For a small additional carbon mass, logarithmic forcing has derivative inversely proportional to the background atmospheric carbon inventory. With other conversion factors fixed, b0 therefore decreases as background concentration rises. Solve the temperature equation using an integrating factor and the pulse burden:At b1=2k the second term is its continuous limit te−b1t. For 0<k≪b1, temperature initially rises over b1−1 toward roughly b0/b1, then relaxes over (2k)−1 toward half that value. This produces an overshoot, rather than permanent growth. The two numerical limits requested separately below also follow directly from the differential equation.
T(t)=2b0[b11−e−b1t+b1−2ke−2kt−e−b1t].
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