1958The Physics of FluidsRequires access

Experimental Study of the Method of Bubble Formation in Bubble Chambers

W. I. Goldburg

Open publisher page 2 citations

Abstract

To help put a lower limit on the sensitive time of organic liquids commonly used in bubble chambers a static electric field of 15 kv/cm was applied across a small propane bubble chamber which was then expanded in the conventional manner when a beam of 450 Mev protons was passed through it. The bubble density along the tracks was measured with both field on and field off. Within statistics (±4%) no difference in bubble density was observed for the two cases. To interpret this result it is assumed that δ rays produce bubbles if they deposit a certain minimum amount of energy within a critical volume of the liquid. It is then concluded from this experiment that either recombination effects are not important in bubble formation or that the recombination time of ions in a critical volume of propane is ≲ 10−11 sec. This figure appears to represent a reasonable theoretical estimate of the sensitive time of propane, liquid hydrogen, and liquid helium.

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What this paper is about

To help put a lower limit on the sensitive time of organic liquids commonly used in bubble chambers a static electric field of 15 kv/cm was applied across a small propane bubble chamber which was then expanded in the conventional manner when a beam of 450 Mev protons was passed through it. The bubble density along the tracks was measured with both field on and field off. Within statistics (±4%) no difference in bubble density was observed for the two cases. To interpret this result it is assumed that δ rays produce bubbles if they deposit a certain minimum amount of energy within a critical volume of the liquid. It is then concluded from this experiment that either recombination effects are not important in bubble formation or that the recombination time of ions in a critical volume of propane is ≲ 10−11 sec. This figure appears to represent a reasonable theoretical estimate of the sensitive time of propane, liquid hydrogen, and liquid helium.

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Available abstract

To help put a lower limit on the sensitive time of organic liquids commonly used in bubble chambers a static electric field of 15 kv/cm was applied across a small propane bubble chamber which was then expanded in the conventional manner when a beam of 450 Mev protons was passed through it. The bubble density along the tracks was measured with both field on and field off. Within statistics (±4%) no difference in bubble density was observed for the two cases. To interpret this result it is assumed that δ rays produce bubbles if they deposit a certain minimum amount of energy within a critical volume of the liquid. It is then concluded from this experiment that either recombination effects are not important in bubble formation or that the recombination time of ions in a critical volume of propane is ≲ 10−11 sec. This figure appears to represent a reasonable theoretical estimate of the sensitive time of propane, liquid hydrogen, and liquid helium.

Key concepts: Bubble, Bubble chamber, Propane, Volume (thermodynamics), Liquid bubble, Helium, Electric field, Number density

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