A) \[T\propto \,\,\sqrt{\rho }\]
B) \[T\propto \,\,\frac{1}{\sqrt{A}}\]
C) \[T\propto \,\,\frac{1}{\rho }\]
D) \[T\propto \,\,\frac{1}{\sqrt{m}}\]
Correct Answer: B
Solution :
Key Idea: Force applied on the body will be equal to up thrust for vertical oscillations. |
Let block is displaced through \[x\,m,\] then weight of displaced water or upthrust (upwards). |
\[=-Ax\rho g\] |
where A is area of cross-section of the block and \[\rho \] is its density. This must be equal to force \[(=ma)\] applied, where m is mass of the block and a is acceleration. |
\[\therefore \] \[ma=-Ax\rho g\] |
or \[a=-\frac{A\rho g}{m}x=-{{\omega }^{2}}x\] |
This is the equation of simple harmonic motion. |
Time period of oscillation |
\[T=\frac{2\pi }{\omega }=2\pi \sqrt{\frac{m}{A\rho g}}\] |
\[\Rightarrow \] \[T\propto \,\frac{1}{\sqrt{A}}\] |
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