professional factory provide TU-1J04 thermal wax actuator for electric switch valve to Chile Factory
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professional factory provide TU-1J04 thermal wax actuator for electric switch valve to Chile Factory Detail:
1. Operation Principle
The Thermostatic Wax that has been sealed in shell body induces expansion by a given temperature, and inner rubber seal part drives its handspike to move under expansion pressure to realize a transition from thermal energy into mechanical energy. The Thermostatic Wax brings an upward movement to its handspike, and automatic control of various function are realized by use of upward movement of handspike. The return of handspike is accomplished by negative load in a given returned temperature.
2. Characteristic
(1)Small body size, occupied limited space, and its size and structure may be designed in according to the location where needs to work.
(2)Temperature control is reliable and nicety
(3)No shaking and tranquilization in working condition.
(4)The element doesn’t need special maintenance.
(5)Working life is long.
3.Main Technical Parameters
(1)Handspike’s height may be confirmed by drawing and technical parameters
(2)Handspike movement is relatives to the temperature range of the element, and the effective distance range is from 1.5mm to 20 mm.
(3)Temperature control range of thermal wax actuator is between –20 ~ 230℃.
(4)Lag phenomenon is generally 1 ~ 2℃. Friction of each component part and lag of the component part temperature cause a lag phenomenon. Because there is a difference between up and down curve of traveling distance.
(5)Loading force of thermal wax actuator is difference, it depends on its’ shell size.
Product detail pictures:
We can easily usually fulfill our respected customers with our very good top quality, very good price tag and excellent support due to we have been more expert and much more hard-working and do it in cost-effective way for professional factory provide TU-1J04 thermal wax actuator for electric switch valve to Chile Factory, The product will supply to all over the world, such as: Egypt , Leicester , Surabaya , We take measure at any expense to achieve essentially the most up-to-date equipment and approaches. The packing of nominated brand is our a further distinguishing feature. The products to assure years of trouble-free service has attracted a great deal customers. The solutions are obtainable in improved designs and richer assortment, they're created scientifically of purely raw supplies. It readily available in a variety of designs and specifications for your selection. The most recent kinds are a great deal better than the preceding one particular and they are quite popular with lots of prospects.
Ball Screw Lifter — Our unique Imported Ball Screw Lift System has safety advantages that are unmatched in the industry. More Robust, incorporating a virtually frictionless hardened screw and nut assembly that has a much greater life cycle than other designs. All motion is created via Direct Drive with Electric Geared TEFC motors. All Positioning is machine tool accurate. The Lift will remain in position under load indefinitely without power. The Steel column is a One-Piece Structure. The internal load bearing tracks are manufactured to a perfect design, and welded to the inside of the column.
Vidéo 4/4 sur la simulation numérique d’un écoulement électroosmotique en milieu poreux.
J’espère que ça vous aidera, et désolé pour la qualité de la vidéo et des explications, j’ai dû faire vite. Bon visionnage et bon courage pour votre travail !
Liens des tutoriaux pour Blender:
Code pour l’UDF dans Fluent:
#include “udf.h”
#include “models.h”
enum
PSI
;
real z = 1;
real F = 96485.33289; /*(C/mol) */
real R = 8.3144621 ; /* (J/mol*K) */
real T = 305; /* (K) */
real epsilon = 6.9*0.0000000001; /* (C/V*m) */
real Ex = 40000; /* (V/m) */
real c_0 = 7.5*0.001; /* (mol/m3) loin du mur */
real x[ND_ND];
real y;
Thread *t;
cell_t c;
face_t f;
DEFINE_SOURCE(axial_mom_source, c, t, dS, eqn)
float S_x;
dS[eqn] = 0;
S_x = -2*z*F*c_0*sinh(z*F*C_UDSI(c, t, 0)/(R*T))*Ex;
return S_x;
DEFINE_SOURCE(psi_source, c, t, dS, eqn)
float S_psi;
dS[eqn] = -2*pow(z,2)*pow(F,2)*c_0*cosh(z*F*C_UDSI(c,t,0)/(R*T))/(epsilon*R*T);
S_psi = -2*z*F*c_0*sinh(z*F*C_UDSI(c, t, 0)/(R*T))/epsilon;
return S_psi;
Sources:
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Wang, X., Cheng, C., Wang, S., & Liu, S. (2009). Electroosmotic pumps and their applications in microfluidic systems. Microfluidics and Nanofluidics.
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Yao, S., & Santiago, J. G. (2003). Porous glass electroosmotic pumps: theory. Journal of Colloid and Interface Science, 268(1), 133-142.
Patel, V., & Kassegne, S. K. (2007). Electroosmosis and thermal effects in magnetohydrodynamic (MHD) micropumps using 3D MHD equations. Sensors and Actuators B: Chemical, 122(1), 42-52.
Pieritz, R. A. (1998). Modélisation et simulation de milieux poreux par réseaux topologiques (Doctoral dissertation, Université Joseph Fourier–Grenoble).
Kang, Y., Yang, C., & Huang, X. (2002). Dynamic aspects of electroosmotic flow in a cylindrical microcapillary. International Journal of Engineering Science, 40(20), 2203-2221.
Balli, M., Mahmed, C., Duc, D., Nikkola, P., Sari, O., Hadorn, J. C., & Rahali, F. (2012). Le renouveau de la réfrigération magnétique. Revue Générale du Froid, 102(1121), 45-54
Drake, D. G., & Abu-Sitta, A. M. (1966). Magnetohydrodynamic flow in a rectangular channel at high Hartmann number. Zeitschrift für angewandte Mathematik und Physik ZAMP, 17(4), 519-528.
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