Scaling relationships, individual variation and the influence of temperature on maximum swimming speed in early settled stages of the turbot Scophthalmus maximus

1995 ◽  
Vol 121 (3) ◽  
pp. 401-408 ◽  
Author(s):  
S. Gibson ◽  
I. A. Johnston
Aquaculture ◽  
2003 ◽  
Vol 217 (1-4) ◽  
pp. 547-558 ◽  
Author(s):  
Erich H Van Ham ◽  
Marc H.G Berntssen ◽  
Albert K Imsland ◽  
Alkistis C Parpoura ◽  
Sjoerd E Wendelaar Bonga ◽  
...  

1992 ◽  
Vol 49 (8) ◽  
pp. 1570-1572 ◽  
Author(s):  
Anne Berit Skiftesvik

The activity and swimming speed of fed and starved larvae of Atlantic cod (Gadus morhua) and turbot (Scophthalmus maximus) were measured from hatching to metamorphosis. The results indicate changes in behaviour over time, as well as differences between starved and fed larvae. It is suggested that determining the point at which activity increases and swimming speed during active periods decreases may be relevant as an indicator of the time of first feeding in marine fish larvae.


Author(s):  
T. Geipel ◽  
W. Mader ◽  
P. Pirouz

Temperature affects both elastic and inelastic scattering of electrons in a crystal. The Debye-Waller factor, B, describes the influence of temperature on the elastic scattering of electrons, whereas the imaginary part of the (complex) atomic form factor, fc = fr + ifi, describes the influence of temperature on the inelastic scattering of electrons (i.e. absorption). In HRTEM simulations, two possible ways to include absorption are: (i) an approximate method in which absorption is described by a phenomenological constant, μ, i.e. fi; - μfr, with the real part of the atomic form factor, fr, obtained from Hartree-Fock calculations, (ii) a more accurate method in which the absorptive components, fi of the atomic form factor are explicitly calculated. In this contribution, the inclusion of both the Debye-Waller factor and absorption on HRTEM images of a (Oll)-oriented GaAs crystal are presented (using the EMS software.Fig. 1 shows the the amplitudes and phases of the dominant 111 beams as a function of the specimen thickness, t, for the cases when μ = 0 (i.e. no absorption, solid line) and μ = 0.1 (with absorption, dashed line).


2010 ◽  
Vol 25 (1) ◽  
pp. 93-105 ◽  
Author(s):  
Daniel Żarski ◽  
Dariusz Kucharczyk ◽  
Wojciech Sasinowski ◽  
Katarzyna Targońska ◽  
Andrzej Mamcarz

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