What are visco-elastic properties?
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if something is viscoelastic, it is both viscous - it will deform irreversably, and elastic - it will deform reversibly. everything is really viscoelastic, but some things, like rubber bands are mostly elastic, and some, like liquids, are mainly viscous.\n\nviscoelastic materials will mostly revert to form when they undergo small stresses, but will deform irreversibly under large stress. good examples are metal springs - they will revert completely if you only pull a little bit, but if you really stretch out a spring, it will lose its springyness.
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The elastic limit is the stress at which a material no longer undergoes a change in strain linearly proportional to the change in stress. At stress levels below the elastic limit the material is said to be elastic.
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The Maxwell model can be represented by a purely viscous damper and a purely elastic spring connected consecutively, as shown in the diagram. In this configuration, under an applied axial stress, the total stress, σTotal and the total strain, εTotal can be defined as follows:\nσTotal = σD = σS \nεTotal = εD + εS \nwhere the subscript D indicates the stress/strain in the damper and the subscript S indicates the stress/strain in the spring. Taking the derivative of strain with respect to time, we obtain:\nwhere E is the elastic modulus and c is the material coefficient of viscosity. This model describes the damper as a Newtonian fluid and models the spring with Hooke's law.\nIf we connect these two elements in parallel, we get a model of Kelvin-Voigt material.\nIn a Maxwell material, stress σ, strain ε and their rates of change with respect to time t are governed by equations of the form:\nor, in dot notation:\nwhere E is a modulus of elasticity and c a "viscosity". The equation can be applied either to the shear stress or to the uniform tension in a material. In the former case, the viscosity corresponds to that for a Newtonian fluid. In the latter case, it has a slightly different meaning relating stress and rate of strain.\nThe model is usually applied to the case of small deformations. For the large deformations we should include some geometrical non-linearity. For the simplest way of generalizing the Maxwell model, refer to the Upper Convected Maxwell Model.
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You can think of viscosity as referring to how much drag is exerted on a surface as the liquid flows by.  Generally, a thicker fluid has higher viscosity so I agree with your choice of honey.\n\nAs particles (molecules) become more loosely connected, the liquid flows more easily, so should be obvious how this relates to viscosity.
281995
Is it elasticity? Try to solve the problem with some formula below:\nYoung's Modulus(Y)=Stress/Strain\n=(F/A)/(dl/L) \nwhere, F=force applied, \nA=cross sectional area, \ndl=leangth increase and L=total lenght.\nBulk Modulus(B)\n=dP/(dV/V) \nwhere P=pressure and V=volume.
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Depends what information you already have. The simplest one I can think of is:\n\nVelocity = Acceleration x Time\n\n-Therefore-\n\nAcceleration = Velocity / Time\n\nBut you might have other variables involved here.
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Thermal Properties Conditions \nTemp. (K) Pressure (Pa) \nMelting Temperature  1357.77 K   101325  \nBoiling Temperature  2835.15 K   101325  \nCritical Temperature  8280 K     \nFusion Enthalpy  208.7 J/g 0  101325  \nHeat Capacity  385 J/kg-K 298.15 more...  100000  \nThermal Conductivity 401 W/m-K 300 more...  101325
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a physical property is something you can see or measure.  stuff like temperature, or color.
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You are talking about viscosity of a liquid. In short: as temp goes up, viscosity or resistance goes down (however, this is not true for all liquids).\n\nViscosity is a measure of the resistance of a fluid to deformation under shear stress It is commonly perceived as "thickness", or resistance to pouring. Viscosity describes a fluid resistance to flow and may be thought of as a measure of fluid friction. Thus, methanol is "thin", having a low viscosity, while vegetable oil is "thick" having a high viscosity.\n\nBasically in a liquid you have a bunch of molecules smashing into each other at a certain "speed". The higher the temperature the faster they move around and the more "spread out" they become. Therefore as temperature goes up it becomes easier for things to move through the liquid and vise versa. Of course, this is true for most liquids but not all. See below for a great site that explains more.
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Examples of extensive properties:\n\nMass \nVolume \nEntropy \nEnergy \nElectrical resistance \nTexture \nHeat \n\nAn extensive property of a system depends on the system size or the amount of material in the system. An intensive property on the other hand is a physical property of the system that does not depend on the system size or the amount of material in the system.\n\nHopefully that gives you and idea and you found what you were looking for.
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ALways by sight at first. The most important properties are visual. Eg: colour, roughness, presence of any strange um 'flecks'..... or 'veins'. And then next, scratch something with it and put it into "moe's scale of hardness"
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You could class them as soft solids, since they do not flow. They may be very viscous liquids... but solid is the closest definition.\n\nThe are not truley fluid {which means "gas or liquid" in Physics}, since I can put it in a bowl and it won't coat the bottom.
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Here is a link to a "Polymer Physical Property Comparison Chart."\nhttp://www.lauren.com/Technical_Info/physical_properties.asp
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D = M/V\n\nDensity= Mass/Volume
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go to encarta.msn.com and search for keys mass/solid structure, surface Structure
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Look up Vector Mechanics for Engineers and Scientists.  This deals with basic Newtonian physics as applied to static structures.\n\nBone up on chemistry.  It is easy to forget your chemistry, and as far as I know you will be required to take a few semesters of basic Chem, even if you are not planning on being a Chem Eng.\n\nDo not lose your Maths either!  Grab a pre-calc or a calculus book and keep practicing.
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It doesn't have one. Young's Modulus is a material property relating stress and strain of a solid during elastic deformation. Water is a fluid and fluids don't "deform"; they take the shapes of their containers.