scholarly journals Strength characteristic determination of a flat wagon carrying structure with a lower centre of gravity

2020 ◽  
Vol 32 ◽  
pp. 99-104
Author(s):  
Oleksij Fomin ◽  
Alyona Lovska ◽  
Václav Píštěk ◽  
Pavel Kučera
2000 ◽  
Vol 203 (6) ◽  
pp. 1059-1070 ◽  
Author(s):  
U. Nagel ◽  
H. Machemer

Wild-type and the morphological mutant kin 241 of Paramecium tetraurelia showed improved orientation away from the centre of gravity (negative gravitaxis) when accelerations were increased from 1 to 7 g. Gravitaxis was more pronounced in the mutant. A correlation between the efficiency of orientation and the applied g value suggests a physical basis for gravitaxis. Transiently enhanced rates of reversal of the swimming direction coincided with transiently enhanced gravitaxis because reversals occurred more often in downward swimmers than in upward swimmers. The results provide evidence of a physiological modulation of gravitaxis by means of the randomizing effect of depolarization-dependent swimming reversals. Gravity bimodally altered propulsion rates of wild-type P. tetraurelia so that sedimentation was partly antagonized in upward and downward swimmers (negative gravikinesis). In the mutant, only increases in propulsion were observed, although the orientation-dependent sensitivity of the gravikinetic response was the same as in the wild-type population. Observed swimming speed and sedimentation rates in the wild-type and mutant cells were linearly related to acceleration, allowing the determination of gravikinesis as a linear (and so far non-saturating) function of gravity.


Author(s):  
R F Allen

Axle loads for laden road tankers depend upon the configuration of the liquid tank. The paper determines the location of the centre of gravity of a liquid load in a tilted cylindrical barrel tank with dished and flanged ends and shows how the centre of gravity varies with the amount of liquid carried. The calculation permits greater accuracy in the determination of axle loads.


The nature of the angular distribution of the particles emitted in artificial transmutations is a matter which has received little attention. Hitherto experimental investigation has been mainly concentrated on the determination of the energy release and nature of various transmutations. But it is now clear that we have sufficiently precise data concerning the nature of many transmutations to make profitable their further investi­gation, and in particular the investigation of the angular distribution of the transmutation products. Moreover, in much of the literature it is implicitly assumed that the transmutation products are uniformly dis­tributed in space when referred to relative coordinates, i. e ., coordinates in which the centre of gravity of the system is considered to be at rest; in particular, all attempts to determine absolute yields depend upon the correctness of this assumption. The work so far published on this subject appears to support the uniformity of angular distribution, but further investigation is clearly of some importance. During the course of some cloud-chamber experiments on the trans­mutation 2 D + 2 D → 3 T + 1 H, (1) Dee formed the tentative opinion that the angular distribution of the protons emitted was not uniform. The alternative transmutation 2 D + 2 D → 3 He + 1 n (2) is very similar to (1), since the spins of the particles are probably identical and the energy balances of the same order of magnitude. We have therefore investigated the angular distribution for both these trans­mutations.


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