Answer:
According to the
law of conservation of angular momentum
\[{{I}_{1}}{{\omega
}_{1}}\,={{I}_{2}}{{\omega }_{2}}\]
or \[\frac{2}{5}\,\,MR_{p}^{2}\,{{\omega
}_{p}}=\,\frac{2}{5}\,MR_{a}^{2}\,{{\omega }_{a}}\]
or \[R_{p}^{2}{{\omega
}_{p}}=\,R_{a}^{2}{{\omega }_{a}}\] or \[\frac{{{\omega }_{p}}}{{{\omega
}_{a}}}\,\,=\,{{\left( \frac{{{R}_{a}}}{{{R}_{p}}} \right)}^{2}}\] ? (i)
Now
\[{{R}_{p}}=a\,(1-e),\] where
\[a=\] semi
major axis and \[{{R}_{a}}\,=a\,(1+\,e)\]
\[\therefore
\] eqn.
(i) becomes \[\frac{{{\omega }_{p}}}{{{\omega
}_{a}}}=\,\frac{{{(1+\,e)}^{2}}}{{{(1-\,e)}^{2}}}\]
\[=\,\frac{(1.0167){{\,}^{2}}}{{{(0.9833)}^{2}}}\,\,=1.0691\]
Now
\[{{\omega }_{p}}\,=\,\frac{2\pi }{{{T}_{p}}}\] and \[{{\omega }_{a}}\,=\,\frac{2\pi
}{{{T}_{a}}}\]
\[\therefore
\] \[\frac{{{\omega }_{p}}}{{{\omega
}_{p}}}=\frac{{{T}_{a}}}{{{T}_{p}}}\,=\,\frac{1}{1.0693\,}\,=\,0.9354\] ... (ii)
Also
\[\frac{{{T}_{a}}+\,{{T}_{p}}}{2}=24\]\[\therefore \] \[{{T}_{a}}\,+{{T}_{p}}=48\] ... (iii)
From
eqns. (ii) and (iii), \[{{T}_{p}}=24.8\,h\] and \[{{T}_{a}}=23.20\,h\]
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