• Title/Summary/Keyword: DDFT

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The Ultrasonographic Evaluation of Digital Flexor Tendon in the Palmar Pastern Region of Normal Racing Horse (정상 경주마의 앞발바닥갓관절부 굽힘근힘줄의 초음파학적 평가)

  • Kim, Kun-Tae;Kim, Joon-Young;Jeong, Soon-Wuk
    • Journal of Veterinary Clinics
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    • v.25 no.2
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    • pp.90-95
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    • 2008
  • One fresh equine cadaver (two forelimbs) and five non-lamed thoroughbreds (ten sound forelimbs) were examined ultrasonographically through 5.0 MHz linear array transducer with a stand-off pad in palmar pastern region. The normal transverse ultrasonographic images of the superficial digital flexor tendon (SDFT), deep digital flexor tendon (DDFT), straight sesamoidean ligament (SSL), oblique sesamoidean ligament (OSL), and medium scutum could be identified at the region. The mean $\pm$ SD (min.$\sim$max. $mm^2$) of SDFT cross-sectional areas at P1A, P1B, P1C in the region were $110.00{\pm}5.38$ ($100{\sim}128$), $100.00{\pm}5.02$ ($90{\sim}111$), $114.00{\pm}3.33$ ($104{\sim}124$), respectively. The mean $\pm$ SD (min.$\sim$max. $mm^2$) of DDFT cross-sectional areas at each phalanx (P1A, P1B, P1C, P2A, P2B) were $136.00{\pm}4.83$ ($125{\sim}147$), $94.00{\pm}5.43$ ($85{\sim}108$), $99.00{\pm}4.87$ ($90{\sim}111$), $115.00{\pm}3.67$ ($108{\sim}124$), $135.00{\pm}3.65$ ($125{\sim}145$), respectively. The mean ratio of SDFT of P1B to DDFT was 0.74, 1.06, 1.01, 0.87, 0.74 at P1A, P1B, P1C, P2A, P2B, respectively.

Unstable Inverted Phases of Di- and Tri-block Copolymers on Solution-Casting Films

  • Sun Dachun;Huang Lei;Liang Haojun
    • Macromolecular Research
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    • v.13 no.2
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    • pp.152-155
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    • 2005
  • A dynamic density functional theory is presented for the observation of the phase revolutions of a solution-casting film of di- and tri-block copolymers under solvent evaporation conditions. With the evaporation of the solvent, the inverted phases, the minor part of the component becomes the continuous phase at the higher solvent evaporation rate, as observed in this experiment. Further simulation revealed that these inverted phases are converted into the normal phase and the major part of the component becomes the continuous phase, implying that the inverted phases observed in this experiment are unstable.