\(\frac {26K}{\rho r\left(L-4s\right)}\)
\(\frac {6K}{\left(\rho x^{2}-L\right)}\)
\(\frac {26K}{\left(\rho xL\right)}\)
\(\frac {26K}{\rho r\left(L+4s\right)}\)
\(KA \frac{[0-(-26)]}{x} dt\)\(= A(dx) \rho L\)
\(\Rightarrow \frac{dx}{dt} = \frac{26K}{\rho K x}\)
So, the correct option is (C): \(\frac {26K}{\left(\rho xL\right)}\).
The rate of increase in the thickness of the ice layer can be calculated using the concept of heat transfer through the ice layer. Heat transfer occurs due to the temperature difference between the water in the pond and the surrounding air.
The rate of heat transfer per unit area (q) through the ice layer can be calculated using Fourier's law of heat conduction, which states that the rate of heat transfer is proportional to the temperature gradient and the thermal conductivity of the material.
\(q = K \times \frac{dT}{dx}\)
where K is the thermal conductivity of ice, \(\frac{dT}{dx}\) is the temperature gradient across the ice layer, and x is the thickness of the ice layer.
The rate of increase of the thickness of the ice layer (dx/dt) can be calculated using the heat transfer equation as:
\(\frac{dx}{dt} = \frac{L}{rAs} \times q\)
where L is the specific latent heat of fusion of ice, r is the density of water, A is the surface area of the pond, and s is the specific heat capacity of water.
Substituting the value of q from Fourier's law of heat conduction, we get:
\(\frac{dx}{dt} = \frac{L}{rAs} \times K \times \frac{dT}{dx}\)
Since the air temperature outside the pond is at a steady value of -26°C, the temperature gradient across the ice layer can be assumed to be constant, and equal to the temperature difference between the water and the air, which is:
\(\frac{dT}{dx} = \frac{0°C - (-26°C)}{x} = \frac{26°C}{x}\)
Substituting this value in the above equation, we get:
\(\frac{dx}{dt} = \frac{LK}{rAs} \times \frac{26°C}{x}\)
Therefore, the rate of increase of the thickness of the ice layer at a certain instant is given by:
\(\frac{dx}{dt} = \frac{LK}{rAs} \times \frac{26°C}{x}\)
Given:
Surface Area = A,
Density = ρ,
Specific heat capacity = s,
Thermal conductivity of ic = K,
Specific latent heat of fusion = L
Assuming Volume to be V.
The rate of increase in the thickness of the ice layer can be calculated using the concept of heat transfer through the ice layer. Heat transfer occurs due to the temperature difference between the water in the pond and the surrounding air.
We assume that at any instant the thickness of ice is (x) and time taken to form an additional thickness (dx) is (dt).
Let the mass formed by the additional thickness of ice be m.
The heat energy released by forming the additional thickness of ice (m) be (dq).
Therefore, \(dq = mL = ρ\times (A \times dx) \times L\)
We know, \(r = \frac mv\)
Therefore, \(m = ρ\times v\)
\(m= ρ \times (A \times dx)\)
Heat current (iH) flows due to (m) which is calculated using Fourier's law of heat conduction, which states that the rate of heat transfer is proportional to the temperature gradient and the thermal conductivity of the material.
\(\frac {dq}{dt}=\frac {KA(0+26)}{x}\)
\(\frac {ρ(Adx)L}{dt}=\frac {KA26}{x}\)
\(\frac {dx}{dt}=\frac {26K}{ρxL}\)
Therefore, the rate of increase of the thickness of the ice layer, at this instant would be given by \(\frac {26K}{ρxL}\).
So, the correct option is (C): \(\frac {26K}{ρxL}\).
Three conductors of same length having thermal conductivity \(k_1\), \(k_2\), and \(k_3\) are connected as shown in figure. Area of cross sections of 1st and 2nd conductor are same and for 3rd conductor it is double of the 1st conductor. The temperatures are given in the figure. In steady state condition, the value of θ is ________ °C. (Given: \(k_1\) = 60 Js⁻¹m⁻¹K⁻¹,\(k_2\) = 120 Js⁻¹m⁻¹K⁻¹, \(k_3\) = 135 Js⁻¹m⁻¹K⁻¹)
It is defined as the movement of heat across the border of the system due to a difference in temperature between system and its surroundings.
Heat can travel from one place to another in several ways. The different modes of heat transfer include: