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鱼鳔逆流倍增的数学模型。

A mathematical model for counter-current multiplications in the swim-bladder.

作者信息

Sund T

出版信息

J Physiol. 1977 Jun;267(3):679-96. doi: 10.1113/jphysiol.1977.sp011833.

Abstract
  1. A computer model for swim-bladder gas filling has been developed. Phenomenological descriptions of the Root effect (pH-dependent O2 capacity of fish haemoglobin), of the lactic acid production in the gas gland and of the geometry of the rete mirabile are incorporated in the general counter-current equations to give a comprehensive model of gas filling. 2. It is known that pH along the rete is not constant, as supposed in an earlier gas-filling model. It is also known that the Root shift reaction has a different half-time model. It is also known that the Root shift reaction has a different half-time depending on whether the haemoglobin absorbs or releases O2. These particular effects are accounted for in the present model. 3. The model gives gas filling rate and maximum swim-bladder pressure for CO2, O2 and N2. The partial pressure of these gases as well as the concentration of lactic acid and the pH along the rete are also calculated. 4. The model reproduces quite accurately experimental values for gas-filling rate in eel, together with lactic acid, CO2 and O2 concentrations measured at the rete end-points. There is also good correlation between maximum predicted stable swim-bladder pressure and maximum recorded depth for four fishes investigated (r=0-937; P=0-06). 5. The model predicts an enhancement of O2 filling rate and maximum swim-bladder pressure of at least 4 when the reaction rates of the Root shift in eel haemoglobin are 0-2 sec (Root-off) and 10 sec (Root-on), as compared to an instantaneous Root shift. 6. With a swim-bladder pressure of 1 atm and Root-shift reaction rates of equal magnitude, the po2-profile along the rete is nearly linear. When the reaction rates are such as found experimentally in eel haemoglobin, the po2 along the rete is non-linear, with a maximum of approximately 2 atm near the bladder pole of the rete. An experimental verification of this maximum will constitute a crucial test of the model. 7. The calculations show that blood flow through rete can regulate both gas-filling rate and stable swim-bladder pressure. At high pressure, the main factor limiting gas filling is loss of gas through back diffusion along the rete. 8. Maximum po2 in the swim-bladder is highly dependent upon the Root effect. If the Root effect persists up to about 100 atm, as seems to be the case blue hake, maximum po2 is more than 200 atm. When the Root effect is abolished at 10 atm, as is expected in eel, the maximum po2 drops to about 30 atm. 9. The pN2 in the bladder can reach 10-15 atm depending on blood flow, whereas PCO2 will not exceed 1 atm.
摘要
  1. 已开发出一种用于鱼鳔气体填充的计算机模型。将罗特效应(鱼类血红蛋白的pH依赖性氧容量)、气体腺中乳酸产生以及神奇网的几何结构的现象学描述纳入通用逆流方程,以给出气体填充的综合模型。2. 众所周知,沿着神奇网的pH并非如早期气体填充模型所假设的那样恒定。还已知罗特位移反应具有不同的半衰期模型。也已知罗特位移反应根据血红蛋白吸收或释放氧气而具有不同的半衰期。本模型考虑了这些特殊效应。3. 该模型给出了二氧化碳、氧气和氮气的气体填充速率以及鱼鳔最大压力。还计算了这些气体的分压以及沿着神奇网的乳酸浓度和pH。4. 该模型相当准确地再现了鳗鱼气体填充速率的实验值,以及在神奇网端点处测得的乳酸、二氧化碳和氧气浓度。对于所研究的四种鱼类,预测的最大稳定鱼鳔压力与记录的最大深度之间也具有良好的相关性(r = 0 - 937;P = 0 - 06)。5. 该模型预测,与瞬时罗特位移相比,当鳗鱼血红蛋白中罗特位移的反应速率为0 - 2秒(罗特关闭)和10秒(罗特开启)时,氧气填充速率和鱼鳔最大压力至少提高4倍。6. 在鱼鳔压力为1个大气压且罗特位移反应速率大小相等的情况下,沿着神奇网的氧分压分布几乎是线性的。当反应速率如在鳗鱼血红蛋白中实验发现的那样时,沿着神奇网的氧分压是非线性的,在神奇网靠近鱼鳔极处最大值约为2个大气压。对这个最大值的实验验证将构成对该模型的关键测试。7. 计算表明,通过神奇网的血流可以调节气体填充速率和稳定的鱼鳔压力。在高压下,限制气体填充的主要因素是气体沿神奇网的反向扩散损失。8. 鱼鳔中的最大氧分压高度依赖于罗特效应。如果罗特效应持续到约100个大气压,如蓝鳕似乎就是这种情况,最大氧分压超过200个大气压。当在10个大气压下罗特效应消失时,如鳗鱼中预期的那样,最大氧分压降至约30个大气压。9. 鱼鳔中的氮分压可根据血流达到10 - 15个大气压,而二氧化碳分压不会超过1个大气压。

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THE SECRETION OF OXYGEN INTO THE SWIM-BLADDER OF FISH. 3. THE ROLE OF CARBON DIOXIDE.
J Gen Physiol. 1964 Nov;48(2):337-55. doi: 10.1085/jgp.48.2.337.
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THE PHYSIOLOGY OF THE SWIMBLADDER IN THE EEL ANGUILLA VULGARIS. III. THE MECHANISM OF GAS SECRETION.
Acta Physiol Scand. 1963 Nov;59:221-41. doi: 10.1111/j.1748-1716.1963.tb02738.x.
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The secretion of inert gas into the swim-bladder of fish.
J Gen Physiol. 1958 Mar 20;41(4):783-804. doi: 10.1085/jgp.41.4.783.
6
The histophysiology of the teleostean physoclistous swimbladder.
J Cell Comp Physiol. 1952 Oct;40(2):317-35. doi: 10.1002/jcp.1030400211.
7
The mechanism of oxygen concentration in the swim-bladder of the eel.
J Physiol. 1968 Apr;195(3):631-8. doi: 10.1113/jphysiol.1968.sp008478.
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Physical aspects of swimbladder function.
Biol Rev Camb Philos Soc. 1966 Feb;41(1):141-76. doi: 10.1111/j.1469-185x.1966.tb01542.x.
9
The rate of the root shift in eel red cells and eel haemoglobin solutions.
J Physiol. 1969 Oct;204(2):259-82. doi: 10.1113/jphysiol.1969.sp008912.

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