1992
DOI: 10.1007/bf00761628
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Toward a theory of self-disposal of high-level waste

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“…The condition for self-sinking of the capsule as a result of melting through the surrounding rock is where χ is the thermal conductivity, W/(m·K); T m is the melting temperature; and T r is the temperature of the rock, K. Capsules with a specific power of heat release less than the threshold q th do not melt the surrounding rock and, consequently, remain stationary. According to [11], motion of the capsule in fissured rock is possible if the surface temperature of the capsule is higher than the melting temperature by some threshold value. This effect can be taken into account by an appropriate correction to the melting temperature T m .…”
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“…The condition for self-sinking of the capsule as a result of melting through the surrounding rock is where χ is the thermal conductivity, W/(m·K); T m is the melting temperature; and T r is the temperature of the rock, K. Capsules with a specific power of heat release less than the threshold q th do not melt the surrounding rock and, consequently, remain stationary. According to [11], motion of the capsule in fissured rock is possible if the surface temperature of the capsule is higher than the melting temperature by some threshold value. This effect can be taken into account by an appropriate correction to the melting temperature T m .…”
mentioning
confidence: 99%
“…Consequently, the time of motion of the capsule is (for t > τ the capsule can no longer melt the rock in its path and remains stationary in the rock). The velocity at which the capsule sinks can be estimated analytically for a capsule with isothermal sources for small Stefan numbers, i.e., in a typical case of not very rapid sinking [10,11]:…”
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