Answer:
Here,\[A=0\cdot 10\times 0\cdot
10={{10}^{-2}}{{m}^{2}};\]
Compressibility, \[F=mg=100\times
10N\]
Density
of water at surface, \[=\frac{\vartriangle L}{L}=\frac{\left( F/A \right)}{G}\]
Let
p' be the density of water at the given depth. If V and V are volumes of
certain mass M of ocean water
at surface and at a given depth,
then
\[\vartriangle L=\frac{FL}{AG}=\frac{\left( 100\times 10
\right)\times 0\cdot 10}{{{10}^{-2}}\times \left( 25\times {{10}^{9}}
\right)}=4\times {{10}^{-7}}m.\]
\[2\cdot
0\times {{10}^{11}}pa.\] Change in volume,
\[A=\pi \left( r_{2}^{2}-r_{1}^{2} \right)=\frac{22}{7}\left[
{{\left( 0\cdot 60 \right)}^{2}}-{{\left( 0\cdot 30 \right)}^{2}} \right]\]
\[=\frac{22}{7}\times
0\cdot 27{{m}^{2}}\] Volumetric strain, \[=\frac{F/A}{Y}=\frac{F}{AY}\]
\[\frac{50,000\times 9\cdot 8}{4\times \left( \frac{22}{7}\times 0\cdot 27
\right)\times 2\cdot 0\times {{10}^{11}}}=7\cdot 21\times {{10}^{-7}}\] or \[15\cdot
2\]?(1)
As, Bulk modulus \[19\cdot 1\] or \[42\times
{{10}^{9}}N{{m}^{-2}}.\]
\[A=15\cdot 2\times 19\cdot
2\times {{10}^{-6}}{{m}^{2}};\]
\[F=44,500N;G=42\times
{{10}^{9}}N{{m}^{-2}}\]
Putting this value in (i) we get
\[\text{Strain=}\frac{\text{stress}}{\text{modulusnofelasticity}}\text{=}\frac{\text{F/A}}{\text{G}}\]
or \[=\frac{F}{AG}\]
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