Question #22316

A block of wood having specific gravity 0.85 floats on water. Some oil of specific gravity 0.82 is poured on the surface of water until the the wooden block is just immersed. calculate the fraction of block lying below the surface of water in the second case.
1

Expert's answer

2013-01-21T10:13:15-0500

A block of wood having specific gravity 0.85 floats on water. Some oil of specific gravity 0.82 is poured on the surface of water until the wooden block is just immersed. Calculate the fraction of block lying below the surface of water in the second case.

Solution.


ρ1ρw=0.85,ρ2ρw=0.82;\frac {\rho_ {1}}{\rho_ {w}} = 0. 8 5, \frac {\rho_ {2}}{\rho_ {w}} = 0. 8 2;V1V?\frac {V _ {1}}{V} -?


Newton's second law in vector form:


ma=B1+B2+mg.m \vec {a} = \overrightarrow {B _ {1}} + \overrightarrow {B _ {2}} + m \vec {g}.


A block is at rest, then:


a=0.\vec {a} = 0.0=B1+B2+mg.0 = \overrightarrow {B _ {1}} + \overrightarrow {B _ {2}} + m \vec {g}.


Projection on Y:


0=B1+B2mg;0 = B _ {1} + B _ {2} - m g;B1+B2=mg.B _ {1} + B _ {2} = m g.

B1B_{1} - the buoyancy force in the water.

B2B_{2} - the buoyancy force in the oil.

mm - the mass of a block.


m=ρ1V;m = \rho_ {1} V;

ρ1\rho_{1} – the density of the wood.

VV – the volume of the block.


B1=ρwV1g;B _ {1} = \rho_ {w} V _ {1} g;B2=ρ2V2g.B _ {2} = \rho_ {2} V _ {2} g.

V2V_{2} – the part of volume of the block above water level.


V2=VV1;V _ {2} = V - V _ {1};B2=ρ2(VV1)g;B _ {2} = \rho_ {2} (V - V _ {1}) g;

ρw\rho_w – the density of the water;

ρ2\rho_{2} – the density of the oil;

V1V_{1} – the part of volume of the block below water level.


ρwV1g+ρ2(VV1)g=ρ1Vg.\rho_ {w} V _ {1} g + \rho_ {2} (V - V _ {1}) g = \rho_ {1} V g.


Divide by gg:


ρwV1+ρ2(VV1)=ρ1V.\rho_ {w} V _ {1} + \rho_ {2} (V - V _ {1}) = \rho_ {1} V.


Divide by ρw\rho_w:


V1+ρ2ρw(VV1)=ρ1ρwV;V _ {1} + \frac {\rho_ {2}}{\rho_ {w}} (V - V _ {1}) = \frac {\rho_ {1}}{\rho_ {w}} V;V1+ρ2ρwVρ2ρwV1=ρ1ρwV.V _ {1} + \frac {\rho_ {2}}{\rho_ {w}} V - \frac {\rho_ {2}}{\rho_ {w}} V _ {1} = \frac {\rho_ {1}}{\rho_ {w}} V.


Divide by VV:


V1V+ρ2ρwρ2ρwV1V=ρ1ρw;\frac {V _ {1}}{V} + \frac {\rho_ {2}}{\rho_ {w}} - \frac {\rho_ {2}}{\rho_ {w}} \frac {V _ {1}}{V} = \frac {\rho_ {1}}{\rho_ {w}};V1V(1ρ2ρw)=ρ1ρwρ2ρw;\frac {V _ {1}}{V} \left(1 - \frac {\rho_ {2}}{\rho_ {w}}\right) = \frac {\rho_ {1}}{\rho_ {w}} - \frac {\rho_ {2}}{\rho_ {w}};V1V=ρ1ρwρ2ρw(1ρ2ρw),\frac {V _ {1}}{V} = \frac {\frac {\rho_ {1}}{\rho_ {w}} - \frac {\rho_ {2}}{\rho_ {w}}{\left(1 - \frac {\rho_ {2}}{\rho_ {w}}\right)}},V1V=0.850.82(10.82)=0.17.\frac {V _ {1}}{V} = \frac {0.85 - 0.82}{(1 - 0.82)} = 0.17.


Answer: V1V=0.17\frac{V_1}{V} = 0.17.


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