| 1. | Fick's first law is also important in radiation transfer equations.
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| 2. | The extinction coefficient \ alpha can be calculated using the transfer equation.
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| 3. | Substituting this result into the solution to the radiation transfer equation and integrating gives
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| 4. | The molecular transfer equations of Fick's law for mass are very similar.
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| 5. | Substitution of \ theta = 0 gives the explicit discretization of the unsteady conductive heat transfer equation.
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| 6. | A attempt to solve the heat transfer equation in a model of pyrolysis spray using 4q-order m-Boubaker polynomials.
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| 7. | This equation will often depend on temperature, so a heat transfer equation is required or the postulate that heat transfer can be neglected.
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| 8. | The code uses N-stream approximation to the radiative transfer equations ( Stamnes et al . 1988 ) and allows for flexible choice of bands.
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| 9. | A DC bias is applied to the valve to ensure that the part of the transfer equation which is most suitable to the required application is used.
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| 10. | At low excess temperatures, the radiative loss is approximately ? " u ", giving a one-dimensional heat-transfer equation of the form
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