gravitational collapse in saiph (kappa orionis) star

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    GRAVITATIONAL COLLAPSE IN SAIPH STAR (ORION

    KAPPA): A NOVEL THEORY

    A.B.RAJIBHAZARIKA

    DEPT. OFMATHEMATICS

    DIPHU GOVT. COLLEGE, DIPHU

    KARBI ANGLONG, ASSAM (INDIA)

    PIN-782462

    E-mail:

    [email protected]

    [email protected]

    [email protected]

    [email protected]

    [email protected]

    ABSTRACT

    The present study is done theoretically to get the gravitational collapse phenomena

    and a search for new concept towards the insight into the behavior of Double trios, Saiph

    star(Orion Kappa) which are symmetrical set of six stars (globs) of the luminosityintensity of 50-52 magnitude found in concurrent doubles at Aldebaran and Betelgeuse

    galaxies where the Saiph stars illuminates with such magnitude .This theory is novel

    approach towards providing certain new results such as fusion process in the double triosstars , confinement time calculated as there are at present no such theory existing.

    Key words: self- gravitating system, transport phenomena, collision, diffusion, skindepth, and space plasma physics, stellar clusters and association, early type stars (O andB),Orion population, binary and multiple stars, supernovae remnants in external galaxies.

    PACS No: 4.40-b, 5.60Cd, 5.60-k, 5.60+w, 5.60-a, 82.56Lz, 94.05-a, 97.20Ec, 97.21+a,98.20-d, 97.80-d, 98.58Mj

    INTRODUCTION

    Bhatia and Hazarika (1995,1996) did some work on gravitational instability using theviscosity term showing influence on the gravitational collapse ,in the later paper the two

    superposed fluid(plasma) flow past each other in horizontal magnetic field with rotation

    and viscosity playing vital role for the collapse rotating neutrons stars Schwarzchildradius is derived. Jeans instability leading to gravitational collapse of stars is studied

    mailto:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]
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    earlier by many authors Jeans (1902), Chandrasekhar (1981), El-Sayed and Mohamed

    (2011) tried to prove the gravitational collapse with finite conductivity playing crucial

    role.

    PRESENT WORKBased on low beta plasma having low frequency fluctuation which is being stabilized by

    skin depth, current diffusivity and with other parameters. The induced gravitational

    instability by above mentioned parameters and as a whole the classical transportphenomenon is taken into consideration. The heat conduction term is calculated ,Banana

    regime (Bootstrap) , ware effect is calculated where an important result Hazarikas

    regime for Saiph star (Kappa orionis) which is R(1+4 -sin3 sin -2sin -2sin ) times of solar radius is found to be correct as 10.8503(approx. 11 ),with right ascession

    (RA) of 05h 47m 45.4s(72.79594 degrees) and declination of -09deg 40m 11sec(-

    9.669723 deg). The above facts compels one to study the phenomena of gravitational

    collapse and thereby the suppression by different parameters.

    Hazarikas constant for Saiph star (Kappa Orionis) is

    1. sin2sin2sin3sin41 +++=hC =10.8503

    BASIC EQUATION

    h

    h

    h

    h

    E RC

    FRCp

    RC

    FpRCR

    eNE

    2

    )(

    2

    1 22 +==

    ..(1)

    [ ]

    =

    22

    222

    2

    h

    th

    t

    i

    CR

    BCR

    B

    ..(2)

    eeee nq

    d t

    d Tn+ =

    2

    3..(3)

    ( )

    2

    s i n22

    )s i n22(

    122

    22

    t

    e

    BR

    R

    q

    +

    +

    = X{

    +

    +22 )sin22(

    1)sin22(

    RR } ..(4)

    ( )

    +=

    iie

    i pen

    EB

    Bv .

    12

    ..(5)

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    GENERAL MHD MODEL :

    [ ] =

    +

    2

    0

    2

    0

    0 ,B

    c

    tB

    cmn i

    ( ) zGnmzmGnBcnm

    RzrpXj

    cB ii .1..cos2 00

    0

    4

    0

    0

    0 ++++

    (6)

    jjtc

    A 2

    +=

    ..(7)

    [ ] ppB

    c

    t

    p 2

    0

    , =+

    (8)

    where Ac

    j 2

    4=

    , [ ] BAXzBA = ., ,Poissons bracket

    Eigen mode equation is obtained by linearizing the eqn.(6)-(8) in toroidal coordinates(r,, )for RTI as

    ( ) ( )( ) ( ) +++=

    = 0

    1

    0 s i n2e x p2),,( qi nrri n qlrqi nlr m n

    l

    ..

    (9)The eigen value equation reduces to a differential equation

    ( ) 0)(

    1 222

    2

    2

    2

    =+

    ++

    sC

    s

    d

    dh ..

    (10)

    ( )2222

    )(

    1

    sCs

    G

    h +

    +

    =

    ... (11)

    On further solving eqn.(11) we get the growth as follows

    ( )

    2/1

    22222

    1

    +

    +

    =

    s

    C

    ss

    G h .. (12)

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    where

    ( )

    [ ]

    ( )

    ( )

    [ ]( )

    ( )

    ( )

    sin2sin2sin3sin41,

    ln

    ,ln

    ,,4

    ,,ln

    ,,

    12

    4

    3

    ,4,ln

    ,8

    ,,sin22

    ,,,

    2

    01

    012

    04

    2

    2

    02

    0

    05

    1

    5

    45

    4

    5

    35

    4

    02

    0

    2

    02

    2

    0

    02

    222222244

    +=

    =

    =

    ====

    ==+

    +

    ===

    ===+

    ====

    R

    cg

    dr

    ndLn

    dr

    pdLp

    Ln

    rnn

    r

    c

    rB

    c

    gLngLnrmn

    BrAAtt

    ls

    aB

    rmngLngLnrmn

    B

    ppqn

    R

    rqnqnqn

    s

    mn

    mnmn

    pa

    mn

    pa

    mni

    pa

    mnpa

    mni

    pa

    mni

    pa

    pa

    DISCUSSION

    The growth rate as a function of finite conductivity we can find the first order derivative

    to find that the function increases or decreases as :

    ( ){ }

    ( ){ }

    0

    12

    2

    1

    2222

    12

    22

    1222

    22

    =

    +

    +

    +

    +

    =

    sC

    s

    s

    ssC

    s

    Gd

    d

    h

    h

    .(13)

    as the above term is positive we can say that it decreases or the function stabilizes.

    If the above term goes to 0 it gives us the root of the equation .i.e.,either the collapsing

    growth rate of Saiph(Kappa Orion) is

    ( )2/1

    222/12/1

    2

    ++=

    ss

    CGh

    Here we see that the function which is dependent on current diffusivity and skin depth ispositive i.e.,stabilizes the growth rate of star .if current diffusivity is more than 1000 the

    potential collapses,similarly the skin depth values (1-10) shows the collapse of the

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    potential of Kappa Orion(Saiph).It stabilizes for >1 always for if

    and s remain constant, roots lies between 30 and 40.If we plot growth against the current

    diffusivity and skin depth we can see the implosion and collapse of potential.

    Gravitational red shift

    For mass of the star including in the stellar spectra with those in spectra obtained in thelaboratory,the ratio M/R is too small for a gravitational redshift to be apparent. A white

    dwarf is an old star whose interior consists of atoms whose electron structure have

    collapsed and so it is very small

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    Rc

    GMsaiph

    =

    2

    12

    Rc

    GMsaiphwith this condition no photons can even leave the star as it cannot radiate

    i.e,a black hole.

    111

    152

    Rc

    GMsun

    Schwarzchilds radius of Saiph star(Kappa Orionis)

    2215

    2

    c

    GM

    c

    GMR sun

    saiph

    s ==

    ss RR 15=

    Schwarzchilds radius of Saiph star (Kappa Orionis) is 15 times the Schwazchilds radiusof sun.

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    REFERENCES

    1.Bhatia P.K and Hazarika,A.B.Rajib: Physica Scripta 52,775(1995)

    2.Bhatia,P.K and Hazarika,A.B.Rajib: Physica Scripta 53,57(1996)3.Jeans,J.H:Philosiphical transactions of Royal society of LondonA 199,1-53 (1902)

    4.El-Sayed,M.F and Mohamed,R.A:ISRN Mechanical Engineering,Vol.2011,Art. ID

    597172 (2011)5.Chandrasekhar,S:Hydrodynamic and hydromagnetic stability,Dover pub.,NY(1981)

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