# Linear Stability Analysis of Thermal Convection in an Infinitely Long Vertical Rectangular Enclosure in the Presence of a Uniform Horizontal Magnetic Field

Authors: Takashi Kitaura; Toshio Tagawa
Journal: Journal of Fluids
 (2014)

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## Abstract

Stability of thermal convection in an infinitely long vertical channel in the presence of a uniform horizontal magnetic field applied in the direction parallel to the hot and cold walls was numerically studied. First, in order to confirm accuracy of the present numerical code, the one-dimensional computations without the effect of magnetic field were computed and they agreed with a previous study quantitatively for various values of the Prandtl number. Then, linear stability analysis for the thermal convection flow in a square horizontal cross section under the magnetic field was carried out for the case of Pr = 0.025. The thermal convection flow was once destabilized at certain low Hartmann numbers, and it was stabilized at high Hartmann numbers.


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## Body

## 1. Introduction

Nuclear fusion energy has received considerable attention as one of the environment-friendly in modern society. Heading towards implementation of the use of nuclear fusion energy, experimental facility called ITER (International Thermonuclear Experimental Reactor) is currently under construction in France. ITER has a toroidal shape like a donut, in which the high-temperature plasma enough to induce nuclear fusion reaction is controlled by both operation of magnetic field generated by the superconducting coils disposed around the plasma and the imposed electric current in the plasma [1]. Blankets located close to the plasma side play an important role for cooling, shielding neutrons, and fuel production.Fusion reactor blanket can be classified into the solid blanket using a solid compound of lithium as fuel production material, or liquid blanket using liquid lithium. Above all, liquid blanket has the advantage of being of relatively simple structure [2], but, on the other hand, it has a serious problem called the MHD pressure loss [3]. The MHD pressure loss obstructs convection of liquid metal as a coolant and it depends on the direction of the magnetic field and the electric conductivity of the wall. To elucidate that problem, researches on thermal convection under the electromagnetic force have been actively conducted not only for the application of fusion reactor blankets but also for crystal growth such as the horizontal Bridgman method.The effect of the direction of uniform magnetic field on the natural convection in a cubic enclosure heated from a vertical wall and cooled from an opposing vertical wall was numerically studied by Ozoe and Okada [5]. They showed that the horizontal magnetic field parallel to the hot and cold walls (Y-directional magnetic field) has much less influence on the damping of natural convection than the two other directions of magnetic field (X- or Z-directional magnetic field). This finding was confirmed with an experiment using 30 mm × 30 mm × 30 mm cubical box filled with molten gallium by Okada and Ozoe [6]. They noticed the heat transfer rate of natural convection under the Y-directional magnetic field indicated not only weak damping of heat transfer rate at high magnetic fields but also slight enhancement of heat transfer rate at low magnetic fields. However, they were not convinced by this enhancement of heat transfer.After several years, Tagawa and Ozoe (1997, 1998) [7, 8] carried out both three-dimensional computations with the higher Rayleigh numbers than those by Ozoe and Okada and the molten gallium experiment using 64 mm × 64 mm × 64 mm cubical box for the Y-directional magnetic field in order to confirm the existence of enhancement of heat transfer rate at low magnetic fields. Due to the exploration of the larger Rayleigh numbers, both the numerical and experimental results showed the enhancement of heat transfer rate (the Nusselt number) when the uniform magnetic field was applied in the Y-direction.The enhancement of Nusselt number in the presence of low magnetic fields has been reported by several other groups. Authié et al. [9] carried out both three-dimensional computations and the corresponding experiment using mercury for the buoyant convection in a long vertical enclosure. Their experiments indicated that the Nusselt number takes its maximum around the Hartmann number 200–250 for the values of the Grashof number from 3
×
10
7 to 1.5
×
10
8. Burr et al. [10] carried out the natural convection for the similar configuration under a horizontal magnetic field perpendicular to both the gravity and the applied heat flux. They showed that the Nusselt numbers increased from the value of natural convection without the magnetic field in the range of the Hartmann number 100
<
Ha
<
225 with a tendency of higher Hartmann numbers at larger heat fluxes. Zhang et al. [11] carried out an experimental study on the flow structure of a bubble-driven liquid-metal jet in a horizontal magnetic field. They concluded that the application of a moderate magnetic field destabilizes the global flow and gives rise to transient, oscillating flow patterns with predominant frequencies. The electric conducting fluid motion is usually damped by the use of static magnetic field. The above-mentioned literatures concern the enhancement of natural convection heat transfer or destabilizing effect of the electric conducting fluid flow at low Hartmann numbers in the presence of static magnetic field. This interesting finding could be related to the flow instability and/or transition.Fujimura and Nagata (1998) [12] studied instability of the natural convection in an infinitely long vertical rectangular channel in the presence of a uniform horizontal magnetic field by two-dimensional analysis. Kakutani (1964) [13] studied the hydromagnetic stability on the plane laminar flow between the parallel plates in the presence of a transverse magnetic field. The plane Couette flow is destabilized by the magnetic field in the range of Hartmann number 3.91
<
Ha
<
5.4.The purpose of this research is to clarify the stability of parallel flow of thermal convection in an infinitely long vertical rectangular channel in the presence of a horizontal magnetic field.


## 2. Numerical Model

The schematic model considered in this study is shown in Figure1. The fluid treated in this research is assumed to be an incompressible Newtonian fluid, and the Boussinesq approximation is employed. The boundary conditions are the no-slip condition for all walls and the heated and cooled walls are isothermal and the other two walls are the thermally insulated. Governing equations are the equations of continuity, the momentum, the energy, Ohm’s law, and the conservation of electric charge. We used a finite difference method with a staggered mesh system. By introducing the time derivative term into the governing equations, we obtain approximated solutions under discretization using a second-order or fourth-order accurate central difference method, together with the use of HS-MAC method for the solution of the Poisson equations of the pressure and the electric potential.Figure 1
Schematic model considered.The instability of the convection of the infinitely long vertical rectangular channel is investigated by using the Grashof number, which is a dimensionless number representing the magnitude of the influence of the inertial and buoyancy forces. Figure2 shows how the flow of a two-dimensional vertical rectangular channel becomes unstable. When the Grashof number exceeds a certain value, the flow structure is divided into a number of cells. In this study, the destabilized flow in the three-dimensional vertical rectangular channel is assumed to be periodic flow in the Z-axis direction, and then we perform the computation with applying a uniform horizontal magnetic field perpendicular to the temperature gradient.Figure 2
An example of destabilization of the thermal convection in a long vertical rectangular channel atPr
=
0.025 and Gr
=
900.0.


## 3. Verification of the Numerical Code

As the verification of the numerical code, preliminary computations were performed for the model of the aspect ratio (h
/
l
→
∞) without magnetic field, and those results were compared with previous results [4]. The present model and the numerical results are described in Figures 3 and 4, respectively. Figure 4 describes the result performed with the number of grids 101 using the discretization of a fourth-order accurate central difference method.Figure 3
Simplified calculation model (A
=
h
/
l
→
∞).Variations of the critical Grashof number and the critical wavenumber for the wide range of the Prandtl number. (a) is referred from a previous study [4] and (b) indicates the present result.
(a)
Reference [4]
(b)
Present resultIt is noted that this graph shows result of the case of the standing wave disturbance. It is known that for the lower Prandtl number(
Pr
<
12.45
) [14], the neutral Grashof number in the case of the standing wave disturbance is lower than that in the case of the traveling wave disturbance. Table 1 shows the numerical results for comparison of the critical Grashof number and the critical wavenumber when air (Pr
=
0.67) and water (Pr
=
7.5) are assumed as test fluids. The agreement between the reference’s result and the present result is negligibly small.Table 1
Comparisons of the critical Grashof number and the critical wavenumber between a reference and the present research atPr
=
0.67 and 7.5.
Method
Reference [4]
Present
Chebyshev polynomials expansion
Fourth-order accurate central difference method with 101 grids
Pr
0.67
7.5
0.67
7.5
k
c
1.40417
1.38334
1.40419
1.38349
G
r
c
503.293
491.900
503.305
491.829


## 4. Dimensionless Equations

The flow instability in a long vertical enclosure in the presence of a magnetic field applied in theY-direction is investigated here. In this study, the destabilized flow is assumed to be periodic and stationary in the Z-axis direction, and then the numerical analyses were performed within a horizontal cross section. Due to the computational resources, we focus on the case that the aspect ratio of the horizontal cross section is unity and the Prandtl number is 0.025, which is a typical value of liquid metals.The dimensionless governing equations are shown below:(1)
∂
V
∂
τ
+
(
V
·
∇
)
V
=
-
∇
P
+
1
Gr
∇
2
V
+
1
Gr
Θ
e
z
+
H
a
2
Gr
J
×
e
B
0
,
∂
Θ
∂
τ
+
V
·
∇
Θ
=
1
GrPr
∇
2
Θ
,
∇
·
V
=
0
,
∇
·
J
=
0
,
J
=
-
∇
Φ
+
V
×
e
B
0
,The dimensionless variables are defined as follows:(2)
τ
=
t
l
2
/
(
Gr
ν
)
,
X
=
x
l
,
V
=
v
Gr
ν
/
l
,
Θ
=
T
-
T
0
Δ
T
,
P
=
p
ρ
0
G
r
2
ν
2
/
l
2
,
J
=
j
Gr
ν
B
0
,
Φ
=
ϕ
Gr
σ
e
ν
B
0
/
l
,
Gr
=
g
β
Δ
T
l
3
ν
2
,
Pr
=
ν
α
,
Ha
=
B
0
l
σ
e
ρ
0
ν
,
A
=
h
l
.Since we limit ourselves to the case that the uniform magnetic field is applied in theY-direction, it holds that e
B
0
=
e
y.


## 5. Basic Flow

First, the flow of the basic state is computed with the assumption that the rectangular enclosure is long enough to neglect recirculation area near the top and the bottom walls. Therefore, the basic state of temperature field is in heat conduction. Since the Prandtl and Grashof numbers are included in the scaling, the dimensionless basic flow is independent of the Grashof and Prandtl numbers. Dimensionless governing equations used in the computation are shown as follows. In this study, the aspect ratio of the horizontal cross section is limited toA
=
h
/
l
=
1:
(3)
∂
2
W
bs
∂
X
2
+
∂
2
W
bs
∂
Y
2
+
Θ
bs
+
H
a
2
J
x
bs
=
0
,
Θ
bs
=
-
X
,
∂
J
x
bs
∂
X
+
∂
J
y
bs
∂
Y
=
0
,
J
x
bs
=
-
∂
Φ
bs
∂
X
-
W
bs
,
J
y
bs
=
-
∂
Φ
bs
∂
Y
.Here, the subscript character bs represents the basic state. The vertical component of velocityW, the streamlines of electric current density Ψ
j, and the electric potential Φ of the basic state at the Hartmann number Ha = 10.0 are depicted in Figure 5.Contour maps of the basic flow atHa
=
10.0: (a) vertical velocity W
bs, (b) stream line of electric current Ψ
J, and (c) electric potential Φ
bs.
(a)
(b)
(c)


## 6. Linear Stability Analysis

Disturbance equations are derived for investigating the flow instability. First of all, velocity, pressure, temperature, electric potential, and electric current density are represented with the sum of the solution of the basic state and the infinitesimal disturbances [15]:
(4)
v
=
v
bs
+
v
′
,
p
=
p
bs
+
p
′
,
T
=
T
bs
+
T
′
,
ϕ
=
ϕ
bs
+
ϕ
′
,
j
=
j
bs
+
j
′
.We assume that the infinitesimal disturbances are represented by the normal mode as follows:(5)
(
v
′
,
p
′
,
T
′
,
ϕ
′
,
j
′
)
=
(
v
~
,
p
~
,
T
~
,
ϕ
~
,
j
~
)
exp
⁡
(
i
a
z
+
λ
t
)
.Note thati is the imaginary unit, λ is the complex growth rate which is a complex number, and a is the wavenumber which is a real number here. The dimensionless equations obtained by substituting (4) and (5) to (1) are shown below. It is known that the natural convection flow in a vertical slot becomes unstable for standing wave disturbance rather than for travelling wave disturbance in the range of Pr
<
12.45 [14]. Therefore, we assumed that the neutral stable state of the flow of Pr
=
0.025 is taken as λ
=
0:
(6)
∂
U
~
∂
X
+
∂
V
~
∂
Y
+
i
k
W
~
=
0
,
i
W
bs
k
U
~
=
-
∂
P
~
∂
X
+
1
Gr
(
∂
2
∂
X
2
+
∂
2
∂
Y
2
-
k
2
)
U
~
+
H
a
2
Gr
(
-
J
~
z
)
,
i
W
bs
k
V
~
=
-
∂
P
~
∂
Y
+
1
Gr
(
∂
2
∂
X
2
+
∂
2
∂
Y
2
-
k
2
)
V
~
,
U
~
∂
W
bs
∂
X
+
V
~
∂
W
bs
∂
Y
+
i
W
bs
k
W
~
=
-
i
k
P
~
+
1
Gr
(
∂
2
∂
X
2
+
∂
2
∂
Y
2
-
k
2
)
W
~
+
1
Gr
Θ
~
+
H
a
2
Gr
J
~
x
,
∂
J
~
x
∂
X
+
∂
J
~
y
∂
Y
+
i
k
J
~
z
=
0
,
J
~
x
=
-
∂
Φ
~
∂
X
-
W
~
,
J
~
y
=
-
∂
Φ
~
∂
Y
,
J
~
z
=
-
i
k
Φ
~
+
U
~
.Table2 shows variation of the critical Grashof number on the number of grids at the dimensionless wavenumber k
=
0.83 and Hartmann number Ha
=
5.0 when discretized with a second-order or a fourth-order accurate central difference. Considering the result of Table 2 and the computational time, we employed 7
0
×
7
0 mesh number with the second-order accurate central difference. For example, the neutral stability curve of the Grashof number at Hartmann number Ha
=
10.0 is depicted in Figure 6. The critical Grashof numbers at the wavenumber 0.821 with mesh size 70
×
70, 90
×
90 and 120
×
120 take the value of 3101, 3109, and 3114, respectively. So the dependency of the mesh size on the result is not so significant.Table 2
Variation of the neutral Grashof number for several cases of number of grids atPr
=
0.025, k
=
0.83, and Ha
=
5.0.
Number of meshes
Gr
2nd-order
4th-order
30 × 30
2280.63
2191.22
50 × 50
2177.64
2152.50
70 × 70
2153.61
2142.76Figure 6
Neutral stability curve of the Grashof number atPr
=
0.025 and Ha
=
10.0.Characteristic functions for various variables at a neutral state are illustrated in Figure7. The pressure and the potential distribution have point symmetry and have reverse sign between the real and the imaginary parts with respect to X
=
0 and Y
=
0. On the other hand, the velocity, temperature, and electric current density distribution have point symmetry with respect to X
=
0 and Y
=
0.Contour maps of the characteristic function at a marginal state atPr
=
0.025, k
=
0.83, Gr
=
2152.5, and Ha
=
5.0: (a) real part of U
~, (b) imaginary part of U
~, (c) real part of V
~, (d) imaginary part of V
~, (e) real part of W
~, (f) imaginary part of W
~, (g) real part of P
~, (h) imaginary part of P
~, (i) real part of Θ
~, (j) imaginary part of Θ
~, (k) real part of J
x
~, (l) imaginary part of J
x
~, (m) real part of J
y
~, (n) imaginary part of J
y
~, (o) real part of J
z
~, (p) imaginary part of J
z
~, (q) real part of Φ
~, and (r) imaginary part of Φ
~.
(a)
(b)
(c)
(d)
(e)
(f)
(g)
(h)
(i)
(j)
(k)
(l)
(m)
(n)
(o)
(p)
(q)
(r)The critical Grashof number and the wavenumber plotted against the Hartmann number up to 12 are shown in Figure8. Concerning the application of a horizontal Bridgeman crystal growth, Lyubimov et al. [16] studied the stability of thermal convection in a rectangular cross section of an oblong channel. They studied two cases of computation, the magnetic field applied in the horizontal direction or in the vertical direction with changing the Prandtl number and the aspect ratio of cross section. It should be noted that the present study could be compared with the study of Lyubimov et al. at the case of zero value of Prandtl number (Pr
=
0). In the configuration of horizontal Bridgeman crystal growth, the plane-parallel flow does not exist in nonzero values of Prandtl number, but in the present study the plane-parallel flow always exists irrespective of Prandtl number since the basic thermal state is independent of Prandtl number. According to the results of horizontal magnetic field by Lyubimov et al., the critical Grashof number takes its minimum at a certain low Hartmann number and the critical wavenumber takes its maximum at another low Hartmann number. This tendency is quite coincident with the finding of the present study. This indicates that a moderate magnetic field destabilizes the natural convection of plane-parallel flow but a strong magnetic field stabilizes the convection.Figure 8
Variation of the critical Grashof number and the critical wavenumber against the Hartmann number atPr
=
0.025.


## 7. Conclusion

In this study, we studied the linear stability of thermal convection in an infinitely long vertical rectangular channel in the presence of a uniform horizontal magnetic field. We obtained some findings. First, the characteristic function of the pressure and the electric potential distribution have point symmetry and have reverse sign between the real and the imaginary parts with respect to the center of cross section. On the other hand, the velocity, temperature, and electric current density distribution have point symmetry with respect to the center of cross section. Second, except in the range of the Hartmann number of0
<
Ha
<
8, increase in the Hartmann number leads to well stabilization. And the critical Grashof number takes a minimum value at the Hartmann number of about Ha
=
4
.
5. Third, the critical wavenumber increases at a low Hartmann number but then decreases for further increase in the Hartmann number.



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*Source: 642042-2014-04-29.xml*