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Question: A cuboidal piece of wood has dimensions \[a\], \[b\] and \[c\]. Its relative density is \[d\]. It is...

A cuboidal piece of wood has dimensions aa, bb and cc. Its relative density is dd. It is floating in a large body of water such that the side aa is vertical. It is pushed down a bit and released. The time period of SHM executed by it is
A. 2πabcg2\pi \sqrt {\dfrac{{abc}}{g}}
B. 2πgda2\pi \sqrt {\dfrac{g}{{da}}}
C. 2πbcdg2\pi \sqrt {\dfrac{{bc}}{{dg}}}
D. 2πdag2\pi \sqrt {\dfrac{{da}}{g}}

Explanation

Solution

Use the law of floatation of an object floating on a liquid. From this law determine the length of the wooden cube immersed in the water. Use this length as the length of the oscillation in the formula for the time period of the simple pendulum and determine the time period of the SHM executed by the cube.

Formulae used:
The time period TT of simple pendulum is
T=2πLgT = 2\pi \sqrt {\dfrac{L}{g}} …… (1)
Here, LL is the length of the simple pendulum and gg is the acceleration due to gravity.
The density ρ\rho of an object is
ρ=MV\rho = \dfrac{M}{V} …… (2)
Here, MM is the mass of the object and VV is the volume of the object.
The upward thrust FF acting on an object floating on water is
F=ρVgF = \rho Vg …… (3)
Here, ρ\rho is density of water, VV is the volume of water displaced by the floating object and gg is acceleration due to gravity.

Complete step by step answer:
We have given that the dimensions of the wooden cube are aa, bb and cc. The relative density of the wooden cube is dd. The length of the wooden block immersed in the water is the length of the cube for oscillations.
Let MM be the mass of the wooden cube.
The weight of the wooden cube is
W=MgW = Mg
According to equation (2), the above equation becomes
W=dVgW = dVg
Substitute abcabc for VV volume of the cube in the above equation.
W=dabcgW = dabcg
The buoyant force acting on the wooden cube is given by equation (3).
F=ρw(ybc)gF = {\rho _w}\left( {ybc} \right)g
Here, ρw{\rho _w} is density of water and yy is the length of the wooden cube immersed in water from the length aa.
Substitute 1g/cc1\,{\text{g/cc}} for ρw{\rho _w} in the above equation.
F=(1g/cc)(ybc)gF = \left( {1\,{\text{g/cc}}} \right)\left( {ybc} \right)g
F=ybcg\Rightarrow F = ybcg
According to the law of floatation, the weight of the wooden block immersed in water is equal to the buoyant force acting on the wooden cube immersed in the water.
W=FW = F
Substitute abcdgabcdg for WW and ybcgybcg for FF in the above equation.
abcdg=ybcgabcdg = ybcg
y=da\Rightarrow y = da
Therefore, the length of oscillation of the cube in the water is dada.
We can determine the time period of oscillation of the cube using equation (1).
Rewrite equation (1) for the time period of oscillation of the cube.
T=2πygT = 2\pi \sqrt {\dfrac{y}{g}}
Substitute dada for yy in the above equation.
T=2πdag\therefore T = 2\pi \sqrt {\dfrac{{da}}{g}}
Therefore, the time period for the SHM of the cube is 2πdag2\pi \sqrt {\dfrac{{da}}{g}} .

Hence, the correct option is D.

Note: The students should be careful while using floatation law. The value of the volume of water displaced by the wooden cube in the formula for upward thrust acting on the wooden cube is equal to the volume of the cube immersed in the water and not the total volume of the wooden cube.