COOLING \[=\FRAC{d\theta }{dt}=\] slope of the curve. At \[P,\frac{d\theta }{dt}=\TAN {{\phi }_{2}}=k({{\theta }_{2}}-{{\theta }_{0}})\], where k=constant. At \[Q\frac{d\theta }{dt}=\tan {{\phi }_{1}}=k({{\theta }_{1}}-{{\theta }_{0}})\] \[\Rightarrow \frac{\tan {{\phi }_{2}}}{\tan {{\phi }_{1}}}=\frac{{{\theta }_{2}}-{{\theta }_{0}}}{{{\theta }_{1}}-{{\theta }_{0}}}\]

"> COOLING \[=\FRAC{d\theta }{dt}=\] slope of the curve. At \[P,\frac{d\theta }{dt}=\TAN {{\phi }_{2}}=k({{\theta }_{2}}-{{\theta }_{0}})\], where k=constant. At \[Q\frac{d\theta }{dt}=\tan {{\phi }_{1}}=k({{\theta }_{1}}-{{\theta }_{0}})\] \[\Rightarrow \frac{\tan {{\phi }_{2}}}{\tan {{\phi }_{1}}}=\frac{{{\theta }_{2}}-{{\theta }_{0}}}{{{\theta }_{1}}-{{\theta }_{0}}}\]

">

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 \[{{\phi }_{2\,}}\] and \[{{\phi }_{1}}\], as shown

NEET Physics in NEET 1 year ago

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[b] For \[\theta -t\] plot, rate of COOLING \[=\FRAC{d\theta }{dt}=\] slope of the curve. At \[P,\frac{d\theta }{dt}=\TAN {{\phi }_{2}}=k({{\theta }_{2}}-{{\theta }_{0}})\], where k=constant. At \[Q\frac{d\theta }{dt}=\tan {{\phi }_{1}}=k({{\theta }_{1}}-{{\theta }_{0}})\] \[\Rightarrow \frac{\tan {{\phi }_{2}}}{\tan {{\phi }_{1}}}=\frac{{{\theta }_{2}}-{{\theta }_{0}}}{{{\theta }_{1}}-{{\theta }_{0}}}\]

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