A body cools in a surrounding which is at a constant temperature of ${\theta _0}$. Assume that it obeys Newton's law of cooling. Its temperature $\theta $ is plotted against time $t$ . Tangents are drawn to the curve at the points $P(\theta = {\theta _1})$ and $Q(\theta = {\theta _2})$. These tangents meet the time axis at angles of ${\varphi _2}$and ${\varphi _1}$, as shown
  • A$\frac{{\tan \,{\varphi _2}}}{{\tan \,{\varphi _1}}} = \frac{{{\theta _1} - {\theta _0}}}{{{\theta _2} - {\theta _0}}}$
  • B$\frac{{\tan \,{\varphi _2}}}{{\tan \,{\varphi _1}}} = \frac{{{\theta _2} - {\theta _0}}}{{{\theta _1} - {\theta _0}}}$
  • C$\frac{{\tan \,{\varphi _1}}}{{\tan \,{\varphi _2}}} = \frac{{{\theta _1}}}{{{\theta _2}}}$
  • D$\frac{{\tan \,{\varphi _1}}}{{\tan \,{\varphi _2}}} = \frac{{{\theta _2}}}{{{\theta _1}}}$
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