When an object moves through a fluid, the fluid exerts a viscous force F on the object that tends to slow it down. For a small sphere of radius R, moving slowly with a speed v, the magnitude of the viscous force is given by Stokes, law, F = 6πηRv, where η is the viscosity of the fluid. (a) What is the viscous force on a sphere of radius R = 8.9 x 10-4 m falling through water (η = 1.00 x 10-3 Pa·s) when the sphere has a speed of 3.9 m/s? (b) The speed of the falling sphere increases until the viscous force balances the weight of the sphere. Thereafter, no net force acts on the sphere, and it falls with a constant speed called the "terminal speed." If the sphere has a mass of 1.5 x 10-5 kg, what is its terminal speed?
When an object moves through a fluid, the fluid exerts a viscous force F on the...
with A small particle of radius R and density p, moving at speed vin a viscous fluid of density dynamic viscosity n experiences a drag force given by Stokes' law F= 69Rv Find an expression for the terminal velocity of the particle as it falls through the fluid under the influence of gravity which includes Pp, pg, R, and n.
A small sphere of mass 9.20 10-5 kg and radius 7.40 10-4 m falls through a fluid of viscosity 0.36 kg/(m · s). Assume that the viscous force (or drag force) is given by Stokes' Law. (a) Calculate the viscous force (in N) when the sphere has a speed of 2.1 cm/s. (b) What is the terminal speed (in cm/s) of the sphere? cm/s
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c. When a spherical object of radius r moves at velocity v in a viscous liquid, the object experi- ences a drag force given by Stokes' Law (Fd = 6πrv. η). Given the apparent weight of the object above, under what condition would the object be falling at "terminal velocity"? State the equation for this...
The average velocity < v > of a viscous fluid through a pipe is proportional to the drop in pressure ∆P, length L, radius of the pipe r, and viscosity of the fluid η (units: kg/m/s). Performing various experiments it has been determined that the velocity is directly proportional to the drop in pressure divided by the length. Determine the dependence of < v > on these quantities.
As an object moves slowly through a viscid fluid, the drag force on the object is proportional to its Group of answer choices speed squared. speed. acceleration. acceleration squared.
A stainless steel ball (radius rsphere = 0.3175 cm, density ρsphere = 7.866 g/cm3) falls through a viscous fluid (density ρfluid = 1.2 g/cm3) and quickly reaches terminal speed v. You measure the ball’s position as a function of time to find v. The ball is at positions y = 10 cm at time 2.402 and at position y = 5 cm at time 3.26. Calculate the viscosity η of the fluid in units of poise = g/(cm-s), using your...
Any object moving in a fluid experiences a drag or viscous force opposing its motion. Assume the object is spherical and the flow around it is laminar. For an object of radius 0.25m moving in honey at 70F (viscosity 20 Pa.s), what is the drag force at a speed of 0.1 m/s? If the object is moving horizontally and at the same constant speed of 0.1 m/s, a force must be exerted on it to maintain that motion. That means...
2. For "sufficiently large" objects moving "sufficiently fast" through a fluid (i.e. for large Reynolds numbers), the drag force on the object is proportional to the square of its ve- locity (quadratic drag). In this limit, we can ignore viscosity and argue this dependence from kinetic considerations. (a) (2 points) Suppose a sphere of radius R moves with speed v through a fluid with mass density ρ. In a small time interval dt, what is the mass m of fluid...
The drag force F acting on a spherical particle of diameter D falling slowly through a viscous fluid at velocity u is found to be influenced by the diameter D, velocity of fall u, and the viscosity . Using the method of dimensional analysis obtain a relationship between the variables. Number of variables is a. (5) Ob. (6) c. (7) d. None of the above Number of the dimensions is e. (3) f. (4) g. (5) Number of the groups...
A body falling in a relatively dense fluid, oil for example, is
acted on by three forces (see Figure 2.3.5): a resistive force R, a
buoyant force B, and its weight w due to gravity. The buoyant force
is equal to the weight of the fluid displaced by the object. For a
slowly moving spherical body of radius a, the resistive force is
given by Stokes's law, R = 6*pi*u*a*|v|, where v is the velocity of
the body, and u...