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首页> 外文期刊>Journal of rubber research >The Kinetics of Latex Flow from the Rubber Tree in Relation to Latex Vessel Plugging and Turgor Pressure
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The Kinetics of Latex Flow from the Rubber Tree in Relation to Latex Vessel Plugging and Turgor Pressure

机译:橡胶树中乳胶流动的动力学与乳胶容器堵塞和压力的关系

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Several attempts have been made in the past to express the rate of latex flow from the tapped tree as a function of time and various parameters concerned with fluid flow dynamics. However, no single model that was proposed could explain the regulation of latex flow rate from tapping to flow cessation. In the current study, the cumulative proportion of latex vessels that are plugged at any time, x, from tapping is shown to be proportional to [(x/t)]~(1/2) where t is the total flow duration. This relationship is maintained when latex vessel plugging rate is increased by shortening the tapping cut from (from half-spiral to one eighth spiral) or decreased by ethephon application. It is deduced that about 71% of the latex vessels would have plugged and are no longer contributing to the latex flow by the mid-point of flow duration. About half of the latex vessels are plugged after one quarter of the total flow duration has elapsed. It is also at this point in the course of latex flow that yielding latex vessels are least liable to plugging. The rapid latex flow observed immediately after tapping is attributed to the high turgor pressure (that is of an order of 10 atmospheres) of the laticifer system before tapping. The sharp decrease in latex flow immediately after tapping is explained by turgor loss. On the other hand, the effect of latex vessel plugging, in which lutoid damage plays a role, becomes more prominent towards the end of flow. The plugging rate among latex vessels that are still yielding rises steeply towards the late flow just before flow cessation. The two variables, turgor pressure and cumulative latex vessel plugging, when taken together account for 99% of the variation inflow rate from the time of tapping until the cessation of flow. Since cumulative latex vessel plugging is itself a function of time, latex flow rate can be expressed as a function of the laticifer turgor pressure and time without having to invoke considerations of fluid dynamics, latex vessel contraction or the dilution of the latex that occur during the course of flow.
机译:过去已经进行了几次尝试,以表示随时间变化以及与流体流动动力学有关的各种参数的关系,来表示从树上流出的乳胶流量。但是,没有提出的单一模型可以解释从流出到停止流动的乳胶流量调节。在当前的研究中,显示出在任何时候被塞住的乳胶容器的累积比例x都与[[x / t)]〜(1/2)成正比,其中t是总流动持续时间。当通过缩短出胶口的截断时间(从半螺旋到八分之一螺旋线)或通过施加乙烯利来降低胶乳容器的堵塞率时,可以维持这种关系。可以推断,大约71%的乳胶容器会堵塞,并且在流动持续时间的中点不再对乳胶的流动有所贡献。在总流量持续时间的四分之一过去后,约有一半的乳胶容器被堵塞。也是在乳胶流动过程中的这一点上,产生的乳胶容器最不容易堵塞。出胶后立即观察到的快速胶乳流动归因于出胶前胶乳系统的高膨胀压力(大约10个大气压)。出胶后,胶乳流量的急剧下降可以通过膨胀损失来解释。另一方面,胶体血管堵塞的作用在黄体样损害中起着重要作用,而胶体血管堵塞在流动末期变得更加明显。在仍要停止流动之前,仍在屈服的乳胶容器之间的堵塞率急剧上升。放在一起时,膨胀压力和乳胶容器的堵塞这两个变量合起来构成了从出水到停止流动为止的流入流量变化的99%。由于累积的乳胶容器堵塞本身是时间的函数,因此乳胶流速可以表示为胶乳膨胀压力和时间的函数,而不必考虑流体动力学,乳胶容器收缩或乳胶在稀释过程中发生的稀释等问题。流程。

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