Fe and that of mercury is
Hg then ratio K1/K2 is? Ans. 1+60
Fe/1+60
Hg
Thermal Physics> Q1. When a block of iron floats in mercur...
Fe and that of mercury is
Hg then ratio K1/K2 is? Ans. 1+60
Fe/1+60
Hg
3 AnswersTo tackle this problem, we need to understand how temperature affects the volume of both the iron block and the mercury in which it floats. The key concepts here are the coefficients of volume expansion for both materials and how they relate to buoyancy.
When an object floats in a fluid, the fraction of its volume that is submerged is determined by the principle of buoyancy, which states that the weight of the fluid displaced by the submerged part of the object equals the weight of the object itself. In this case, we have an iron block floating in mercury.
The coefficient of volume expansion (denoted as β) indicates how much a material's volume changes with temperature. For our scenario:
As temperature increases, the volume of both the iron block and the mercury will change according to their respective coefficients of volume expansion.
Let’s denote:
VFe = V0 (1 + 60βFe)
Similarly, for mercury, we denote the initial volume as VHg and the volume at 60°C as:
VHg = V0 (1 + 60βHg)
At 0°C, the fraction of the iron block submerged in mercury is:
K1 = Viron submerged / VHg
At 60°C, the fraction submerged becomes:
K2 = Viron submerged at 60°C / VHg at 60°C
To find the ratio K1/K2, we can substitute the expressions for the volumes at different temperatures:
K1 = V0 / VHg
K2 = V0 (1 + 60βFe) / V0 (1 + 60βHg)
Now, simplifying the ratio gives us:
K1 / K2 = (V0 / VHg) / [(V0 (1 + 60βFe)) / (V0 (1 + 60βHg))]
This simplifies to:
K1 / K2 = (1 + 60βHg) / (1 + 60βFe)
Thus, the ratio of the submerged fractions at the two temperatures can be expressed as:
K1 / K2 = 1 + (60βFe) / (1 + 60βHg)
In conclusion, the ratio K1/K2 is indeed given by:
K1 / K2 = 1 + (60βFe) / (1 + 60βHg)
This relationship illustrates how the differing expansion rates of iron and mercury affect the buoyancy of the iron block as the temperature changes. Understanding these principles helps us grasp the fundamental concepts of thermodynamics and fluid mechanics.
To tackle the problem of how the fraction of a block of iron submerged in mercury changes with temperature, we need to consider the principles of buoyancy and thermal expansion. The key here is to understand how both the iron and the mercury respond to temperature changes.
When an object is placed in a fluid, it experiences an upward force known as buoyancy, which is equal to the weight of the fluid displaced by the submerged part of the object. For our scenario, the fraction of the iron block submerged in mercury can be expressed using Archimedes' principle.
At 0 degrees Celsius, let’s denote the fraction of the volume of the iron block that is submerged in mercury as K1. The weight of the displaced mercury equals the weight of the iron block. Mathematically, this can be expressed as:
As the temperature increases to 60 degrees Celsius, both the iron and the mercury will expand. The volume expansion can be described by the formula:
ΔV = V0 × β × ΔT
Where:
For the iron block, the new volume at 60 degrees Celsius becomes:
V_iron(60) = V_iron(0) × (1 + 60 × β_Fe)
For mercury, the new volume is:
V_mercury(60) = V_mercury(0) × (1 + 60 × β_Hg)
At the new temperature, we denote the fraction of the iron block submerged in mercury as K2. The relationship between the submerged volumes at the two temperatures can be expressed as:
K1 × V_mercury(0) × ρ_Hg = V_iron(0) × ρ_Fe
And for the second condition:
K2 × V_mercury(60) × ρ_Hg = V_iron(60) × ρ_Fe
To find the ratio K1/K2, we can divide the two equations:
K1/K2 = (V_iron(0) × ρ_Fe) / (V_mercury(0) × ρ_Hg) × (V_mercury(60) / V_iron(60))
Substituting the expressions for the volumes at 60 degrees Celsius, we get:
K1/K2 = (1 + 60 × β_Fe) / (1 + 60 × β_Hg)
Thus, the ratio of the fractions submerged at the two temperatures is:
K1/K2 = 1 + 60 × β_Fe / (1 + 60 × β_Hg)
This result shows how the different coefficients of volume expansion for iron and mercury affect the buoyancy and, consequently, the fraction of the iron block submerged in mercury at different temperatures.
To tackle the problem of how the fraction of a block of iron submerged in mercury changes with temperature, we need to consider the principles of buoyancy and thermal expansion. The key here is to understand how both the iron and mercury respond to temperature changes and how that affects their respective volumes.
When an object is placed in a fluid, it experiences an upward force known as buoyancy, which is equal to the weight of the fluid displaced by the object. The fraction of the object submerged in the fluid can be expressed as:
For a block of iron floating in mercury, the buoyant force must equal the weight of the iron block. Hence, we can write:
K1 = V_submerged / V_total = (Weight of iron) / (Weight of displaced mercury)
As temperature increases, both the iron and mercury will expand. The volume expansion can be described by the formula:
ΔV = V0 * β * ΔT
Where:
For our scenario, at 0°C, the volume of iron is V0 and at 60°C, its volume becomes:
V_iron(60°C) = V0 * (1 + 60 * β_Fe)
Similarly, for mercury, the volume at 60°C becomes:
V_mercury(60°C) = V_mercury(0°C) * (1 + 60 * β_Hg)
At 0°C, the fraction submerged is:
K1 = V_iron(0°C) / V_mercury(0°C)
At 60°C, the fraction submerged becomes:
K2 = V_iron(60°C) / V_mercury(60°C)
Substituting the expanded volumes into the equation gives:
K2 = (V0 * (1 + 60 * β_Fe)) / (V_mercury(0°C) * (1 + 60 * β_Hg))
Now, we can find the ratio of K1 to K2:
K1/K2 = (V_iron(0°C) / V_mercury(0°C)) / ((V_iron(0°C) * (1 + 60 * β_Fe)) / (V_mercury(0°C) * (1 + 60 * β_Hg)))
This simplifies to:
K1/K2 = (1) / (1 + 60 * β_Fe) / (1 + 60 * β_Hg)
Thus, we arrive at the final ratio:
K1/K2 = (1 + 60 * β_Hg) / (1 + 60 * β_Fe)
In conclusion, the ratio of the fractions submerged at different temperatures is:
K1/K2 = 1 + 60 * β_Fe / (1 + 60 * β_Hg)
This relationship illustrates how the thermal expansion of both materials affects their buoyancy in a fluid, providing a clear understanding of the interplay between temperature and volume in this context.

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