Explicit immersions of surfaces in $${{\mathbb {R}}}^4$$ with arbitrary constant Jordan angles

2020 ◽  
Vol 209 (1) ◽  
pp. 15-30
Author(s):  
J. Monterde ◽  
R. C. Volpe
Keyword(s):  
1964 ◽  
Vol 86 (2) ◽  
pp. 265-270 ◽  
Author(s):  
G. Horvay ◽  
M. Dacosta

When an infinitely long cylindrical rod travels from a chamber at one temperature ϑa to a chamber (insulated from the first) at a higher temperature ϑf, then heat will leak out along the rod from the second chamber to the first, whose amount decreases as the speed of the rod increases. Using the Wiener-Hopf method of solution, we determine the temperature distribution in the rod for the case where in the second chamber the heat-transfer coefficient h+ is infinite, while in the first chamber it has an arbitrary constant value h. Families of curves illustrate the temperature distribution in the two special cases where h = ∞ (isothermal boundary conditions in lower chamber) and where h = 0 (rod is insulated in lower chamber).


1890 ◽  
Vol 28 (4) ◽  
pp. 316-332 ◽  
Author(s):  
William Matthew Makeham

Referring again to Art. 4 of Gompertz's treatise, let us denote by a0dx the actual probability of dying in the infinitely small time dx, at the initial age of the mortality table, and by axdx the abstract chance of death (in the time dx) at the end of x years; that is to say, the chance considered “independently of” (as Gompertz expresses it) or as “abstracted from” the deterioration resulting from increased age, then, according to Gompertz's law, the actual probability of dying, in the time dx, at the latter age will be axqxdx, in which expression q only is an arbitrary constant denoting the rate of deterioration. If, in axqxdx, we put x=0, it becomes a0dx, which coincides with the expression first assumed. Hence, Gompertz's law, which supposes that “the “vital force or recuperative power loses equal proportions in equal “times”, is expressed, in its general form, by the equation μxdx=axqxdx, or, which is the same thing, by μx=axqx.


1991 ◽  
Vol 113 (2) ◽  
pp. 339-342 ◽  
Author(s):  
Prawal Sinha ◽  
C. M. Rodkiewicz

The influence of the inclusion of convection and dissipation terms in the energy equation, on the characteristics of a conical bearing with constant film thickness, rotating with a uniform angular velocity is examined. The slider temperature is taken to be an arbitrary constant, greater, equal or smaller, than the assumed constant temperature of the pad. The fluid is considered to be incompressible and the viscosity is assumed to vary exponentially with temperature. The governing system of coupled momentum and energy equations, in conical coordinates, is solved numerically using the finite difference method to yield the various bearing characteristics. The results show that the inclusion of dissipation function alone leads to an underestimation of load capacity and torque, whereas the inclusion of convection terms alone leads to an overestimation of the same.


1924 ◽  
Vol 22 (3) ◽  
pp. 248-252
Author(s):  
R. Hargreaves

§ 1. In the transformation corresponding to constant acceleration, and in the resulting quadratic form, there is an arbitrary constant. In Einstein's formula for central acceleration a mass m defining the acceleration appears, but no arbitrary constant. In seeking to account for, or to repair, the deficiency I retained all constants naturally arising in the integration of the differential equations, and it then appeared that the result could be obtained by transformation. It will be convenient to state the transformation at the outset, and then to examine the differential equations with a view to a clear understanding of the assumptions made in reaching the more general result.


The purpose of this note is to describe a certain class of solutions of the Klein-Gordon equation, free of singularities and involving an arbitrary constant β in addition to the massparameter μ . Examination of the field suggests that it might be interpreted as a model particle with half-life β and radius r 1 = ( β/μ ) ½ .


1968 ◽  
Vol 1 (11) ◽  
pp. 12
Author(s):  
D.H. Peregrine

This warier summarises some recent work on lone gravity waves on still water m channels of arbitrary constant cross-section. Theoretical results have been obtained for both straight and curved channels. Some experimental work has been performed m straight trapezoidal channels and shows reasonable agreement with theory. For straight channels some details of the second approximation are given, and the cases where the approximation breaks down are indicated. For curved channels it is found that the effect of channel curvature is more pronounced when the cross-sectional shane of the channel is not symmetric with resnect to its centre-line.


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