A nanolaminated material is fabricated with an atomic layer deposition process, resulting in a series of stacked, alternating layers of tungsten and aluminumoxide, each layer being δ = 0.5 nm thick. Each tungsten-aluminum oxide interface is associated with a thermal resistance of R t , i n = 3.85 × 10 − 9 m 2 ⋅ K/W . The theoretical values of the thermal conductivities of the thin aluminum oxide and tungsten layers are k A = 1.65 W/m ⋅ K and k T = 6.10 W/m ⋅ K, respectively. The properties are evaluated at T = 300 K . Determine the effective thermal conductivity of the nanolaminated material. Compare the value ofthe effective thermal conductivity to the bulk thermal conductivities of aluminum oxide and tungsten,given in Tables A.1 and A.2. Determine the effective thermal conductivity of the nanolaminated material assuming that thethermal conductivities of the tungsten and aluminum oxide layers are equal to their bulk values.
A nanolaminated material is fabricated with an atomic layer deposition process, resulting in a series of stacked, alternating layers of tungsten and aluminumoxide, each layer being δ = 0.5 nm thick. Each tungsten-aluminum oxide interface is associated with a thermal resistance of R t , i n = 3.85 × 10 − 9 m 2 ⋅ K/W . The theoretical values of the thermal conductivities of the thin aluminum oxide and tungsten layers are k A = 1.65 W/m ⋅ K and k T = 6.10 W/m ⋅ K, respectively. The properties are evaluated at T = 300 K . Determine the effective thermal conductivity of the nanolaminated material. Compare the value ofthe effective thermal conductivity to the bulk thermal conductivities of aluminum oxide and tungsten,given in Tables A.1 and A.2. Determine the effective thermal conductivity of the nanolaminated material assuming that thethermal conductivities of the tungsten and aluminum oxide layers are equal to their bulk values.
Solution Summary: The author explains the effective thermal conductivity of the nanolaminated material.
A nanolaminated material is fabricated with an atomic layer deposition process, resulting in a series of stacked, alternating layers of tungsten and aluminumoxide, each layer being
δ
=
0.5
nm
thick. Each tungsten-aluminum oxide interface is associated with a thermal resistance of
R
t
,
i
n
=
3.85
×
10
−
9
m
2
⋅
K/W
.
The theoretical values of the thermal conductivities of the thin aluminum oxide and tungsten layers are
k
A
=
1.65
W/m
⋅
K
and
k
T
=
6.10
W/m
⋅
K,
respectively. The properties are evaluated at
T
=
300
K
.
Determine the effective thermal conductivity of the nanolaminated material. Compare the value ofthe effective thermal conductivity to the bulk thermal conductivities of aluminum oxide and tungsten,given in Tables A.1 and A.2.
Determine the effective thermal conductivity of the nanolaminated material assuming that thethermal conductivities of the tungsten and aluminum oxide layers are equal to their bulk values.
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