• Title/Summary/Keyword: $C_2$ Dissociation

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Studies on X-Y Chromosome Dissociation Induced by Environmental Mutagens in Mouse (환경성 돌연변이원에 의한 Mouse의 X-Y 염색체 조기분리에 관한 연구)

  • 윤경희;이원호
    • Journal of Environmental Science International
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    • v.7 no.5
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    • pp.599-605
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    • 1998
  • The purpose of this work was to examine whether X-Y chromosome dissociation in the primary spermatocytes of mice could be used as an in vivo short-term assaying system that detect environmental mutagens. Four alkylating agents(EMS, MMS, MMC and MNNG) which were known as strong mutagens were administered to BALB/c male mice 3-4 months old. In the control group, the mean frequencies of previously dissociated X and Y chromosomes and autosomes were 7.17% and 2.12%, respectively. Compared to the control group, mutagen-treated groups have no significant differences in dissociation rate of autosomes, while these poops were about 1.2-2.5 times higher in the frequencies of X-Y dissociation. Generally, X-Y dissociation frequency increased consistently with the concentration of mutagens whereas the tendency of autosome dissociation frequency was variable among several mutagens. These results suggest that X-Y dissociation in the primary spermatocytes of mice is applicable as an vivo short-term assaying system for environmental mutagens. There were significantly distinct increase in dissociation of X-Y chromosome in both the hybrid and parents but the X-Y previous dissociation of hybrid appeared higher frequency than BALB /c and wild mice. These results indicate that the factor related to binding X-Y chromosome is specific to strains.

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Reconsideration of CN Radiation an d $C_2$ Dissociation Rate Coefficient ($C_2$의 해리 반응 계수와 CN 복사에 대한 재고찰)

  • Hyun, Seong-Yoon;Park, Chul;Chang, Keun-Shik
    • 한국전산유체공학회:학술대회논문집
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    • 2008.03b
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    • pp.92-95
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    • 2008
  • We performed the theoretical calculation of CN Violet radiation using the code SPRADIAN07 to predict the Lee et al.'s experimental measurements and to reinvestigate $C_2$ dissociation rate. CN Violet radiations are calculated under the Boltzmann and non-Boltzmann distribution using two chemical reaction sets: Park-Losev-G\"{o}kcen-Tsang and Park-Losev-G\"{o}kcen-Tsang-Lee models. Our SPRADIAN07 calculations show improvement in prediction of absolute radiation intensity of CN Violet and its decay rate by Park-Losev-G\"{o}kcen-Tsang reaction set with $C_2$ dissociation rate coefficient of $k_f$ = 1.5${\times}$10$^{16}$ exp(-71,600/$T_x$) cm$^3$ mole$^{-1}$ s$^{-1}$.

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Vibrational Relaxation and Bond Dissociation in Methylpyrazine on Collision with N2 and O2

  • Young-Jin Yu;Sang Kwon Lee;Jongbaik Ree
    • Journal of the Korean Chemical Society
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    • v.67 no.6
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    • pp.407-414
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    • 2023
  • The present study uses quasi-classical trajectory procedures to examine the vibrational relaxation and dissociation of the methyl and ring C-H bonds in excited methylpyrazine (MP) during collision with either N2 or O2. The energy-loss (-ΔE) of the excited MP is calculated as the total vibrational energy (ET) of MP is increased in the range of 5,000 to 40,000cm-1. The results indicate that the collision-induced vibrational relaxation of MP is not large, increasing gradually with increasing ET between 5,000 and 30,000 cm-1, but then decreasing with the further increase in ET. In both N2 and O2 collisions, the vibrational relaxation of MP occurs mainly via the vibration-to-translation (V→T) and vibration-to-vibration (V→V) energy transfer pathways, while the vibration-to-rotation (V→R) energy transfer pathway is negligible. In both collision systems, the V→T transfer shows a similar pattern and amount of energy loss in the ET range of 5,000 to 40,000cm-1, whereas the pattern and amount of energy transfer via the V→V pathway differs significantly between two collision systems. The collision-induced dissociation of the C-Hmethyl or C-Hring bond occurs when highly excited MP (65,000-72,000 cm-1) interacts with the ground-state N2 or O2. Here, the dissociation probability is low (10-4-10-1), but increases exponentially with increasing vibrational excitation. This can be interpreted as the intermolecular interaction below ET = 71,000 cm-1. By contrast, the bond dissociation above ET = 71,000 cm-1 is due to the intramolecular energy flow between the excited C-H bonds. The probability of C-Hmethyl dissociation is higher than that of C-Hring dissociation.

Collision-induced Energy Transfer and Bond Dissociation in Toluene by H2/D2

  • Ree, Jongbaik;Kim, Yoo Hang;Shin, Hyung Kyu
    • Bulletin of the Korean Chemical Society
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    • v.34 no.12
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    • pp.3641-3648
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    • 2013
  • Energy transfer and bond dissociation of $C-H_{methyl}$ and $C-H_{ring}$ in excited toluene in the collision with $H_2$ and $D_2$ have been studied by use of classical trajectory procedures at 300 K. Energy lost by the vibrationally excited toluene to the ground-state $H_2/D_2$ is not large, but the amount increases with increasing vibrational excitation from 5000 and $40,000cm^{-1}$. The principal energy transfer pathway is vibration to translation (V-T) in both systems. The vibration to vibration (V-V) step is important in toluene + $D_2$, but plays a minor role in toluene + $H_2$. When the incident molecule is also vibrationally excited, toluene loses energy to $D_2$, whereas it gains energy from $H_2$ instead. The overall extent of energy loss is greater in toluene + $D_2$ than that in toluene + $H_2$. The different efficiency of the energy transfer pathways in two collisions is mainly due to the near-resonant condition between $D_2$ and C-H vibrations. Collision-induced dissociation of $C-H_{methyl}$ and $C-H_{ring}$ bonds occurs when highly excited toluene ($55,000-70,400cm^{-1}$) interacts with the ground-state $H_2/D_2$. Dissociation probabilities are low ($10^{-5}{\sim}10^{-2}$) but increase exponentially with rising vibrational excitation. Intramolecular energy flow between the excited C-H bonds occurring on a subpicosecond timescale is responsible for the bond dissociation.

Dissociation Equilibrium of Dimeric Association of 3,3-Diethyl-9-Methyl-Thiacarbocyanine Dye (3,3’-Diethyl-9-Methyl-Thiacarbocyanine 색소 2 분자 회합체의 해리평형)

  • 김성훈;김재홍;송경헌;임용진
    • Textile Coloration and Finishing
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    • v.5 no.3
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    • pp.216-220
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    • 1993
  • Dissociation constants and heat of dissociation of dimers of 3, 3'-diethyl-thiacarbocyanine dye(Dye 2) have been studied. At $10~40^{\circ}C$, absorption spectra of 2 vol% aqueous ethanol solutions of Dye 2 showed monomer and dimer bands. From the temperature dependence of monomer absorbance, dissociation constants K and ${\Delta}H$ were estimated to be $6.2(10^{\circ}C)-10.6(40^{\circ}C)mon/\ell$ and 3kcal/mol, respectively. These K valus are about one half of those for 3,3'-diethyl-2,2'-cyanine dye with one methine carbon, indication a higher dimer stability than that of 3,3-diethyl-2,2'-cyanine dye.

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Excursion, Roaming and Migration of Hydrogen Atom during Dissociation of Formaldehyde

  • Kim, Hyung-Rae
    • Bulletin of the Korean Chemical Society
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    • v.35 no.5
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    • pp.1285-1293
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    • 2014
  • Several interesting features in trajectory were observed in the direct dynamics study of formaldehyde dissociation above radical dissociation limit. The hydrogen atom deliberately placed on the radical dissociation path can turn around at some distance from C without completion of dissociation and return to HCO moiety, colliding with it just as in a radical-radical recombination and producing a highly energized molecule. Excursion of a hydrogen atom to a distance of 6-8 bohrs and migration of a hydrogen atom back and forth between C and O are two of the most interesting features exhibited by the energized molecule. A series of excursions is seen to lead to a different kind of dissociation resembling roaming-like dissociation characterized by high vibrational excitation of $H_2$ fragment. It is suggested that excursion occurs due to involvement of two different force field systems that exhibit discontinuity in 6-8 bohrs from HCO moiety. We argue that roaming is a non-zero impact parameter version of the excursion.

Theoretical study on the dissociation reactions of C4F6 molecules

  • Choe, Hui-Cheol;Park, Yeong-Chun;Lee, Yun-Seop
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.08a
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    • pp.36-36
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    • 2010
  • Low-pressure fluorocarbon plasmas are widely used in microelectronics fabrication for a variety of surface modification purposes. In particular, fluorocarbon plasmas are used for the etching of dielectrics such as silicon dioxide and silicon nitride. Among the various fluorocarbons, this study focuses on C4F6 molecules (C4F6s) which are composed of hexafluorocyclobutene (c-C4F6), hexafluoro-1, 3-butadiene (1, 3-C4F6), and hexafluoro-2-butyne (2-C4F6). We have investigated the dissociation reactions of C4F6s, resulting in CF2, CF3, C2F3, and C3F3 fragments, by using the wB97X-D functional with various basis sets. In this presentation, the geometrical properties, energetics, and dissociation mechanisms of C4F6s will be suggested.

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Energy Flow and Bond Dissociation of Vibrationally Excited Toluene in Collisions with N2 and O2

  • Ree, Jongbaik;Kim, Sung Hee;Lee, Sang Kwon
    • Bulletin of the Korean Chemical Society
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    • v.34 no.5
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    • pp.1494-1502
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    • 2013
  • Energy flow and C-$H_{methyl}$ and C-$H_{ring}$ bond dissociations in vibrationally excited toluene in the collision with $N_2$ and $O_2$ have been studied by use of classical trajectory procedures. The energy lost by the vibrationally excited toluene upon collision is not large and it increases slowly with increasing total vibrational energy content between 5,000 and 45,000 $cm^{-1}$. Intermolecular energy transfer occurs via both of V-T and V-V transfers. Both of V-T and V-V transfers increase as the total vibrational energy of toluene increases. When the total energy content $E_T$ of toluene is sufficiently high, either C-H bond can dissociate. The C-$H_{methyl}$ dissociation probability is higher than the C-$H_{ring}$ dissociation probability, and that in the collision with $N_2$ is larger than with $O_2$.

An anomalous dissociation of protonated cluster ions of DNA guanine-cytosine base-pair

  • Seong, Yeon-Mi;Han, Sang-Yun;Jo, Sung-Chan;Oh, Han-Bin
    • Mass Spectrometry Letters
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    • v.2 no.3
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    • pp.73-75
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    • 2011
  • In the collisionally-activated dissociation of the proton-bound cluster ions of DNA base guanine (G) and cytosine (C), $G{\bullet}{\bullet}H^+{\bullet}{\bullet}C$, the abundance of [$CH^+$] ions was found to be higher than that of [$GH^+$] despite the fact that G has a higher proton affinity than C. This unexpected observation seems to demonstrate another example that the simple kinetic method scheme does not work. We suggest that a kinetic factor or detailed dynamics governing the proton transfer and dissociation should be carefully considered in the applications of the kinetic method to the proton affinity measurements.

Regulation of c-fos promoter through interaction between dopamine D3 receptor and RGL, ral GDP dissociation stimulator-like

  • Park, Ju-Ran;Kim, So-Young;Kim, Kyeong-Man
    • Proceedings of the PSK Conference
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    • 2003.10b
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    • pp.89.2-89.2
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    • 2003
  • Ral GDP dissociation stimulator (Ral GDS) has been found to be an effector protein of Ras, and Ral, a member of small GTP-binding protein (G protein) superfamily, has been suggested to act downstream of Ras. Ral GDP dissociation stimulator-like (RGL) shares 50% amino acid identity with Ral GDP dissociation stimulator, and assumed to possess similar functional role. Using yeast two-hybrid screening, we found that dopamine D3 receptor interacts with RGL. Since RGL is known to regulate the expression of c-fos promoter, effects of D3R on gene expression of c-fos promoter was studied. (omitted)

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