Phasing

Physics articles and information
RSS icon Home icon
  • Power - formulas and an explanation

    Posted on February 8th, 2010 admin No comments

    Short and sweet presentation on power.

    Click here to see

    Cant access the above link ? Download from here !

  • The world’s most precise clock

    Posted on February 8th, 2010 admin No comments

    Physicists have just built an enhanced version of an experimental atomic clock based on a single aluminum atom that is now the world’s most precise clock, more than twice as precise as the previous pacesetter based on a mercury atom.

    The new aluminum clock would neither gain nor lose one second in about 3.7 billion years! WOW! Read more here or here.

  • Copernicus and Heliocentrism

    Posted on February 8th, 2010 admin No comments

    Sky, the most fascinating thing which keeps human kind occupied for centuries. To talk about Helioce

  • What matters

    Posted on February 8th, 2010 admin No comments
    It's dead letter week on Foolish Notions, just because. Here's no. 1:

    Sir,

    According to the Law of Conservation of Matter, every atom is continually recycled in the universe and never lost. In other words, we breathe the same atoms as those breathed by Galileo (approx 4.3 x 109 atoms per breath). Similarly, we drink – in every glass of water – some atoms of Adolph Hitler’s urine, while, on a lighter note, we also drink some atoms of Jennifer Lopez’s body fluids (provided they have had sufficient time to disperse). Conversely, Jennifer Lopez is drinking – in every glass of water she swallows – some of my body fluids. I would, therefore, like to ask Jennifer (if, indeed, she is prone to brush over this esteemed organ) if she would like to try the undiluted variety … purely for the purposes of scientific investigation. Of course.

    Yours

    R.H. Schmitt

  • chi2cdf

    Posted on February 8th, 2010 admin No comments

    If you’re a luddite like me (all my analysis code these days is written in octave-2.1.73 and octave-3.0 (better octave-forge support)) and you have a propensity o,  you may have encountered this error:

    </code>
    
    octave:1> chi2cdf(4000,4000)
     ***MESSAGE FROM ROUTINE D9LGIT IN LIBRARY SLATEC.
     ***FATAL ERROR, PROG ABORTED, TRACEBACK REQUESTED
     *  NO CONVERGENCE IN 200 TERMS OF CONTINUED FRACTION
     *  ERROR NUMBER = 3
     *
     ***END OF MESSAGE
    
     ***JOB ABORT DUE TO FATAL ERROR.
    0          ERROR MESSAGE SUMMARY
     LIBRARY    SUBROUTINE MESSAGE START             NERR     LEVEL     COUNT
     SLATEC     D9LGIT     NO CONVERGENCE IN 20         3         2         2
    
    error: exception encountered in Fortran subroutine xgammainc_
    error: evaluating assignment expression near line 54, column 15
    error: evaluating if command near line 53, column 5
    error: evaluating if command near line 52, column 3
    error: called from `gamcdf' in file `/usr/share/octave/3.0.1/m/statistics/distributions/gamcdf.m'
    error: evaluating assignment expression near line 42, column 7
    error: called from `chi2cdf' in file `/usr/share/octave/3.0.1/m/statistics/distributions/chi2cdf.m'
    
    <code>

    This is related (as above) to the library D9LGIT. Certainly in my case, and probably in general, there is another way to solve the problem. The gamma functions that underpin all of it will probably have nice asymptotics in any regime that triggers the error.  There’s scuttlebutt that this problem is better handled by the GSL library with hooks to Octave – it may be implemented “upstream” in the current Octave 3.2.

    In the case of

    chi2cdf

    , for k sufficiently large (look here to determine “large” for yourself),

    chi2cdf(x,k) and normcdf(x,k,sqrt(2*k))

    will generate essentially equivalent results. The absence of  incomplete gamma functions in

    normcdf

    make it more general (and inapplicable for small k).

  • …what

    Posted on February 8th, 2010 admin No comments

    (Recital was OK. Finished one more application problem. Everything else that happened since the last update is trivial.)

    I failed a practice AMC 12 (2007 B); I could only answer 1-12 and 23 (and got them all right, but that’s still not AIME qualification). (I also failed 2007 A because I remembered Vieta incorrectly and didn’t notice that 3 = 1 x 3.)

    I’m also failing at electricity (well, potential/capacitance and currents).

    Why am I becoming (more) stupid? >_<

    We have an Algebra 2 quiz tomorrow, and I have the feeling I’m going to get 11.5/12 again. I’ll just have to check more. After that, I’ll ask Mr Mallon about not taking precalculus at MSJ, instead taking AP Stats and AoPS Precalculus and possibly AoPS Calculus. (Maybe Spivak’s Calculus. I’m not sure yet.)

    I also hear on AoPS that USPhO (F=ma) results come back tomorrow. Apparently the cutoff was 13.75 last year, and will probably be lower this year. I answered 15 (and would have gotten one more correct if I didn’t solve that one right before we had to put our pencils down). Maybe I’ll make it. Who knows?

  • Science & Soul: Book Review: Born to Run: A Hidden Tribe, Superathletes, and the Greatest Race the World Has Never Seen

    Posted on February 8th, 2010 admin No comments

    Author and journalist Christopher McDougall begins his journey with one simple question: “Why do my feet hurt?”  McDougall was an avid runner whose running days seemed to be ending due to acute foot pain.  Cushioned shoes and orthotics did not seem to help.  Running is simply bad for you, claimed most sport doctors.  But then, McDougall stumbled across the story of the Tarahumara, or, in their own language, Raramuri, which directly translates to “running people.”  These indigenous people from the Copper Canyon region of Mexico, an area known for its harsh beauty (Copper Canyon is the deepest canyon in the world).  They hunt their prey by exhaustion: they chase their prey for several miles to tire it out and then can catch it and kill it.  Also, they competed in one of the most difficult ultra-marathons (100 miles plus at a time) in the world and shattered the world record.  Then, disenfranchised by the modern world, disappeared back into the canyons.  Not only are the Tarahumara excellent runners, they are also known for serenity, and peaceful, good-hearted nature. Oh yeah, and the winner was 50 years old and ran in tire-soled sandals. ” So why, if these guys can do all this into their fifties, why can’t I run 3 miles,” McDougall asks.  The answer, he finds, is in the shoes, or lack thereof.  We evolved to run great distances in our bare feet, not oddly shaped shoes (I’ll post about the science of barefoot running one of these days).

    Born

    Born to Run

    He then embarks on a quest to find and learn from the mysterious Raramuri the way to run.  To do so, he must evade dangerous Mexican drug cartels,  deal with outrageous long-distance runners, and find the elusive tribe itself!  The result is Born to Run: A Hidden Tribe, Superathletes, and the Greatest Race the World Has Never Seen. This book is part adventure, part running guide, part history, and part science.  I enjoyed this book so much that I polished off this book in a single night.  Without a doubt, this is the most fun book I have read in a long time.

    Grade: A

  • Pengujian sederhana untuk BDS Program

    Posted on February 8th, 2010 admin No comments
    Pengujian sederhana terhadap program simulasi dinamis brownian yang telah dibuat ini bertujuan untuk menguji jalannya program dalam menghitung besaran-besaran fisika yang diinginkan, yaitu posisi dan kecepatan partikel Brownian serta energi sebagai fungsi waktu. Program BDS yang telah dibuat memanfaatkan sistem Lennard-Jonnes Fluid (gas mulia), dengan alasan demi kemudahan dalam menganalisis hasil yang telah diperoleh. Satuan yang digunakan adalah LJ units, yang mana memberikan beberapa definisi satuan untuk energi, panjang, dan massa sebagai berikut: satuan energi = EPS; satuan panjang = SIGMA; satuan massa = massa partikel (= 1). Besaran turunan yang lain adalah volume dari sel satuan fcc cubic = a**3, volume per atom = a**3/4, kerapatan (densitas) = 4/a**3.
    Langkah-langkah yang saya lakukan untuk menguji dan memastikan jalannya program BDS adalah sebagai berikut.
    1. Menentukan kerapatan dari kisi fcc (dengan parameter kisi = a) sama dengan SQRT(2)*r0, di mana r0 = 2**(1/6) berkaitan dengan jarak equilibrium pada sumur potensial LJ untuk energi = 1_EPS, dan jarak potensial cutoff antara partikel-partikel tetangga terdekat di dalam kisi fcc: rcut = 1.2 SIGMA. Dari sini, saya dapat menentukan besarnya kerapatan (scaled density) dalam satuan SIGMA**3. Untuk sistem riil, nilai potential cutoff adalah rcut = 2.5 SIGMA.
    2. Memeriksa apakah posisi dan kecepatan yang dihasilkan telah sesuai dengan skala yang ditentukan dalam teori. Saya perlu mengamati bahwa besarnya orde posisi setiap atom tidak lebih besar dari orde parameter kisi fcc yang digunkan. Selain itu, saya menerapkan order parameter calculation untuk kisi fcc agar memperoleh hasil harga mutlak Sk = 1.
    3. Mengatur jumlah partikel dalam kisi fcc sebanyak 256 atom, dan potential cutoff 2.5 SIGMA. Ada empat sel satuan dalam setiap arah koordinat Kartesian. Simulasi dijalankan dengan time step 0.001 sampai 0.004. Sistem yang disimulasikan harus tetap berada dalam “constant total energy surface.” Nilai energi total ditentukan dari nilai kecepatan mula-mula (energi kinetik). Menampilkan hasil perhitungan energi total sebagai fungsi time step dan membuat plot.
    Tiga langkah di atas dapat digunakan untuk menguji keberhasilan program simulasi yang telah saya buat. Langkah-langkah ini telah sering dilakukan oleh para pemogram simulasi dinamis molekuler dengan sistem LJ Fluid. Saya cukup yakin dengan pengujian sederhana semacam ini.

    04.gifdionisius montja

    testingMD.pdf

  • Graphene

    Posted on February 8th, 2010 admin No comments

    definition of graphene

  • NEMD

    Posted on February 8th, 2010 admin No comments
    Pukul 08.44 pagi ini, saya menemukan sebuah artikel yang memuat informasi tentang simulasi dinamis molekuler non-equilibirum (sebuah jenis lain simulasi dinamis molekuler yang telah banyak dipakai untuk mempelajari model dinamis partikel-partikel mikiroskopis):
    Sumber: http://www.swinburne.edu.au/ict/research/cms/documents/publications/jcpV115Yr2001b.pdf
    Judul : On the relationship between tow body and three body interactions from nonequilibrium molecular dynamics simulation.pdf
    Dari artikel ini, saya memperoleh informasi tentang penggunaan satuan-satuan “tereduksi” (reduced units) dalam simulasi dinamis molekuler, yang mungkin juga bermanfaat untuk keperluan simulasi dinamis Brownian. Untuk paper berjudul “Shear viscosity of model mixtures by NEMD.I.Argon-Krypton mixtures”, ada hubungan yang menarik dengan sebuah paper lain berjudul “Effect of three-body forces on the shear viscosity of liquid argon”.
    Ada sumber lain yang relevan:
    1. http://arxiv.org/PS_cache/cond-mat/pdf/0504/0504605v1.pdf
    Judul: Histogram reweighting method for dynamic properties.pdf
    2. http://huggins.vuse.vanderbilt.edu/groupweb/research/pdfs/paper086-lee-jcp-99-93-3919.pdf
    Judul: Shear viscosity of moedl mixtures by nonequilibrium molecular dynamics.I.Argon-krypton mixtures.pdf
    Paper yang kedua ini memberikan informasi tentang simulasi dinamis molekuler nonequilibrium.
    3. Judul: Transport properties of Ar-Kr mixtures: A molecular dynamics simulation study.pdf
    Untuk hari ini, ada 5 paper yang saya kirim ke arsip blog sebagai bahan referensi penelitian: Empat paper saya sertakan bersama alamat websitenya, sedangkan satu paper tersisa tidak diketahui dari mana asalnya (alamatnya bisa ditelusuri, hanya saja cukup memakan waktu-tidak bagus dilakukan sekarang, sementara saya harus kuliah pagi ini.)

    04.gifdionisius montja

    On the relationship between tow body and three body interactions from nonequilibrium molecular dynamics simulation.pdf
    Histogram reweighting method for dynamic properties.pdf
    Shear viscosity of moedl mixtures by nonequilibrium molecular dynamics.I.Argon-krypton mixtures.pdf
    Transport properties of ArKr mixtures A molecular dynamics simulation study.pdf
    Effect of three-body forces on the shear viscosity of liquid argon.pdf