Biot Number Formula:
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The Biot Number is a dimensionless quantity that represents the ratio of internal conduction resistance to surface convection resistance. It's used in heat transfer analysis to determine if a body can be treated with the lumped capacitance method.
The calculator uses the Biot Number formula:
Where:
Explanation: The Biot Number compares the rate of heat transfer at the surface to the rate of heat conduction within the body.
Details: The Biot Number is crucial in heat transfer analysis. When Bi < 0.1, the temperature gradient within the body is negligible, and the lumped capacitance method can be applied. For higher values, spatial temperature variations must be considered.
Tips: Enter all parameters in the specified units. Ensure all values are positive and valid for accurate calculation of the Biot Number.
Q1: What does a Biot Number less than 0.1 indicate?
A: A Biot Number less than 0.1 suggests that the internal resistance to heat conduction is much smaller than the external convection resistance, allowing the use of lumped capacitance method.
Q2: How is the Fourier Number related to Biot Number?
A: The Fourier Number represents dimensionless time, while the Biot Number represents the ratio of internal to external heat transfer resistances. Both are important in transient heat conduction analysis.
Q3: What are typical applications of Biot Number analysis?
A: Biot Number analysis is used in cooling/heating of electronic components, food processing, metallurgical processes, and various engineering applications involving heat transfer.
Q4: Can Biot Number be applied to mass transfer problems?
A: Yes, an analogous Biot Number exists for mass transfer, where it represents the ratio of internal diffusion resistance to external mass transfer resistance.
Q5: What limitations should be considered when using this formula?
A: This formula assumes constant properties and uniform surface conditions. It may not be accurate for complex geometries or when property variations with temperature are significant.