Home
Class 11
PHYSICS
When a block of iron in mercury at 0^@C,...

When a block of iron in mercury at `0^@C,` fraction `K_1`of its volume is submerged, while at the temperature `60^@C,` a fraction `K_2` is seen to be submerged. If the coefficient of volume expansion of iron is `gamma_(Fe)` and that of mercury is `gamma_(Hg),` then the ratio `(K_1)//(K_2)` can be expressed as

A

`(1+60gamma_(Fe))/(1+60gamma_(Hg))`

B

`(1-60gamma_(Fe))/(1+60gamma_(Hg))`

C

`(1+60gamma_(Fe))/(1-60gamma_(Hg))`

D

`(1+60gamma_(Hg))/(1+60gamma_(Fe))`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to analyze the situation where a block of iron is submerged in mercury at two different temperatures, and we want to find the ratio of the fractions of the volume submerged at these two temperatures. ### Step-by-Step Solution: 1. **Understanding the Problem**: - At `0°C`, a fraction `K1` of the volume of the iron block is submerged in mercury. - At `60°C`, a fraction `K2` of the volume is submerged. - We need to express the ratio \( \frac{K1}{K2} \) in terms of the coefficients of volume expansion of iron (\( \gamma_{Fe} \)) and mercury (\( \gamma_{Hg} \)). 2. **Buoyant Force and Weight**: - The weight of the iron block is balanced by the buoyant force exerted by the mercury. - The buoyant force can be expressed as: \[ F_b = \rho_{Hg} \cdot V_s \cdot g \] - The weight of the iron block is: \[ F_w = \rho_{Fe} \cdot V \cdot g \] - Setting these equal gives us: \[ \rho_{Hg} \cdot V_s = \rho_{Fe} \cdot V \] 3. **Defining the Fractions**: - The fraction of the volume submerged \( K \) can be defined as: \[ K = \frac{V_s}{V} \] - Therefore, we can write: \[ K1 = \frac{\rho_{Fe}}{\rho_{Hg}} \quad \text{at } 0°C \] \[ K2 = \frac{\rho_{Fe}'}{\rho_{Hg}'} \quad \text{at } 60°C \] 4. **Density Changes with Temperature**: - The density of a substance changes with temperature according to the formula: \[ \rho' = \frac{\rho}{1 + \gamma \Delta T} \] - For iron at `60°C`: \[ \rho_{Fe}' = \frac{\rho_{Fe}}{1 + \gamma_{Fe} \cdot 60} \] - For mercury at `60°C`: \[ \rho_{Hg}' = \frac{\rho_{Hg}}{1 + \gamma_{Hg} \cdot 60} \] 5. **Substituting into the Fractions**: - Now substituting these into the expressions for \( K2 \): \[ K2 = \frac{\rho_{Fe}'}{\rho_{Hg}'} = \frac{\frac{\rho_{Fe}}{1 + \gamma_{Fe} \cdot 60}}{\frac{\rho_{Hg}}{1 + \gamma_{Hg} \cdot 60}} = \frac{\rho_{Fe} \cdot (1 + \gamma_{Hg} \cdot 60)}{\rho_{Hg} \cdot (1 + \gamma_{Fe} \cdot 60)} \] 6. **Finding the Ratio \( \frac{K1}{K2} \)**: - Now, substituting \( K1 \) and \( K2 \) into the ratio: \[ \frac{K1}{K2} = \frac{\frac{\rho_{Fe}}{\rho_{Hg}}}{\frac{\rho_{Fe} \cdot (1 + \gamma_{Hg} \cdot 60)}{\rho_{Hg} \cdot (1 + \gamma_{Fe} \cdot 60)}} \] - Simplifying this gives: \[ \frac{K1}{K2} = \frac{1 + \gamma_{Hg} \cdot 60}{1 + \gamma_{Fe} \cdot 60} \] ### Final Expression: Thus, the ratio \( \frac{K1}{K2} \) can be expressed as: \[ \frac{K1}{K2} = \frac{1 + 60 \cdot \gamma_{Hg}}{1 + 60 \cdot \gamma_{Fe}} \]

To solve the problem, we need to analyze the situation where a block of iron is submerged in mercury at two different temperatures, and we want to find the ratio of the fractions of the volume submerged at these two temperatures. ### Step-by-Step Solution: 1. **Understanding the Problem**: - At `0°C`, a fraction `K1` of the volume of the iron block is submerged in mercury. - At `60°C`, a fraction `K2` of the volume is submerged. - We need to express the ratio \( \frac{K1}{K2} \) in terms of the coefficients of volume expansion of iron (\( \gamma_{Fe} \)) and mercury (\( \gamma_{Hg} \)). ...
Promotional Banner

Topper's Solved these Questions

  • FLUID MECHANICS

    CENGAGE PHYSICS ENGLISH|Exercise AR_TYPE|1 Videos
  • FLUID MECHANICS

    CENGAGE PHYSICS ENGLISH|Exercise MCQ_TYPE|3 Videos
  • FLUID MECHANICS

    CENGAGE PHYSICS ENGLISH|Exercise True/False|1 Videos
  • DIMENSIONS & MEASUREMENT

    CENGAGE PHYSICS ENGLISH|Exercise Integer|2 Videos
  • GRAVITATION

    CENGAGE PHYSICS ENGLISH|Exercise INTEGER_TYPE|1 Videos

Similar Questions

Explore conceptually related problems

Determine the lengths of an iron rod and copper ruler at 0^@ C if the difference in their lengths at 50^@ C and 450^@ C is the same and is equal to 2 cm. the coefficient of linear expansion of iron =12xx10^(-6)//K and that of copper =17xx10^(-6)//K .

Determine the lengths of an iron rod and copper ruler at 0^@ C if the difference in their lengths at 50^@ C and 450^@ C is the same and is equal to 2 cm. the coefficient of linear expansion of iron =12xx10^(-6)//K and that of copper =17xx10^(-6)//K .

A glass bulb contains air and mercury. What fraction of the bulb must be occupied by mercury if the volume of air in the bulb is to remain constant at all temperatures? The coefficent of linear expansion of glass is 9xx10^(-6)//K .

At 4^(@)C, 0.98 of the volume of a body is immersed in water. The temperature at which the entire body gets immersed in water is (neglect the expansion of the body ) ( gamma_(w) = 3.3 xx10 ^(-4)K^(-1) ):-

There are two layers of water in a calorimeter, the lower one colder at temperature 30^(@)C and the upper one hotter at temperature 60^(@)C . The mass of lower water is m and volume is V . The mass of upper water is 2 m and volume is 2V . The coefficient of volume expansion for water is gamma . When the temperature of the whole system becomes equal , the ratio of new volume to the old volume is .

A cube is floating on mercury with (1//5)^(th) of its volume submerged. If suficient water Is added to cover the cube, what fraction of its volume will remain immersed in mercury ? Density of mercury = 13600 kg//m^(3) .

A glass cylinder contains m_0=100g of mercury at a temperature of t_0=0^@C . When temperature becomes t_1=20^@C the cylinder contains m_1=99.7g of mercury The coefficient of volume expansion of mercury gamma_(He)=18xx(10^(-5)//^(@)C Assume that the temperature of the mercury is equal to that of the cylinder. The coefficient of linear expansion of glass alpha is

A glass cylinder contains m_0=100g of mercury at a temperature of t_0=0^@C . When temperature becomes t_1=20^@C the cylinder contains m_1=99.7g of mercury The coefficient of volume expansion of mercury gamma_(He)=18xx(10^(-5)//^(@)C Assume that the temperature of the mercury is equal to that of the cylinder. The corfficient of linear expansion of glass alpha is

Solids and liquids both expands on heating. The density of substance decreases on expanding according to the relation rho_(2) = (rho_(1))/(1 + gamma(T_(2)- T_(1))) , where , rho_(1) rarr "density at" T_(1) , rho_(2) rarr "density at" T_(2) , gamma rarr coefficient of volume expansion of substances. When a solid is submerged in a liquid , liquid exerts an upward force on solid which is equal to the weight of liquid displaced by submerged part of solid. Solid will float or sink depends on relative densities of solid and liquid . A cubical block of solid floats in a liquid with half ot its volume submerged in liquid as shown in figure (at temperature T ) alpha_(S) rarr Coefficient of linear expansion of solid gamma_(L) rarr "Coefficient of volume expansion of liquid" rho_(S) rarr "Density of solid at temperature" T rho_(L) rarr" Density of liquid at temperature" T If temperature of system increases, then fraction of solid submerged in liquid

Solids and liquids both expands on heating. The density of substance decreases on expanding according to the relation rho_(2) = (rho_(1))/(1 + gamma(T_(2)- T_(1))) , where , rho_(1) rarr "density at" T_(1) , rho_(2) rarr "density at" T_(2) , gamma rarr coefficient of volume expansion of substances. When a solid is submerged in a liquid , liquid exerts an upward force on solid which is equal to the weight of liquid displaced by submerged part of solid. Solid will float or sink depends on relative densities of solid and liquid . A cubical block of solid floats in a liquid with half ot its volume submerged in liquid as shown in figure (at temperature T ) alpha_(S) rarr Coefficient of linear expansion of solid gamma_(L) rarr "Coefficient of volume expansion of liquid" rho_(S) rarr "Density of solid at temperature" T rho_(L) rarr" Density of liquid at temperature" T Imagine the depth of the block submerged in the liquid ,does not change on increasing temperature then