Consider fully developed pressure-driven flow in a cylindrical tube of radius, R , and length, L = 10 mm, with flow generated by an applied pressure gradient, Δ p . Tests are performed with room temperature water for various values of R , with a fixed flow rate of Q =10 μ L/min. The hydraulic resistance is defined as R hyd = Δ p / Q (by analogy with the electrical resistance R elec = Δ V / I , where Δ V is the electrical potential drop and l is the electric current). Calculate the required pressure gradient and hydraulic resistance for the range of tube radii listed in the table. Based on the results, is it appropriate to use a pressure gradient to pump fluids in microchannels, or should some other driving mechanism be used?
Consider fully developed pressure-driven flow in a cylindrical tube of radius, R , and length, L = 10 mm, with flow generated by an applied pressure gradient, Δ p . Tests are performed with room temperature water for various values of R , with a fixed flow rate of Q =10 μ L/min. The hydraulic resistance is defined as R hyd = Δ p / Q (by analogy with the electrical resistance R elec = Δ V / I , where Δ V is the electrical potential drop and l is the electric current). Calculate the required pressure gradient and hydraulic resistance for the range of tube radii listed in the table. Based on the results, is it appropriate to use a pressure gradient to pump fluids in microchannels, or should some other driving mechanism be used?
Consider fully developed pressure-driven flow in a cylindrical tube of radius, R, and length, L= 10 mm, with flow generated by an applied pressure gradient, Δp. Tests are performed with room temperature water for various values of R, with a fixed flow rate of Q =10 μL/min. The hydraulic resistance is defined as Rhyd = Δp/Q (by analogy with the electrical resistance Relec = ΔV/I, where ΔV is the electrical potential drop and l is the electric current). Calculate the required pressure gradient and hydraulic resistance for the range of tube radii listed in the table. Based on the results, is it appropriate to use a pressure gradient to pump fluids in microchannels, or should some other driving mechanism be used?
Branch of science that deals with the stationary and moving bodies under the influence of forces.
The 2-mass system shown below depicts a disk which rotates about its center and has rotational
moment of inertia Jo and radius r. The angular displacement of the disk is given by 0. The spring
with constant k₂ is attached to the disk at a distance from the center. The mass m has linear
displacement & and is subject to an external force u. When the system is at equilibrium, the spring
forces due to k₁ and k₂ are zero. Neglect gravity and aerodynamic drag in this problem. You may
assume the small angle approximation which implies (i) that the springs and dampers remain in
their horizontal / vertical configurations and (ii) that the linear displacement d of a point on the
edge of the disk can be approximated by d≈re.
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K2
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m
4
Cz
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Jo
Make the following assumptions when analyzing the forces and torques:
тв
2
0>0, 0>0, x> > 0, >0
Derive the differential equations of motion for this dynamic system. Start by sketching
LARGE and carefully drawn free-body-diagrams for the disk and the…
A linear system is one that satisfies the principle of superposition. In other words, if an input u₁
yields the output y₁, and an input u2 yields the output y2, the system is said to be linear if a com-
bination of the inputs u = u₁ + u2 yield the sum of the outputs y = y1 + y2.
Using this fact, determine the output y(t) of the following linear system:
given the input:
P(s) =
=
Y(s)
U(s)
=
s+1
s+10
u(t) = e−2+ sin(t)
=e
The manometer fluid in the figure given below is mercury where D = 3 in and h = 1 in. Estimate the volume flow in the tube (ft3/s) if the flowing fluid is gasoline at 20°C and 1 atm. The density of mercury and gasoline are 26.34 slug/ft3 and 1.32 slug/ft3 respectively. The gravitational force is 32.2 ft/s2.
Chapter 8 Solutions
Fox And Mcdonald's Introduction To Fluid Mechanics
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8.01x - Lect 27 - Fluid Mechanics, Hydrostatics, Pascal's Principle, Atmosph. Pressure; Author: Lectures by Walter Lewin. They will make you ♥ Physics.;https://www.youtube.com/watch?v=O_HQklhIlwQ;License: Standard YouTube License, CC-BY