内蒙古毛乌素沙地不同生境油蒿(Artemisia ordosica Krasch.)灌丛地碳动态研究

油蒿(Artemisia ordosica Krasch.)是内蒙古鄂尔多斯高原特有的半灌木，构成该地区沙地优势植被类型。主要分布在固定、半固定沙丘，同时在流动沙丘也有少量分布。它在当地经济价值、防风固沙环保方面均处于无以取代的地位。在毛乌素沙地沙漠化日益扩大的严峻态势下,研究其群落地上、地下过程对生境变化的响应不仅对维持干旱、半干旱区生态系统稳定的管理措施上有所帮助，而且也有助于了解全球变化背景下物种对环境条件的长期变化适应策略。 为此，本项研究以毛乌素沙地为研究区域，利用异速生长关系确立不同生境油蒿生物量最佳回归方程，并调查、比较了毛乌素沙地固定沙丘、半固定沙丘和流动沙丘三个生境油蒿灌丛地的生物量、土壤和植被的碳储量、生产力和细根周转、土壤微生物生物量碳、氮和土壤呼吸。具体结果如下： 1. 建立并比较了油蒿枝、株两个水平上各部分（不含细根）生物量异速生长关系式，其中枝形态指标（枝直径BD、枝长BL、叶枝长LBL）与油蒿叶、枝、果各部分生物量的异速关系最好;株水平上冠层面积CA与其叶、枝干、果、粗根各部分生物量的回归效果较好。不同生境生物量与其生长变量的异速生长关系存在差异。2004年调查的油蒿灌丛生物量从固定沙丘、半固定沙丘到流动沙丘分别是354.8，178.3和30.4 g m-2;各部分（叶、枝干、果、粗根、不同径级细根的)生物量都呈递减趋势。地下根与总生物量比值排序为固定>半固定>流动沙丘。不同生境细根生物量垂直分布存在差异，在固定沙丘根可至100 cm，半固定沙丘达90 cm，而在流动沙丘仅为60 cm，这些结果有助于使了解不同生境中的相同物种如何通过自身形态及其生物量调整来适应生境的差异。 2. 不同生境油蒿灌丛地植被碳储量和土壤碳储量在P < 0.05水平上差异显著，其中固定沙丘植被碳储量和土壤碳储量分别为224.04和7521 g C m-2，半固定沙丘是119.27和3029 g C m-2，流动沙丘是16.83和2300 g C m-2。可见沙区土壤有机碳远大于植被碳量。 3. 利用最大值减最小值方法、标准取样法和内生长土芯法研究了不同生境油蒿灌丛地的地上、粗根生产力和地下细根生产力。发现各生境生产力、细根周转都随着植被盖度增加而增加，地下根生产力与总生产力之比随着植被盖度增加而减少;不同生境油蒿灌丛地生产力在P < 0.05水平上存在显著差异，2005年总生产力范围在18.23-293.82 g m-2 yr-1之间;细根总周转率在0.16-0.54 yr-1之间。 4. 利用异速生产关系确立不同生境不同水平上油蒿叶面积的最佳回归关系式并对不同生境的比叶面积（SLA）进行了比较，其中枝水平上各生境叶面积与枝直径、枝叶长、枝长相关关系在P < 0.001水平上显著;株水平上各生境叶面积与株高、冠层面积相关关系在P < 0.001水平显著;从固定沙丘、半固定沙丘到流动沙丘SLA由大变小，这可能与生境养分差异有关。 5. 不同生境油蒿灌丛地土壤微生物碳、氮和土壤呼吸范围分别在117.99-153.99 mg kg-1、1.49-3.31mg kg-1和0.54-1.96 μmol m-2 s-1之间，它们从固定沙丘、半固定沙丘到流动沙丘依次下降。

Temperature and biomass influences on interannual changes in CO2 exchange in an alpine meadow on the Qinghai-Tibetan Plateau

Three years of eddy covariance measurements were used to characterize the seasonal and interannual variability of the CO2 fluxes above an alpine meadow (3250 m a.s.l.) on the Qinghai-Tibetan Plateau, China. This alpine meadow was a weak sink for atmospheric CO2, with a net ecosystem production (NEP) of 78.5, 91.7, and 192.5 g C m(-2) yr(-1) in 2002, 2003, and 2004, respectively. The prominent, high NEP in 2004 resulted from the combination of high gross primary production (GPP) and low ecosystem respiration (R-e) during the growing season. The period of net absorption of CO2 in 2004, 179 days, was 10 days longer than that in 2002 and 5 days longer than that in 2003. Moreover, the date on which the mean air temperature first exceeded 5.0 degrees C was 10 days earlier in 2004 (DOY110) than in 2002 or 2003. This date agrees well with that on which the green aboveground biomass (Green AGB) started to increase. The relationship between light-use efficiency and Green AGB was similar among the three years. In 2002, however, earlier senescence possibly caused low autumn GPP, and thus the annual NEP, to be lower. The low summertime R-e in 2004 was apparently caused by lower soil temperatures and the relatively lower temperature dependence of R-e in comparison with the other years. These results suggest that (1) the Qinghai-Tibetan Plateau plays a potentially significant role in global carbon sequestration, because alpine meadow covers about one-third of this vast plateau, and (2) the annual NEP in the alpine meadow was comprehensively controlled by the temperature environment, including its effect on biomass growth.

Characterizing CO2 fluxes for growing and non-growing seasons in a shrub ecosystem on the Qinghai-Tibet Plateau

To assess carbon budget for shrub ecosystems on the Qinghai-Tibet Plateau, CO2 flux was measured with an open-path eddy covariance system for an alpine shrub ecosystem during growing and non-growing seasons. CO2 flux dynamics was distinct between the two seasons. During the growing season from May to September, the ecosystem exhibited net CO2 uptake from 08:00 to 19:00 (Beijing Standard Time), but net CO2 emission from 19:00 to 08:00. Maximum CO2 uptake appeared around 12:00 with values of 0.71, 1,19, 1.46 and 0.67 g CO2 m(-2) h(-1) for June, July, August and September, respectively. Diurnal fluctuation Of CO2 flux showed higher correlation with photosynthetic photon flux density than temperature. The maximum net CO2 influx occurred in August with a value of 247 g CO2 m(-2). The total CO2 uptake by the ecosystem was up to 583 g CO2 m(-2) for the growing season. During the non-growing season from January to April and from October to December, CO2 flux showed small fluctuation with the largest net CO2 efflux of 0.30 g CO2 m(-2) h(-1) in April. The diurnal CO2 flux was close to zero during most time of the day, but showed a small net CO2 eff lux from 11:00 to 18:00. Diurnal CO2 flux, is significantly correlated to diurnal temperature in the non-growing season. The maximum monthly net CO2 eff lux appeared in April, with a value of 105 g CO2 m(-2). The total net CO2 eff lux for the whole non-growing season was 356 g CO2 m(-2).

Seasonal patterns of gross primary production and ecosystem respiration in an alpine meadow ecosystem on the Qinghai-Tibetan Plateau

We measured the net ecosystem CO2 exchange (NEE) in an alpine meadow ecosystem (latitude 37degrees29'-45'N, longitude 101degrees12'-23'E, 3250 m above sea level) on the Qinghai-Tibetan Plateau throughout 2002 by the eddy covariance method to examine the carbon dynamics and budget on this unique plateau. Diurnal changes in gross primary production (GPP) and ecosystem respiration (R-e) showed that an afternoon increase of NEE was highly associated with an increase of R-e. Seasonal changes in GPP corresponded well to changes in the leaf area index and daily photosynthetic photon flux density. The ratio of GPP/R-e was high and reached about 2.0 during the peak growing season, which indicates that mainly autotrophic respiration controlled the carbon dynamics of the ecosystem. Seasonal changes in mean GPP and R-e showed compensatory behavior as reported for temperate and Mediterranean ecosystems, but those of GPP(max) and R-emax were poorly synchronized. The alpine ecosystem exhibited lower GPP (575 g C m(-2) y(-1)) than, but net ecosystem production (78.5 g C m(-2) y(-1)) similar to, that of subalpine forest ecosystems. The results suggest that the alpine meadow behaved as a CO2 sink during the 1-year measurement period but apparently sequestered a rather small amount of C in comparison with similar alpine ecosystems.

Molecular Dynamics Simulation of Thermal and Mechanical Properties of Polyimide-Carbon-Nanotube Composites

An aromatic polyimide and its mixture with randomly distributed carbon nanotubes (NTs) are simulated by using molecular dynamics, repeated energy minimization and cooling processes. The glass transition temperatures are identified through volume-temperature curves. Stress-strain curves, Young's moduli, densities and Poisson ratios are computed at different temperatures. It is demonstrated that the carbon NT reduces the softening effects of temperature on mechanical properties and increases the ability to resist deformation.

Tolman Effect On Fluid Dynamics In Carbon Nanotubes

The numerical solutions of or(R) given by two different methods (Samsonov et al., 2003; and Lu et al., 2005) are compared with the result that they are coincident closely (the difference is within 4%). We conclude that it is necessary to consider the Tolman correction in the calculation of fluid dynamics in carbon nanotubes. Although our conclusion is the same as that of Prylutskyy et al. (2005), the sign of our Tolman correction is opposite to theirs, and the difference can be attributed to the errors appeared in the paper of Prylutskyy et al.

Chiral symmetry analysis and rigid rotational invariance for the lattice dynamics of single-wall carbon nanotubes

We provide a detailed expression of the vibrational potential for the lattice dynamics of single-wall carbon nanotubes (SWCNT's) satisfying the requirements of the exact rigid translational as well as rotational symmetries, which is a nontrivial generalization of the valence force model for the planar graphene sheet. With the model, the low-frequency behavior of the dispersion of the acoustic modes as well as the flexure mode can be precisely calculated. Based upon a comprehensive chiral symmetry analysis, the calculated mode frequencies (including all the Raman- and infrared-active modes), velocities of acoustic modes, and the polarization vectors are systematically fitted in terms of the chiral angle and radius, where the restrictions of various symmetry operations of SWCNT's are fulfilled.