Abstract
The results of experiments investigating the exponential dependence of the vapor bubble radius on time at saturated boiling are generalized. Three different methods to obtain this dependence are suggested: (1) by the application of the transient heat conduction equation, (2) by using the correlations of energy conservation, and (3) by solving a similar electrodynamic problem. Based on the known experimental data, the accuracy of the dependence up to one percent and a few percent accuracy of its description based on the sound pressure generated by a vapor bubble have been determined. A significant divergence of the power dependence of the vapor bubble radius on time (with an exponent of 1/2) with the experimental results and its inadequacy for the description of the sound pulse generated by the bubble have been demonstrated.
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Abbreviations
- a′:
-
Temperature diffusivity of the fluid (m2/s)
- b :
-
Numerical coefficient
- c′:
-
Specific heat of the fluid [J/(kg K)]
- C :
-
Capacitance (F)
- \(C_{*}\) :
-
Heat capacity of the superheated fluid layer (J/K)
- f(t):
-
Time function
- g :
-
Electrical conductivity (Cm)
- \(g_{*}\) :
-
Thermal conductivity (W/K)
- J S :
-
Jacob similarity parameter
- k :
-
Exponent of power dependence
- K :
-
Proportionality factor of power dependence
- l * :
-
Parameter of thermal conductivity, m
- L :
-
Specific heat of vaporization (J/kg)
- m′:
-
Mass of the superheated fluid layer (kg)
- n :
-
Exponent of power dependence
- p :
-
Sound pressure (Pa)
- P m :
-
Maximum sound pressure (Pa)
- q :
-
Heat flow density (W/m2)
- q 0 :
-
The initial density of heat flow (W/m2)
- q e :
-
Electric charge (C)
- q e0 :
-
Initial electric charge (C)
- r :
-
Distance between the vapor bubble center and the point of sound pressure determination (m)
- R :
-
Radius of the vapor bubble (m)
- R * :
-
Parameter of exponential dependence (m)
- R e :
-
Electrical resistance (Ω)
- S :
-
Interphase surface of the bubble (m2)
- T :
-
Time (s)
- T :
-
Average temperature of the superheated fluid layer (K)
- T S :
-
Saturation temperature (K)
- U :
-
Voltage (V)
- V :
-
Volume of the bubble (m3)
- V′ :
-
Volume of superheated liquid layer (m3)
- X :
-
Relative radius of the bubble
- Y :
-
Relative growth rate of the bubble
- Z :
-
Relative acceleration during the growth of the bubble
- α :
-
Heat transfer coefficient [W/(m K)]
- ±δ :
-
Discrepancy between the theory and the experiment (%)
- ε :
-
Constant (1/m)
- θ :
-
Average superheat of the superheated fluid layer (K)
- θ 0 :
-
Initial superheat of the superheated fluid layer (K)
- λ′ :
-
Thermal conductivity of the fluid [W/(m K)]
- ρ′:
-
Fluid density (kg/m3)
- ρ′′:
-
Vapor density (kg/m3)
- τ :
-
Time constant of circuit (s)
- \(\tau_{*}\) :
-
Time constant of the exponential growth of the vapor bubble (s)
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Dorofeev, B.M., Volkova, V.I. Dynamics of vapor bubbles growth at boiling resulting from enthalpy excess of the surrounding superheated liquid and sound pulses generated by bubbles. Heat Mass Transfer 52, 39–45 (2016). https://doi.org/10.1007/s00231-015-1698-9
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DOI: https://doi.org/10.1007/s00231-015-1698-9