A 30cm-tall, 4.0cm-diameter plastic tube has a sealed bottom. 250gof lead pellets are poured into the bottom of the tube, whose mass is 30g, then the tube is lowered into a liquid. The tube floats with5.0cm extending above the surface. What is the density of the liquid?

Short Answer

Expert verified

Therefore the mass of the rock is113g

Step by step solution

01

Step : 1 Introduction 

Archimedes principle states that the upward force acts on the object when an object partly or fully immersed in a fluid. This force is called buoyant force. Mathematically, the buoyant force can be expressed as,

FB=ρV/g

Here, ρis the density of fluid, Vis volume of displaced fluid, andg is acceleration due to gravity.

02

Step :2 Explanation 

Let rbe the radius of the hemisphere. The diameter of the hemisphere is 0.8cm. Thus, the radius of the hemisphere is,

r=8.0cm2

=4.0cm1m100cm

=0.04m

The volume of the hemisphere is half of the sphere. Thus, the volume of hemisphere is,

V=23πr3

Substitute 0.04mforrin above equation

V=23π(0.04m)3

=1.34×104m3

03

Step :3 Weight of the rock 

The weight of the rock and the hemisphere bowl

Fg=mg+MgFs=g(m+M)

Fz=mg+MgFs=g(m+M)

Here, mis the mass of the rock, Mis the mass of the hemisphere, and gis the acceleration due to gravity.

After the rock is placed in the bottom of a plastic boat with maximum weight, the hemisphere gets totally dipped in the water without sinking it, and the water level is just in level with the hemisphere. So, the total buoyant force exerted on the hemisphere is equal to the total weight of the system of rock and the hemisphere bowl. Thus.

FB=Fg

Substitute ρVgforFB,g(m+M)forFgin above equation

ρVg=(m+M)g

ρV=m+M

Rewrite the equation in ρwV=m+Mform

m=ρwVM

Substitute 1000kg/m3forρ,1.34×104m3forV, and21gforMin above equation

M=1000kg/m31.34×104m3(21g)103kg1g

=0.113kg

=0.113kg1000g1kg

=113g

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Most popular questions from this chapter

In addition to the buoyant force, an object moving in a liquid experiences a linear drag force Fdrag=(bv, direction opposite the motion), where bis a constant. For a sphere of radius R, the drag constant can be shown to be b=6πηR, where ηis the viscosity of the liquid. Consider a sphere of radiusRand density ρthat is released from rest at the surface of a liquid with density ρf.

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