Discuss Newton's second law (the linear momentum rela- tion) in these three forms: Σr-mΣr- (mV) na dt Er -_Vpav) Vpdv) 'system Are they all equally valid? Are they equivalent? Are some forms better for fluid mechanics as opposed to solid mechanics?
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- Consider a two-dimensional flow which varies in time and is defined by the velocity field, u = 1 and v = 2yt. Given that the density of the fluid does not vary spatially and changes only with time, what differential equa9on for the density, ⍴(t), must be satisfied for this scenario to represent a physical, compressible flow field?Consider the steady, two-dimensional, incompressible velocity field, V-› = (u, ?)=(ax + b) i-› + (−ay + c) j-›, where a, b, and c are constants. Calculate the pressure as a function of x and y.Consider the steady, two-dimensional velocity field given by V-› = (u, ?) = (1.6 + 2.8x) i-› + (1.5 − 2.8y) j-›. Verify that this flow field is incompressible.
- Consider the following steady, two-dimensional velocity field: V-›= (u, ? ) = (a2 − (b − cx)2) i-›+ (−2cby + 2c2xy) j-›Is there a stagnation point in this flow field? If so, where is it?Define variable flow? Also discuss the forces encoundered in fluid mechanics?A curved blood vessel has an internal diameter ? = 5 mm and a radius of curvature of ?? = 17 mm. Blood has a density of ρ = 1060 kg/m3 and a viscosity of 3.5 cP, and travels at an average velocity of ? = 1 m/s. a) Comment on the nature of the flow with reference to relevant non-dimensional groups. b) Can the flow be modelled using the Hagen-Poisseuile equation? If not, explain what specific assumptions are invalid. c) The viscosity of blood is measured and is shown in Figure Q2. Consider two long straight blood vessels with steady flow. The diameter of the first vessel is 5 mm and the average velocity is 6 cm/s. The internal diameter of the second vessel is 2.2 mm and the average velocity is 50 cm/s. Which vessel would you expect the Hagen-Poisseiulle equation to be more accurate in? Explain your answer (1-2 sentences).
- Consider the two-dimensional incompressible velocity potentialϕ = xy + x 2 - y 2 . ( a ) Is it true that = ∆2 ϕ = 0, and, ifso, what does this mean? ( b ) If it exists, fi nd the streamfunction ψ ( x , y ) of this fl ow. ( c ) Find the equation of thestreamline that passes through ( x , y ) = (2, 1).Water flows through a two-dimensional narrowing wedgeat 9.96 gal/min per meter of width into the paper(Fig. P4.72). If this inward flow is purely radial, find anexpression, in SI units, for ( a ) the stream function and( b ) the velocity potential of the flow. Assume onedimensionalflow. The included angle of the wedge is 45 ° .Consider a steady velocity field given by V-› = (u, ?, w) = a(x2y + y2)i→ + bxy2 j→ + cxk→, where a, b, and c are constants. Under what conditions is this flow field incompressible?
- Hint: take partial derivatives of the given shallow water equations and subtract them, e.g. d(eq2)/dx - d(eq1)/dy, and look for bits that make up vorticity, vorticity advection and divergenceDefine and briefly explain the_terms listed below, support your elaboration with mathematicalequations and illustrations where necessary:1. Viscous flow, inviscid flow, compressible and incompressible flow2. Laminar flow, tubulent flow, steady and unsteady tlow3. Reynolds number and Mach number4. VIScOSty, specific gravity, specitic densityBuoyancy., centre of gravity and center of pressure. Bemoulli's equationImagine a steady, two-dimensional, incompressible flow that is purely circular in the xy- or r?-plane. In other words, velocity component u? is nonzero, but ur is zero everywhere. What is the most general form of velocity component u? that does not violate conservation of mass?