addition to the justifications above, which take into account that in induction machine model the magnetizing reactance is in parallel, but in synchronous machines the synchronous reactance is in series, another reason for larger airgaps in synchronous and DC machines in comparison to induction machines is the effect of armature reaction.

It is desirable to avoid distortion of the main flux created by rotor in synchronous machines and by stator in DC machines , this can be achieved by a larger airgap. Of course, this will lead to higher field current requirements and thus higher field circuit copper losses.

Can you help by adding an answer? Question followers 25 See all. To precisely analyze the timing of synaptic vesicle fusion in C2A and C2B mutants, we performed a detailed latency analyses Fig.

The latency histogram revealed a large asynchronous release component in C2A mutant rescued animals, which is more enhanced than that observed in null mutants Fig. We next assayed spontaneous release rates during the 0. Latency analyses of nerve-evoked synaptic currents. A Latencies of synaptic currents within 1 s following nerve stimulation were measured and plotted for each genotype as indicated in Fig.

All latencies were counted for each ms bin and presented as the number of events per stimulation in each bin. Examples containing spontaneous bursting activity originating from the CNS were excluded from the analysis. A small number of events triggered by endogenous action potentials, as well as spontaneous miniature release, were observed as random fusion events unrelated to stimulation in the background in each panel.

Data shown with enlarged y axis to highlight asynchronous release component. Note that the C2A mutant rescue displays a clear asynchronous component, whereas the C2B mutant rescue does not. In null mutants Left , the first bin does not show increased height compared with other bins, indicating no contribution of a synchronous component with the exponential distribution of asynchronous release component 9.

The numbers analyzed for each genotype were: B Quantification of asynchronous release. We counted release events occurring between 10 and ms per stimulation as the asynchronous component in the same experiments for A.

The numbers analyzed for each genotype were the same as those of A. C Quantification of spontaneous release. Synaptic currents were recorded between 0. Release frequency per second was calculated per animal.

Given occasional sparse action potential firings in motor neurons, these values are an overestimate of miniature release occurring at presynaptic terminals. Results were averaged between animals. The numbers of animal for each genotype were: To further characterize the role of the Syt 1 C2A domain in release, we extended the analysis of the synchronous and asynchronous release components at C2A mutant synapses.

These findings are consistent with the hypothesis that reduced suppression of synaptic vesicle fusion via the C2A domain enhances vesicle release. A The synchronous release component measured as charge transfer within 10 ms following nerve stimulation is plotted. Note that release at 0. B The asynchronous release component measured as charge transfer from 10 ms to ms following stimulation is plotted.

Asynchronous release at 0. Previous studies in Drosophila demonstrated that Syt 1 -null mutants have a smaller releasable vesicle pool as revealed by hypertonic stimulation 9 , This reduction in the releasable vesicle pool is hypothesized to result from a lack of Syt 1 binding to the soluble N-ethylmaleimide—sensitive fusion protein attachment protein receptor SNARE complex, the fusion machinery required for synaptic vesicle release The loss of SNARE binding by Syt 1 may disrupt intimate docking of synaptic vesicles with the plasma membrane, resulting in loss of synchronous fusion and reduction in hypertonic-induced release.

To determine whether the phenotypes observed in C2A and C2B mutations are caused by abnormalities in synaptic vesicle pool size, we performed hypertonic stimulation to measure fusion-competent vesicles.

As shown in Fig. These results indicate that phenotypes observed at C2A and C2B mutant synapses are not secondary to abnormal vesicle pool sizes. In summary, the defects in evoked transmission at synapses expressing C2A and C2B mutations reflect changes in release properties, as opposed to alterations in synaptic vesicle pool size.

Hypertonic-induced release reveals restoration of the readily releasable pool in the C2A and C2B mutant rescues. A Sample traces of hypertonic-induced release for each genotype.

Miniature synaptic currents occurring within 5 s after the onset of stimulation were counted. The numbers of samples analyzed for each genotype were: Recordings of nerve-evoked synaptic currents revealed contrasting roles for the two C2 domains in triggering fusion.

Transgenic rescue animals expressing Syt 1 with C2A mutations displayed enhanced asynchronous release and retained robust synchronous fusion, whereas Syt 1 with C2B mutations largely suppressed the asynchronous component, but limited ability to rescue synchronous fusion.

These observations suggest distinct roles for Syt 1 during the fusion process. Third, the enhanced asynchronous release observed in the absence of Syt 1 does not require reduction of the synchronous component, as observed in the C2A mutant rescue experiments.

Based on this model, asynchronous release is eliminated by binding of Syt 1 to SNARE complexes, preventing access of the asynchronous sensor to the fusion machinery. As the enhancement of asynchronous release observed in the C2A mutant rescue occurs without a corresponding reduction in synchronous fusion, it does not require a competitive reduction of the synchronous component. Support for the competition model was based on observations that total release between Syt 1 and WT neurons was unchanged at autapses 11 , but this is not observed at the calyx of Held 13 , in dissociated hippocampal cultures 23 , and our present study.

Previous studies in hippocampal neurons support an inhibitory role for the C2A domain of Syt 1 in exocytosis. The lack of an increase in spontaneous release in Syt 1 -null mutant embryonic synapses is likely a result of the known role of the protein in docking 33 , and the corresponding reduction in the readily releasable pool revealed by hypertonic sucrose application 9.

Consistent with this model, a reduction in synaptic vesicle docking has been observed by EM 23 , 33 and functionally demonstrated by loss of hypertonic-induced release 9 , 23 , 25 in Syt 1 -null mutants. Further studies will be required to define precise molecular interactions required for the function of each C2 domain during vesicle fusion.

The dual roles of the Syt 1 C2 domains is consistent with observations that synaptotagmins have universally evolved with both a C2A and C2B domain throughout the animal kingdom In summary, we conclude that the C2A domain of Syt 1 suppresses asynchronous release, whereas the C2B domain acts as a synchronous fusion trigger.

All transgenic strains were generated using standard microinjection into white - embryos. UAS transgenes were expressed using a GAL4 driver under control of the pan-neuronal elav promoter 21 on the third chromosome in the Syt 1 -null background. Null mutants lacking endogenous Syt 1 were generated by crossing Syt 1 N13 , an intragenic Syt 1 deficiency 7 , with Syt 1 AD4 , which truncates Syt 1 before the transmembrane domain 8.

These null alleles were recombined with a chromosome containing the muscle-specific myosin heavy chain Mhc null mutant, Mhc 1 , to inhibit muscle contraction and facilitate stable recordings as previously described The Mhc 1 mutant had no observed effect on synapse formation, neurotransmitter release, or postsynaptic glutamate receptor clustering 9 , Mutant chromosomes were placed over a CyO balancer containing actin-driven GFP to allow unambiguous identification of embryos with Syt 1 null and Mhc 1 backgrounds.

Embryos were aged 21 to 24 h after fertilization and recorded in HL3. The internal solution in patch pipettes contained: Motor nerves were positioned in a suction electrode at their site of emergence from the CNS for nerve stimulation. Before recording, embryos were treated for 1 min with 0. Hypertonic solution was puffed using positive pressure for 3 s.

Slow responses originating from electrically coupled muscle fibers were excluded in subsequent analysis in all genotypes. Statistical analysis was performed using Prism 5 software GraphPad. The variation of data between animals average of five animals was small compared with the larger variation in data from one animal.

Thus, results were combined and the number of events recorded shown as N. Immunostaining on filleted embryos was performed as previously described DSYT2 against Syt 1 22 was used at 1: We thank Chip Quinn and members of the Littleton and Yoshihara laboratories for helpful scientific discussions and Drs. Francis for critical reading. This article contains supporting information online at www.

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Topics which have been largely absent in text books, such as multiplexing, formatting and format synchronization, are also considered. Although PCM evolved as a communication technology, it has become an important technology in data recording.

In a sense, magnetic or optical media are just specialized communication media and the key technologies discussed in this book are just as important to recording applications as to communications. PCM codes used for magnetic recording applications are discussed along with traditional communication codes. The design, analysis and implementation of a PCM system requires knowledge of very specific techniques associated with detection, synchronization and coding.

The techniques have evolved from both ad hoc methods and complex theory. One of the goals of this book is to bridge the gap between theory and practice in the key techniques. Matched filters are not only discussed theoretically, but means for implementing them are also considered.

The same is true with symbol synchronization. Multiplexing Formatting and Encoding. Error Detection and Correction. Nyquist Signaling and Partial Response Coding. Matched Filters and Binary Symbols. Fundamentals of Digital Communication. Probability Random Processes and Noise. Among the classic examples of this phenomenon is that of induction motors and asynchronous motors. All induction motors are asynchronous motors. The asynchronous nature of induction-motor operation comes from the slip between the rotational speed of the stator field and somewhat slower speed of the rotor.

A more-specific explanation of how this slip arises gets into details of the motor internals. Most induction motors today contain a rotational element the rotor dubbed a squirrel cage. The cylindrical squirrel cage consists of heavy copper, aluminum, or brass bars set into grooves and connected at both ends by conductive rings that electrically short the bars together.

The solid core of the rotor is built with stacks of electrical steel laminations. The rotor contains fewer slots than the stator. The number of rotor slots must also be a nonintegral multiple of stator slots so as to prevent magnetic interlocking of rotor and stator teeth when the motor starts. It is also possible to find induction motors containing rotors made up of windings rather than a squirrel cage.

The point of this wound-rotor configuration is to provide a means of reducing the rotor current as the motor first begins to spin. This is generally accomplished by connecting each rotor winding to a resistor in series. The windings receive current through some kind of slip-ring arrangement. Once the rotor reaches final speed, the rotor poles get switched to a short circuit, thus becoming electrically the same as a squirrel cage rotor.

The stationary part of the motor windings is called the armature or the stator. The stator windings connect to the ac supply. Applying a voltage to the stator causes a current to flow in the stator windings. The current flow induces a magnetic field which affects the rotor, setting up voltage and current flow in the rotor elements.

A north pole in the stator induces a south pole in rotor. But the stator pole rotates as the ac voltage varies in amplitude and polarity. The induced pole attempts to follow the rotating stator pole. If the rotor exactly followed the moving stator pole, there would be no change in magnetic-field strength.

Thus, the rotor always lags behind the stator field rotation. The rotor field always lags behind the stator field by some amount so it rotates at a speed that is somewhat slower than that of the stator. The difference between the two is called the slip. The amount of slip can vary. It depends principally on the load the motor drives, but also is affected by the resistance of the rotor circuit and the strength of the field that the stator flux induces.

When ac is initially applied to the stator, the rotor is stationary. The voltage induced in the rotor has the same frequency as that of the stator. As the rotor starts spinning, the frequency of the voltage induced in it, f r , drops. Here s is expressed as a decimal. When the rotor is standing still, the rotor and stator effectively form a transformer.

So the voltage E induced in the rotor is given by the transformer equation. Thus, the voltage E r induced while the rotor spins depends on the slip:.

A synchronous motor has a special rotor construction that lets it rotate at the same speed — that is, in synchronization — with the stator field.

One example of a synchronous motor is the stepping motor, widely used in applications that involve position control. However, recent advances in power-control circuitry have given rise to synchronous-motor designs optimized for use in such higher power situations as fans, blowers, and to drive axles in off-road vehicles.

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