Consider the laminar thermal boundary layer development near the entrance of the tube shown in Figure 8A. When the hydrodynamic boundary layer is thin relative to the tube diameter, the inviscid flow region has a uniform velocity that is approximately equal to the mean velocity. Hence the boundary layer development is similar to what would occur for a flat plate. (a) Beginning with Equation 7.23, derive an expression for the local Nusseltnumber N u D , as a function of the Prandtl number Prand the inverse Graetz number G z D − 1 . Plot the expression using the coordinates shown in Figure 8. 10afor Pr = 0.7 . (b) Beginning with Equation 7.30, derive an expression for the average Nusseltnumber N u ¯ D , as a function of the Prandtl number Pr and the Inverse Graetz number G z D − 1 . Compare your results with the Nussek number for the combined entrancelength in the limit of small x.
Consider the laminar thermal boundary layer development near the entrance of the tube shown in Figure 8A. When the hydrodynamic boundary layer is thin relative to the tube diameter, the inviscid flow region has a uniform velocity that is approximately equal to the mean velocity. Hence the boundary layer development is similar to what would occur for a flat plate. (a) Beginning with Equation 7.23, derive an expression for the local Nusseltnumber N u D , as a function of the Prandtl number Prand the inverse Graetz number G z D − 1 . Plot the expression using the coordinates shown in Figure 8. 10afor Pr = 0.7 . (b) Beginning with Equation 7.30, derive an expression for the average Nusseltnumber N u ¯ D , as a function of the Prandtl number Pr and the Inverse Graetz number G z D − 1 . Compare your results with the Nussek number for the combined entrancelength in the limit of small x.
Solution Summary: The author plots the expression for local Nusselt number as a function of Prandtl number and inverse Graetz number.
Consider the laminar thermal boundary layer development near the entrance of the tube shown in Figure 8A. When the hydrodynamic boundary layer is thin relative to the tube diameter, the inviscid flow region has a uniform velocity that is approximately equal to the mean velocity. Hence the boundary layer development is similar to what would occur for a flat plate. (a) Beginning with Equation 7.23, derive an expression for the local Nusseltnumber
N
u
D
, as a function of the Prandtl number Prand the inverse Graetz number
G
z
D
−
1
. Plot the expression using the coordinates shown in Figure 8.10afor
Pr
=
0.7
. (b) Beginning with Equation 7.30, derive an expression for the average Nusseltnumber
N
u
¯
D
, as a function of the Prandtl number Pr and the Inverse Graetz number
G
z
D
−
1
. Compare your results with the Nussek number for the combined entrancelength in the limit of small x.
An elastic bar of length L = 1m and cross section A = 1cm2 spins with
angular velocity ω about an axis, as shown in the figure below. The
radial acceleration at a generic point x along the bar is a(x) = ω2x,
where ω= 100rad/s is the angular velocity. The bar is pinned on the
rotation axis at x = 0. A mass M = 1kg is attached to the right end of
the bar. Due to the radial acceleration, the bar stretches along x with
displacement function u(x). The displacement u(x) solves the BVP
(strong form) sketched below:
d
dx (σ(x)) + ρa(x) = 0 PDE
σ(x) = E du
dx Hooke’s law
(1)
u(0) =?? essential BC
σ(L) =?? natural BC
where σ(x) is the axial stress in the rod, ρ= 2700kg /m3 is the mass
density, and E = 70GPa is the Young’s modulus
1. Define appropriate BCs for the strong BVP
2. Find the solution of the strong BVP analytically
3. Derive the weak form of the BVP.
Gruebler's formula for the following mechanism?
w/I
- |
العنوان
I need a detailed drawing with explanation
SOLL
эт
4
حكا
The guide vane angle of a reaction turbine (Francis type
make 20° with the tangent. The moving blade angle at entry is
120°. The external diameter of runner is 450 mm and the internal
diameter is 300 mm. Runner width at entry is 62.5mm and at exit
100mm. Calculate the blade angle at exit for radial discharge.
96252
-20125
750 ×2.01
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