r_{LS} = r_{RS} = 0.01s | r_{LS} = r_{RS} = 0.05s | r_{LS} = r_{RS} = 0.1s | ||||
---|---|---|---|---|---|---|

t | Exact | Equation 33 | Exact | Equation 33 | Exact | Equation 33 |

0 | 2.42 | 2.42 | 2.42 | 2.42 | 2.42 | 2.42 |

500 | 2.21 | 2.21 | 1.48 | 1.48 | 0.90 | 0.90 |

1000 | 2.18 | 2.18 | 0.98 | 0.98 | 0.36 | 0.36 |

1500 | 3.67 | 3.70 | 1.11 | 1.12 | 0.25 | 0.25 |

2000 | 6.91 | 6.89 | 1.39 | 1.39 | 0.19 | 0.19 |

2500 | 1.59 | 1.53 | 0.21 | 0.21 | 0.02 | 0.02 |

3000 | 0.14 | 0.13 | 0.01 | 0.01 | 0.00 | 0.00 |

3500 | 0.01 | 0.01 | 0.00 | 0.00 | 0.00 | 0.00 |

3982 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 |

The values shown are in units of 10

^{−2}. We used*s*= 0.01,*p*_{S}(0) = 0.00005,*p*_{L}(0) = 0.38,*p*_{R}(0) = 0.41, and*C*_{LR}(0) = 0.0242. In the exact numerical computation,*p*_{S}(*t*) = 1 –*p*_{S}(0) at*t*= 3982.