Abstract
A unique experimental set-up was fabricated to carry out axial heat flow steady state experiments for the assessment of thermal contact conductance (TCC) at the interface of two materials. Three different materials (copper, brass and stainless steel) were selected for the experiments considering their mechanical and thermal properties. Heat transfer experiments were performed in vacuum environment (0.045 torr) to find out solid spot contact conductance for nominally flat surfaces with different surface roughness (1–5 μm) for each specimen under several load conditions (0.6–15 MPa). A precise estimation of TCC for the interface of sets of similar materials was one of the most important results of this research. The effects of the surface roughness, the material properties and the load conditions (nominal interface pressure) have been studied and documented. Furthermore, the experimental results of solid spot contact conductance were compared with four theoretical models, showing their limitations to make a precise estimation of the TCC in the range of the used parameters.
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Abbreviations
- A :
-
Nominal contact area
- A r :
-
Real contact area
- E :
-
Modulus of elasticity
- E′:
-
Reduced modulus of elasticity, \(E^{\prime } = \left[ {\left( {\left( {1 - \nu_{1}^{2} } \right)/E_{1} } \right) + \left( {\left( {1 - \nu_{2}^{2} } \right)/E_{2} } \right)} \right]^{ - 1}\)
- h c :
-
Solid spot conductance
- \(\bar{h}_{c}\) :
-
Normalized solid spot contact conductance, \(\bar{h}_{c} = {{\left( {h_{c} R_{q} } \right)} \mathord{\left/ {\vphantom {{\left( {h_{c} R_{q} } \right)} {\left( {mk} \right)}}} \right. \kern-0pt} {\left( {mk} \right)}}\)
- h g :
-
Gap conductance
- h j :
-
Joint thermal contact conductance
- h r :
-
Radiation heat transfer coefficient
- ΔT :
-
Temperature drop across the interface
- H :
-
Vickers hardness
- k :
-
Effective thermal conductivity, \(k = 2k_{1} k_{2} /\left( {k_{1} + k_{2} } \right)\)
- m :
-
Effective arithmetic average slope, \(m = \sqrt {\left( {m_{1}^{2} + m_{2}^{2} } \right)}\)
- \(\bar{P}\) :
-
Normalized pressure, \(\bar{P} = {P \mathord{\left/ {\vphantom {P H}} \right. \kern-0pt} H}\)
- P :
-
Applied pressure
- Q :
-
Heat flow rate
- R q :
-
Effective root mean square roughness, \(R_{q} = \sqrt {\left( {R_{q1}^{2} + R_{q2}^{2} } \right)}\)
- \(U_{{Q_{1} }} ,U_{{Q_{2} }}\) :
-
Uncertainties in the estimation of heat fluxes, Q 1 and Q 2
- ν :
-
Poisson’s ratio
- ɛ :
-
Emissivity
- 1:
-
Specimen 1
- 2:
-
Specimen 2
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Acknowledgments
The authors acknowledge the financial support of the Bhabha Atomic Research Centre (BARC), India for initiating this research activity in Mechanical & Industrial Engineering Department at Indian Institute of Technology Roorkee, India.
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Tariq, A., Asif, M. Experimental investigation of thermal contact conductance for nominally flat metallic contact. Heat Mass Transfer 52, 291–307 (2016). https://doi.org/10.1007/s00231-015-1551-1
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DOI: https://doi.org/10.1007/s00231-015-1551-1