scholarly journals A shape equation for Hayward Kiwifruit

2019 ◽  
Vol 22 (1) ◽  
pp. 371-382 ◽  
Author(s):  
J. R. Olatunji ◽  
R. J. Love ◽  
Y. M. Shim ◽  
A. R. East
Keyword(s):  
Shape Equation

Numerical Simulation Research on the Shape of Top Coal Drawn-Body in Gently Inclined Seam

2012 ◽  
Vol 468-471 ◽  
pp. 2248-2254
Author(s):  
Qiang Li ◽  
Wan Kui Bu ◽  
Hui Xu ◽  
Xiao Bo Song
Keyword(s):  
Numerical Simulation ◽  
Numerical Model ◽  
Random Medium ◽  
Body Movement ◽  
The Other ◽  
Simulation Research ◽  
Research Results ◽  
Shape Equation ◽  
The Difference ◽  
Meso Scale

The numerical model of top coal drawing in gently inclined seam is built based on PFC2d software. By comparing with the theory of drawn-body movement law, it can be obtained that the shape of top coal drawn-body accords with the theory of random medium movement. The research results show that the form of the shape equation of top coal drawn-body is uniform while the top coal caving angle is different. On the other hand, with the difference of top coal caving angle and drawing height, the shape of top coal drawn-body is differential at the meso scale, which depends on the parameters of the shape equation of top coal drawn-body.

EQUIVALENCE OF THE TWO METHODS IN CALCULATING THE EQUILIBRIUM SHAPES OF CYLINDRICAL VESICLES

1999 ◽  
Vol 13 (16) ◽  
pp. 547-553
Author(s):  
SHAOGUANG ZHANG ◽  
ZHONGCAN OUYANG ◽  
JIXING LIU
Keyword(s):  
Differential Equations ◽  
Ordinary Differential Equations ◽  
The Other ◽  
General Shape ◽  
Calculus Of Variation ◽  
And Topology ◽  
Shape Equation ◽  
Equilibrium Shapes ◽  
Comparison Of The Results ◽  
The Relationship

So far, two methods are often used in solving the equilibrium shapes of vesicles. One method is by starting with the general shape equation and restricting it to the shapes with particular symmetry. The other method is by assuming the symmetry and topology of the vesicle first and treating it with the calculus of variation to get a set of ordinary differential equations. The relationship between these two methods in the case of cylindrical vesicles, and a comparison of the results are given.

THE HOT CARRIER TEMPERATURE IN THE ANALYSIS OF THE FREE TO ACCEPTOR PHOTOLUMINESCENCE TRANSITION

2001 ◽  
Vol 15 (17n19) ◽  
pp. 696-699 ◽  
Author(s):  
G. Fonthal ◽  
M. de los Rios ◽  
J. Quintero ◽  
N. Piraquive ◽  
H. Ariza-Calderón
Keyword(s):  
Fermi Level ◽  
Band Gap ◽  
Density Of States ◽  
Impurity Concentration ◽  
Lattice Temperature ◽  
Band Tail ◽  
Hot Carrier ◽  
Additional Information ◽  
Carrier Temperature ◽  
Shape Equation

We analyzed the free to acceptor (e-A) photoluminescence transition on a GaAs:Ge sample using the hot carrier temperature and the Kane's DOS. This latter temperature was calculated by the spectra largest energy tail. While the lattice temperature was put in the e-A Eagles' shape equation, the fitting was poor but if the modified line was put into the equation, the fitting was better. So, the ionization impurity energy, the band gap, the Fermi level and the band tail can be measured with a better precision than the measurements traditionally made with this method, Additional information about phonons participant can be obtained. In conclusion, the hot carrier temperature and the density of states due to the impurity concentration should be used in the e-A transition photoluminescence analysis.

The evolution of slender inviscid drops in an axisymmetric straining flow

1980 ◽  
Vol 101 (3) ◽  
pp. 545-553 ◽  
Author(s):  
E. J. Hinch
Keyword(s):  
Global Stability ◽  
Stable Equilibrium ◽  
Stability Result ◽  
Reynolds Numbers ◽  
Time Dependent ◽  
Initial Shape ◽  
Low Reynolds Numbers ◽  
Long Wavelength ◽  
Shape Equation ◽  
Low Reynolds

The evolution of the shape of a slender inviscid drop in an axisymmetric straining motion is studied at low Reynolds numbers. It is found that the shape equation can be solved by polynommals with time-dependent coefficients. A global stability result can be used to show simply that only one possible equilibrium is stable. It is further shown that if the slender drop starts with a long-wavelength waist then it cannot go to this stable equilibrium and must either extend indefinitely or burst. In the class of trinomial shapes, it is shown that the drop either bursts or goes to the stable equilibrium, depending on whether or not the initial shape has a waist.

• Symmetry Properties of the Membrane Shape Equation

2013 ◽  
Author(s):  
Vladimir Pulov ◽  
Edy Chacarov ◽  
Mariana Hadzhilazova ◽  
Ivaïlo Mladenov
Keyword(s):  
Symmetry Properties ◽  
Shape Equation ◽  
Membrane Shape

New solutions of the shape equation

2002 ◽  
Vol 29 (2) ◽  
pp. 327-330 ◽  
Author(s):  
I.M. Mladenov
Keyword(s):  
Shape Equation
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