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For Peer Review Only Technique to Determine the Optimised Harmonic Switching Angles of a Cascaded Multilevel Inverter for Minimum Harmonic Distortion Journal: IETE Journal of Research Manuscript ID: TIJR-2015-1247 Manuscript Type: Original Article Date Submitted by the Author: 24-Aug-2015 Complete List of Authors: Sharma, Angshuman; Tezpur University, Electronics & Communication Engineering Dept. Bardalai, Aroop; Assam Engineering College, Electrical Engineering Keywords: Harmonic distortion , Inverters, Multilevel systems, Switching frequency Abstract: Multilevel inverters have received considerable attention from industries and researchers for its high power and voltage applications. Various switching techniques have been suggested for improving the quality and performance of inverters. One of the conventional techniques for implementing the switching algorithm in these inverters is Optimised Harmonic Stepped Waveform (OHSW). However, this technique involves the major problem of solving nonlinear and complex equations, which indicates a possibility of multiple solutions. This paper describes a novel technique that uses the simple arithmetic sequence of natural numbers to determine the optimised switching angles of a single phase cascaded multilevel inverter of any number of levels and fed by equal dc sources. The basic objective was to avoid the laborious process of solving the non- linear equations using complex switching algorithm for finding the optimal solution of the switching angles. This technique is implemented to calculate the optimised switching angles of a 9-level cascaded inverter that reduces the total harmonic distortion to below 9%. URL: https://mc.manuscriptcentral.com/tijr E-mail: [email protected] IETE Journal of Research

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Multilevel inverters have received considerable attention from industries and researchers for its high power and voltage applications. Various switching techniques have been suggested for improving the quality and performance of inverters. One of the conventional techniques for implementing the switching algorithm in these inverters is Optimised Harmonic Stepped Waveform (OHSW). However, this technique involves the major problem of solving nonlinear and complex equations, which indicates a possibility of multiple solutions. This paper describes a novel technique that uses the simple arithmetic sequence of natural numbers to determine the optimised switching angles of a single phase cascaded multilevel inverter of any number of levels and fed by equal dc sources. The basic objective was to avoid the laborious process of solving the non-linear equations using complex switching algorithm for finding the optimal solution of the switching angles. This technique is implemented to calculate the optimised switching angles of a 9-level cascaded inverter that reduces the total harmonic distortion to below 9%

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  • For Peer Review Only

    Technique to Determine the Optimised Harmonic Switching Angles of a Cascaded Multilevel Inverter for Minimum

    Harmonic Distortion

    Journal: IETE Journal of Research

    Manuscript ID: TIJR-2015-1247

    Manuscript Type: Original Article

    Date Submitted by the Author: 24-Aug-2015

    Complete List of Authors: Sharma, Angshuman; Tezpur University, Electronics & Communication Engineering Dept. Bardalai, Aroop; Assam Engineering College, Electrical Engineering

    Keywords: Harmonic distortion , Inverters, Multilevel systems, Switching frequency

    Abstract:

    Multilevel inverters have received considerable attention from industries and researchers for its high power and voltage applications. Various switching techniques have been suggested for improving the quality and

    performance of inverters. One of the conventional techniques for implementing the switching algorithm in these inverters is Optimised Harmonic Stepped Waveform (OHSW). However, this technique involves the major problem of solving nonlinear and complex equations, which indicates a possibility of multiple solutions. This paper describes a novel technique that uses the simple arithmetic sequence of natural numbers to determine the optimised switching angles of a single phase cascaded multilevel inverter of any number of levels and fed by equal dc sources. The basic objective was to avoid the laborious process of solving the non-linear equations using complex switching algorithm for finding the optimal solution of the switching angles. This technique is implemented to calculate the optimised switching angles of a 9-level cascaded inverter that reduces

    the total harmonic distortion to below 9%.

    URL: https://mc.manuscriptcentral.com/tijr E-mail: [email protected]

    IETE Journal of Research

  • For Peer Review Only

    Figure 1. Odd quarter wave symmetric 9-level cascaded inverter waveform.

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    Figure 2. Optimised harmonic stepped voltage waveform of a nine-level inverter. 153x79mm (96 x 96 DPI)

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    Figure 3. Column chart showing the amplitudes of the harmonic components of 9-level inverter. 174x120mm (96 x 96 DPI)

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    Figure 4. Column chart showing the comparison of the THD between the three multilevel inverters. 80x60mm (96 x 96 DPI)

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    1

    Technique to Determine the Optimised Harmonic

    Switching Angles of a Cascaded Multilevel Inverter

    for Minimum Harmonic Distortion

    Angshuman Sharma and AroopBardalai

    Angshuman Sharma was with Electrical Engineering Department, Assam Engineering College, Guwahati 781013, Assam, India. He is now with the

    Department of Electronics & Communication Engineering, Tezpur University, Tezpur - 784028, Assam, India (corresponding author, phone: 03712-273199; +91-9707475263, fax: 03712-267005; e-mail: [email protected]).

    AroopBardalai is with the Electrical Engineering Department, Assam Engineering College, Guwahati 781013, Assam, India. (e-mail:

    [email protected]).

    ABSTRACT

    Multilevel inverters have received considerable attention from industries and researchers for its high power and voltage

    applications. Various switching techniques have been suggested for improving the quality and performance of inverters. One

    of the conventional techniques for implementing the switching algorithm in these inverters is Optimised Harmonic Stepped

    Waveform (OHSW). However, this technique involves the major problem of solving nonlinear and complex equations,

    which indicates a possibility of multiple solutions. This paper describes a novel technique that uses the simple arithmetic

    sequence of natural numbers to determine the optimised switching angles of a single phase cascaded multilevel inverter of

    any number of levels and fed by equal dc sources. The basic objective was to avoid the laborious process of solving the non-

    linear equations using complex switching algorithm for finding the optimal solution of the switching angles. This technique

    is implemented to calculate the optimised switching angles of a 9-level cascaded inverter that reduces the total harmonic

    distortion to below 9%.

    Keywords:

    Arithmetic sequence; multilevel inverter; natural number, optimised harmonic stepped waveform; switching angles; total harmonic

    distortion.

    1. INTRODUCTION

    The concept of multilevel inverters has revolutionised

    inverter technology. A multilevel voltage source inverter

    divides the main dc supply voltage into several smaller dc

    sources which are used to synthesise an ac voltage into a

    staircase or stepped approximation of the desired sinusoidal

    waveform [1]. Among the significant advantages of

    multilevel configuration is the harmonic reduction in the

    output voltage waveform without increasing switching

    frequency or decreasing the inverter power output [2-4]. The

    so-called multilevel starts from three levels. The multilevel

    inverter topology can overcome many limitations of the

    standard bipolar inverter. Output voltage and power increase

    with number of levels. Increasing the output voltage does

    not require an increase in the voltage rating of individual

    force commutated devices. If the multilevel inverter output

    increases to infinite level, the harmonic content of the output

    voltage is reduced to zero [5]. But for increasing voltage

    levels, the number of switches also will increase in number.

    Hence the voltage stresses and switching losses will also

    increase [6]. So the number of achievable voltage levels is

    limited by voltage unbalance problem, voltage clamping

    requirement, circuit layout, and packaging constraints [7].

    The multilevel inverter can yield operating characteristics

    such as high voltage, high power level and high efficiency

    without the use of transformers [2,8]. It is recently applied

    in static synchronous compensators, active filters, reactive

    power compensation applications [9], photovoltaic power

    conversion, uninterruptible power supplies and magnetic

    resonance imaging. Furthermore, one of the growing

    applications for multilevel inverter is electric and hybrid

    motor drives.

    The multilevel inverters are mainly classified as Diode

    Clamped [4,10], Flying Capacitor [11] and Cascaded H-

    bridge multilevel inverter with separate dc sources

    (SDCSs)[2,12-14].The cascaded multilevel inverter was first

    proposed in 1975 [1`3]. The cascaded multilevel inverter is

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    2

    made of several H-bridge inverters, each powered by a

    separate dc source which may be obtained from batteries,

    fuel cells, or solar cells. It synthesises a desired voltage from

    several independent DC voltage sources, such that the

    synthesised voltage waveform corresponds to the sum of the

    inverter outputs. Since this topology consist of series power

    conversion cells, the voltage and power level may be easily

    scaled. The cascaded inverter control method is easier to

    implement when compared to other multilevel inverters due

    to circuit layout flexibility, absence of transformer, extra

    clamping diode or voltage balancing capacitor [15], and

    easy adjustment of the number of output voltage levels by

    adding or reducing H-bridge cells [16]. This configuration

    has recently become very popular in ac power supplies and

    adjustable speed drive applications [1,12,13].

    An important key in designing an effective and efficient

    multilevel inverter is to ensure that the total harmonic

    distortion (THD) in the output voltage waveform is small

    enough [17,18]. With more voltage levels, the multilevel

    waveform becomes smoother with low harmonic content,

    but with many levels, the design becomes more complicated

    with more components and a more complicated controller

    for the inverter is required [19]. Power electronics

    researchers have suggested several switching strategies,

    such as sinusoidal or sub-harmonic natural pulse width

    modulation (SPWM) [20,21], selective harmonic-eliminated

    pulse width modulation (SHE PWM) [20,22], space-vector

    modulation (SVM) [23,24], optimised harmonic-stepped

    waveform (OHSW) [3,10-12], and optimal minimisation of

    THD (OMTHD) [25], to eliminate or minimise the harmonic

    content in multilevel waveforms comprising a specific

    number of levels.

    The OHSW technique is very suitable for a multilevel

    inverter circuit [26].In this method, the goal is to conduct

    potential elimination of low order harmonics; when this goal

    cannot be achieved, the highest possible harmonics

    optimisation is desired [16]. The challenge associated with

    such techniques is to obtain the optimised harmonic

    switching angles through analytical solutions of non-linear

    transcendental equations that contain trigonometric terms

    which naturally exhibit multiple sets of solutions. Attention

    has previously been focused on using the numerical iterative

    methods and the evolutionary search algorithms for solution

    of the non-linear complex equations. However, each of them

    has their own advantages and disadvantages.

    In this paper, the optimums witching angles for a

    cascaded multilevel inverter are determined using a simple,

    fast, efficient and reliable technique that does not require to

    solve the complex non-linear equations at all, in order to

    achieve minimum harmonic distortion of the output voltage

    waveform. The method focuses on quarter wave symmetric

    multilevel inverter waveform having equal step height, i.e.

    fed by equal dc sources. It uses the arithmetic sequence of

    natural numbers to determine the step spaces and henceforth

    the switching angles of the cascaded multilevel inverter.

    This technique involves simpler formulation and can be

    used with multilevel inverters having any odd number of

    levels. A 9-level cascaded inverter is considered in this

    paper for analysis and the optimised harmonic switching

    angles are calculated.

    2. OPTIMISED HARMONIC STEPPED WAVEFORM TECHNIQUE (OHSW)

    A general odd quarter wave symmetric 9-level cascaded

    inverter waveform is represented in Figure 1. To achieve the

    9-level waveform, four separate dc sources are required. V1

    to V4 are dc voltage supplies from separated dc sources.

    Figure 1. Odd quarter wave symmetric 9-level cascaded

    inverter waveform.

    Considering equal amplitude of all dc sources, i.e.,

    V1=V2=V3=V4=E, the expression of the amplitude of the

    fundamental and harmonic components of the waveform are

    given as:

    Hn() = foroddn0forevenn (1)

    Hence the Fourier series of the output voltage waveform

    is given as:

    Vout() = (2) where

    E dc voltage supply;

    n odd harmonic order;

    s number of dc sources; optimised harmonic switching angle, which must satisfy the condition:, !, ", # !

    For determining the Fourier series of the 9-level output

    voltage waveform, four switching angles,, !, ", , need to be known. Mathematically, four equations are required to

    be set up to solve these switching angles. Unfortunately,

    these equations are nonlinear as well as transcendental in

    nature, which indicates a possibility of multiple solutions.

    Moreover, the estimated solutions must be less than /2.

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    3

    Several methods have been suggested for solving these

    equations which can be broadly categorised into two sets.

    The first group attempts to solve these equations using the

    Newton-Raphson (N-R) iterative method [27]. Iterative

    methods mainly depend on an initial guess. Moreover,

    divergence problems are likely to occur, especially when the

    number of inverter levels is more [28]. Although the N-R

    method is conveniently fast, it can only find one set of

    solutions. Chiassonet. al. [29] derived analytical expressions

    using the mathematical Resultant Theory to compute the

    optimum switching angles with the exact range of

    modulation index (M). These expressions were polynomials

    of 22nd

    degree which were difficult and time consuming to

    derive, and for any change of levels or voltage inputs, new

    expressions were required [30]. Homotopy algorithm is

    another approach applied to determine one set of solutions

    [31]. Overall, all methods included in the first group do not

    suggest any optimum solutions for a particular M.

    The second group finds solutions that deal with

    eliminating the lower order harmonics completely. In this

    case, all evolutionary search algorithms can be regarded as

    suitable choices. These approaches are applicable for

    problems that deal with any number of levels, with simple

    derivation of analytical expressions. But these approaches

    involve extensive computing [10,16,28,32,33] and are not as

    fast as the first group of methods.

    One of the major problems in electric power quality is the

    harmonic contents. There are several methods of indicating

    the quantity of harmonic contents. The most widely used

    measure is the total harmonic distortion (THD) [3]. The

    THD evaluates the extent of harmonic contents in the output

    waveform [7]. THD is mathematically given by,

    THD = $ %&'(&)'

    %* (3) where H1is the amplitudes of the fundamental component,

    whose frequency is 0 and H(n) is the amplitude of the nth

    harmonic at frequency n0.

    Substituting H1 and H(n) in the above equation, we have

    THD = $ +*& ,-./010)* 2

    '(&)' ,-./010)* (4)

    Therefore, output voltage THD of the presented waveform

    can be calculated. Theoretically, to get exact THD, infinite

    harmonics need to be calculated. However, practically, it is

    not possible. Therefore, certain number of harmonics is

    calculated. It relies on how precise the THD is needed.

    3. PROPOSED TECHNIQUE

    The technique that has been developed for the

    determination of step spaces is based on the simple

    Arithmetic Sequence of Natural Numbers, which is 1, 2, 3,

    4,, n. If time is considered as the reference, then for

    the 1st positive quarter wave, this technique assigns 1 unit of

    time for the 1st step space, 2 units of time for the 2

    nd step

    space, 3 units of time for the 3rd

    step space and so on till the

    last step space is completed at /2. Since the 9-levelwaveform of Figure 1 is considered to be

    quarter-wave symmetric, so Fourier analysis of the first

    quarter wave from 0 to /2 is sufficient to compute the

    amplitude of the fundamental and odd harmonic components

    of the complete waveform. There are five steps in the 1st

    quarter wave of the waveform, which indicates that there are

    4 H-bridge cells in the 9-level cascaded inverter. Following

    this technique, the step spaces can be assigned as follows: 1st

    step space is assigned 1 unit of time, 2nd

    step space is

    assigned 2 units of time, 3rd

    step space is assigned 3 units of

    time, 4th

    step space is assigned 4 units of time, and the 5th

    and final step space of the 1st quarter wave is assigned 5

    units of time.

    The procedure can be further described as follows. Let t1,

    t2, t3, t4 are the switching instants of the four H-bridge cells

    of the cascaded 9-level inverter. Initially, all the H-bridge

    cells are in the OFF state and will continue to be in the OFF

    state for 1 unit of time till t1 is reached. At the instant t1, the

    1st H-bridge cell is switched ON. The 2

    nd H-bridge cell is

    switched ON after 2 units of time at the instant t2. Now both

    the 1st and the 2

    nd H-bridge cells are in the ON state for the

    next 3 units of time till the instant t3 is reached. At the

    instant t3, the 3rd

    H-bridge cell is switched ON and the 1st,

    2nd

    and 3rd

    H-bridge cells operate simultaneously for the

    next 4 units of time till the instant t4 is reached. At the

    instant t4, the 4th

    and the last H-bridge cell is switched ON.

    Now all the four H-bridge cells operate simultaneously

    for the next 5 units of time when finally /2 is reached and

    the first quarter wave is accomplished. Total number of units assigned for all the step spaces of the 1

    st quarter wave = 1 + 2 + 3 + 4 + 5 = 15

    For the waveform of Figure 1, let the frequency be 50Hz,

    so that the time period of the complete wave is,

    T = 1/50 second = 0.02 second.

    Time for half wave = 0.01 second. Time for quarter wave = 0.005 second. Let tbe the time for each unit. Since there are total 15

    units assigned in the 1st quarter wave which has a time

    period of 0.005 seconds, therefore, we can write,

    15t = 0.005 second

    t = 5.5566 s

    t = 0.000333 s

    1st step space, t1 = t = 0.000333 s 2

    nd step space, t2 = 2t = 0.000667 s

    3rd

    step space, t3= 3t = 0.000999 s 4

    th step space, t4 = 4t = 0.001333 s

    5th

    step space, t5 = 5t = 0.001667 s Then,

    t1 = 0 + t1 = 0.000333 s t2 = t1 + t2 = 0.001 s

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    4

    t3 = t2 + t3 = 0.002 s t4 = t3 + t4 = 0.003333 s Thus the 4

    thH-bridge cell is switched on at instant t4 =

    0.003333 s and is operated for t5 = 0.001667 s when the 1st quarter wave is completed at 0.005 s.

    Since we know, angle = t = !8 9 = !5.5! 9 0.000333, ! = !5.5! 9 0.001, " = !5.5! 9 0.002, = !5.5! 9 0.003333 Thus the optimised harmonic switching angles of the four

    H-bridge cells in the first quarter wave are

    = 0.0333, ! = 0.1, "= 0.2, = 0.3333 in radian

    or, = 6,! = 18, "= 36, = 60 in degrees These switching angles were used to generate the

    optimised harmonic stepped voltage waveform of the nine-

    level inverter operating at 50 Hz frequency and fed by four

    equal dc sources of magnitude E each, so as to maintain

    equal step height. The waveform is depicted in Figure 2,

    where 1,2,3,4 and 5 indicate the 1st, 2

    nd, 3

    rd, 4

    th and 5

    th step

    space respectively.

    4. RESULTS AND DISCUSSION

    Let the 9-level cascaded inverter, shown in Figure 2, be

    fed by four identical dc sources of 100V each. The output

    voltage waveform is controlled by four switching angles, !, "and. Performing Fourier analysis, the amplitude of the fundamental and odd harmonic components and the

    Total Harmonic Distortion (THD) can be easily calculated.

    Using the nonlinear equation system (1) and the optimised

    harmonic switching angles, , !, "and, obtained in the previous section, the amplitude of the fundamental

    component, H1 is calculated and is found to be 414.40 V.

    The same equation system also allows us to calculate the

    amplitudes of the odd harmonic components. The Column

    chart of Figure 3 shows the amplitudes of the fundamental

    and odd harmonic components up to the 63rd

    harmonic.

    Results show that the proposed technique does not eliminate

    the harmonics, but minimises it satisfactorily. Further, the

    amplitude of each odd harmonic component is reduced

    below 4.1% of the amplitude of the fundamental component

    for the 9-level inverter. By substituting the amplitudes of the

    harmonic components in (4), the output voltage THD,

    calculated up to63rd

    harmonic, is found to be 8.99%.

    This technique has also been applied to determine the

    optimised harmonic switching angles of 11-level and 13-

    level cascaded inverters and study their respective harmonic

    distribution. Assuming identical operating conditions, it is

    found that the amplitude of the fundamental component and

    the THD are 514.41V and 8.14% respectively in case of 11-

    level cascaded inverter and 614.20V and 7.99% respectively

    in case of 13-level cascaded inverter. Studying the results

    obtained for the 9-level, 11-level and 13-level cascaded

    inverters, it is observed that the output voltage of the

    inverters increase as the number of levels increase while

    their THD decrease with higher number of levels. This can

    be seen from the column chart of Figure 4 which compares

    the output voltage THD of the 9-level, 11-level and 13-level

    cascaded inverters.

    Figure 2. Optimised harmonic stepped voltage waveform of a nine-level inverter.

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    5

    Figure 3.Column chart showing the amplitudes of the harmonic components of9-level inverter.

    Figure 4.Column chart showing the comparison of the THD between

    the three multilevel inverters

    5. CONCLUSION

    The goal of this technique was to calculate the optimised

    harmonic switching angles for which the multilevel

    waveform exhibits minimum harmonic distortion. The idea

    was to avoid the tedious process of solving non-linear and

    complex equations to find the optimised harmonic switching

    angles. A fast, efficient and reliable

    mathematicaltechnique,involving simpler calculations, was

    presented to determine the switching angles of a cascaded

    multilevel inverter without extensive derivation of analytical

    expressions.The proposed technique includes the Arithmetic

    Sequence of natural numbers to assignthe step spaces and

    henceforth to determine the optimised harmonic switching

    angles of the cascaded multilevel inverter having any odd

    number of levels. The technique holds good for multilevel

    inverters having quarter wave symmetric waveform and fed

    by equal dc sources. As an example, it was used to solve the

    switching angles of a nine-level cascaded inverter and the

    output voltage THD was found to be 8.99%. Results show

    that the proposed technique does not eliminate the

    harmonics, but minimises it satisfactorily. Further, this

    technique has also been applied to 11-level and 13-level

    cascaded inverters and their output voltage THDs are found

    to be 8.14% and 7.99% respectively, which indicates that

    the THD decrease with higher number of levels.

    REFERENCES

    1. Tim Cunnyngham, Cascade Multilevel Inverters for

    Large Hybrid-Electric Vehicle Applications with

    Variant DC Sources, M.S. Thesis, Dept. Elect. Eng.,

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    0

    50

    100

    150

    200

    250

    300

    350

    400

    450

    1 3 5 7 9 1 1 1 3 1 5 1 7 1 9 2 1 2 3 2 5 2 7 2 9 3 1 3 3 3 5 3 7 3 9 4 1 4 3 4 5 4 7 4 9 5 1 5 3 5 5 5 7 5 9 6 1 6 3

    Vo

    lta

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    pli

    tud

    e

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    7.4

    7.6

    7.8

    8

    8.2

    8.4

    8.6

    8.8

    9

    9.2

    9-level 11-level 13-level

    TH

    D

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    6

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    95, Jan. 2008.

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    May 2009.

    Angshuman Sharma was born in

    Assam, India in 1989. He received his

    B.E. degree in Electrical Engineering

    from Jorhat Engineering College

    (JEC), Jorhat, Assam, India in 2012,

    and his M.E. degree in Power Systems

    from Assam Engineering College

    (AEC), Guwahati, Assam, India in 2014. Soon thereafter, he

    joined Tezpur University, Tezpur, Assam, India and is

    presently working as an Assistant Professor in Electrical

    Engineering in the Dept. of ECE. His current research

    interests include multilevel inverters, analysis and control of

    power electronics devices, application of power electronics

    in power system, solid state transformers and robotics.

    AroopBardalai received his B.E.

    degree in Electrical Engineering from

    Assam Engineering College (AEC),

    Guwahati, Assam, India in 1984. After

    a brief period in BRPL as an executive

    trainee, he joined AEC in 1985 as a

    Lecturer in Electrical Engineering

    Department. Subsequently he obtained Masters degree from

    Indian Institute of Science, Bangalore, India in 1988 and

    was awarded PhD from Gauhati University, Guwahati,

    Assam, India in 2008. He is presently working as an

    Associate Professor in the Department of Electrical

    Engineering, AEC. During his long academic career, apart

    from offering various courses and laboratories, he has

    guided numerous projects of practical importance for under

    graduate and graduate students. He has also been

    instrumental in developing laboratories in the Department,

    steering the examination process for a long time, and

    involved in hostel administration. He has been an active

    member of the Institution of Engineers (India), Assam State

    Centre.

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