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A hollow sphere floats in a liquid just submerged.what fraction of the volume of the sphere remains submerged in the liquid after its temperature is brought down to dt. the coefficient of cubical expansion for solid and liquid are γ1 and γ2

deepika sharma , 10 Years ago
Grade 11
anser 1 Answers
Askiitians Tutor Team

To determine the fraction of the volume of a hollow sphere that remains submerged in a liquid after a temperature change, we need to consider the effects of thermal expansion on both the sphere and the liquid. This involves understanding how the volume of both the solid and the liquid changes with temperature.

Understanding Thermal Expansion

Every material expands when heated and contracts when cooled. The degree of expansion is quantified by the coefficient of cubical expansion, denoted as γ. For solids, we have γ1, and for liquids, we have γ2. The change in volume (ΔV) due to a temperature change (ΔT) can be expressed as:

  • ΔV_solid = V_initial * γ1 * ΔT
  • ΔV_liquid = V_initial * γ2 * ΔT

Volume Changes in the Sphere and Liquid

Let's denote the initial volume of the hollow sphere as V_s and the initial volume of the liquid as V_l. When the temperature of the system is decreased by dt, the volumes change as follows:

  • New volume of the sphere, V_s' = V_s * (1 - γ1 * dt)
  • New volume of the liquid, V_l' = V_l * (1 - γ2 * dt)

Buoyancy and Submersion

For the sphere to float, the weight of the liquid displaced must equal the weight of the sphere. The principle of buoyancy states that the volume of liquid displaced (V_d) is equal to the volume of the submerged part of the sphere (V_sub). Thus, we can express this relationship as:

  • Weight of the sphere = Weight of the displaced liquid
  • ρ_s * V_s' = ρ_l * V_sub

Here, ρ_s is the density of the sphere and ρ_l is the density of the liquid. The density of the sphere can be expressed in terms of its volume and mass, and similarly for the liquid.

Calculating the Submerged Volume

As the temperature decreases, the density of the liquid increases due to the contraction, while the density of the sphere decreases due to its expansion. The new densities can be expressed as:

  • ρ_s' = ρ_s / (1 - γ1 * dt)
  • ρ_l' = ρ_l / (1 - γ2 * dt)

Substituting these new densities into the buoyancy equation gives us:

  • (ρ_s / (1 - γ1 * dt)) * (V_s * (1 - γ1 * dt)) = (ρ_l / (1 - γ2 * dt)) * V_sub

Finding the Fraction Submerged

To find the fraction of the volume of the sphere that remains submerged, we can rearrange the equation to solve for V_sub:

  • V_sub = (ρ_s * V_s * (1 - γ1 * dt)) / (ρ_l * (1 - γ2 * dt))

The fraction submerged can then be expressed as:

  • Fraction submerged = V_sub / V_s = (ρ_s * (1 - γ1 * dt)) / (ρ_l * (1 - γ2 * dt))

Final Expression

Thus, the fraction of the volume of the hollow sphere that remains submerged in the liquid after the temperature is decreased by dt is:

Fraction submerged = (ρ_s * (1 - γ1 * dt)) / (ρ_l * (1 - γ2 * dt))

This equation shows how the thermal properties of both the sphere and the liquid interact to determine the submerged volume, highlighting the importance of understanding thermal expansion in fluid mechanics.

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