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Transient Hotwire Measurement of
Diamondoid Thermal Conductivity
Esteban Pacheco • Matthew Powell-Palm
Transient Hotwire Raw Data
Iterations of
Experimental Setup
Thermal Conductivity Results
DeltaT[K]
Time [s]
Abstract
Materials of ultralow thermal conductivity have considerable potential as thermal insulators in micro and nanoscale electromechanical systems and as thermoelectric generators. We have developed a
method of experimentally determining the thermal conductivities of powdered crystalline substances at high pressures and low temperatures using a transient hotwire technique. We have successfully
determined the thermal conductivity of the diamondoid adamantane with this method and refined a novel experiemtnal procedure. We have attained good agreement with published values and will
test other diamdoids in the coming future.
λ =
q
4π
dΔT
dln(t)
Motivation Transient Hotwire
Adamantane is the most structurally simple
member the diamondoids. It undergoes a
high-entropy phase change at 208.7 K which
results in an increase in density from 1.08 to 1.18
g/cm3 and a transition from a plastic face
centered cubic to a normal tetratgonal
crystalline structure. It has a notably low room
temperature thermal conductivity of 0.21 W/m-K.
Having validatated our experimental method
with adamantane, we plan next to develop
polycrystalline diamondoid alloys, taking
advantage of unique phonon mismatches to
create substances of ultralow thermal
conductivity.
Theory
Derived from the Heat Conduction
Equation in a Radial Coordinate System
assuming infinite wire length.
Experimental Method
1. Compress powdered adamantane to 80,000 psi, forming single crystal.
2. Drill a tunnel through crystal.
3. Thread platinum wire probe through tunnel.
4. Recompress crystal with 8,000 psi, collapsing tunnel around wire.
5. Cool entire apparatus in cryostat, taking transient hotwire measurements.
180 200 220 240 260 280 300
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Adamantane Thermal Conductivity
Temperature (K)
ThermalConductivity(W/m−K)
Powell−Palm/Pacheco 2015
Powell−Palm/Pacheco 2015
Powell−Palm/Pacheco 2015
Wigren 2011
Cahill−Pohl Lower Limit
1. Horseshoe 2. Cold Finger
3. Pacquiao 4. The Big Break
5. The Main Squeeze

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MotM Poster

  • 1. Transient Hotwire Measurement of Diamondoid Thermal Conductivity Esteban Pacheco • Matthew Powell-Palm Transient Hotwire Raw Data Iterations of Experimental Setup Thermal Conductivity Results DeltaT[K] Time [s] Abstract Materials of ultralow thermal conductivity have considerable potential as thermal insulators in micro and nanoscale electromechanical systems and as thermoelectric generators. We have developed a method of experimentally determining the thermal conductivities of powdered crystalline substances at high pressures and low temperatures using a transient hotwire technique. We have successfully determined the thermal conductivity of the diamondoid adamantane with this method and refined a novel experiemtnal procedure. We have attained good agreement with published values and will test other diamdoids in the coming future. λ = q 4π dΔT dln(t) Motivation Transient Hotwire Adamantane is the most structurally simple member the diamondoids. It undergoes a high-entropy phase change at 208.7 K which results in an increase in density from 1.08 to 1.18 g/cm3 and a transition from a plastic face centered cubic to a normal tetratgonal crystalline structure. It has a notably low room temperature thermal conductivity of 0.21 W/m-K. Having validatated our experimental method with adamantane, we plan next to develop polycrystalline diamondoid alloys, taking advantage of unique phonon mismatches to create substances of ultralow thermal conductivity. Theory Derived from the Heat Conduction Equation in a Radial Coordinate System assuming infinite wire length. Experimental Method 1. Compress powdered adamantane to 80,000 psi, forming single crystal. 2. Drill a tunnel through crystal. 3. Thread platinum wire probe through tunnel. 4. Recompress crystal with 8,000 psi, collapsing tunnel around wire. 5. Cool entire apparatus in cryostat, taking transient hotwire measurements. 180 200 220 240 260 280 300 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 Adamantane Thermal Conductivity Temperature (K) ThermalConductivity(W/m−K) Powell−Palm/Pacheco 2015 Powell−Palm/Pacheco 2015 Powell−Palm/Pacheco 2015 Wigren 2011 Cahill−Pohl Lower Limit 1. Horseshoe 2. Cold Finger 3. Pacquiao 4. The Big Break 5. The Main Squeeze