| 41. | Over time, the exponential decay acts to distribute the values at these points evenly throughout the entire grid.
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| 42. | In simple cases, an exponential decay is measured which is described by the " T " 2 time.
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| 43. | It is expected that the system will experience exponential decay with time in the temperature of a body.
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| 44. | That is, the change from one filter output to the next is exponential decay seen in the continuous-time system.
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| 45. | This is an exponential decay process that steadily decreases the proportion of the remaining isotope by 50 % every half-life.
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| 46. | This overestimation is visible at distances less than half the Debye length, where the decay is steeper than exponential decay.
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| 47. | As a consequence, in the crystal these states are characterized by an imaginary wavenumber leading to an exponential decay into the bulk.
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| 48. | Prior to wave reflection, they both are characterized by a steep wave front followed by a nearly exponential decay at close distances.
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| 49. | It is expected that the system will experience exponential decay in the temperature difference of body and surroundings as a function of time.
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| 50. | Now compute the number of atoms that are left after one hour using the exponential decay formula slightly above in the same article.
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