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A metallic sphere having radius 0.08 m a...

A metallic sphere having radius `0.08 m` and mass `m = 10 kg` is heated to a temperature of `227^(@)C` and suspended inside a box whose walls ae at a temperature of `27^(@)C`. The maximum rate at which its temperature will fall is:-
(Take `e =1`, Stefan's constant `sigma = 5.8 xx 10^(-8) W//m^(-2)K^(-4)` and specific heat of the metal `s = 90 cal//kg//deg J = 4.2 "Joules"//"Calorie")`

A

`0.55^(@)C//sec`

B

`0.66^(@)C//sec`

C

`0.44^(@)C//sec`

D

`0.03^(@)C//sec`

Text Solution

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The correct Answer is:
To find the maximum rate at which the temperature of the metallic sphere will fall, we can use the Stefan-Boltzmann law for radiation. The formula for the rate of cooling is given by: \[ \frac{dT}{dt} = -\frac{\sigma \cdot e \cdot A \cdot (T^4 - T_w^4)}{m \cdot s} \] Where: - \(\sigma\) is the Stefan-Boltzmann constant, - \(e\) is the emissivity (given as 1), - \(A\) is the surface area of the sphere, - \(T\) is the initial temperature of the sphere in Kelvin, - \(T_w\) is the temperature of the walls in Kelvin, - \(m\) is the mass of the sphere, - \(s\) is the specific heat of the metal. ### Step 1: Convert temperatures to Kelvin - Initial temperature of the sphere: \[ T = 227^\circ C = 227 + 273 = 500 \, K \] - Temperature of the walls: \[ T_w = 27^\circ C = 27 + 273 = 300 \, K \] ### Step 2: Calculate the surface area of the sphere The surface area \(A\) of a sphere is given by the formula: \[ A = 4\pi r^2 \] Where \(r\) is the radius of the sphere. Given \(r = 0.08 \, m\): \[ A = 4\pi (0.08)^2 = 4\pi (0.0064) \approx 0.0804 \, m^2 \] ### Step 3: Substitute values into the cooling rate formula Using the values: - \(\sigma = 5.8 \times 10^{-8} \, W/m^2K^4\) - \(e = 1\) - \(A \approx 0.0804 \, m^2\) - \(T = 500 \, K\) - \(T_w = 300 \, K\) - \(m = 10 \, kg\) - \(s = 90 \, cal/kg \cdot K = 90 \times 4.2 \, J/kg \cdot K = 378 \, J/kg \cdot K\) Now substituting these values into the cooling rate formula: \[ \frac{dT}{dt} = -\frac{(5.8 \times 10^{-8}) \cdot (1) \cdot (0.0804) \cdot ((500)^4 - (300)^4)}{10 \cdot 378} \] ### Step 4: Calculate \( (500)^4 - (300)^4 \) Calculating \( (500)^4 \) and \( (300)^4 \): \[ (500)^4 = 62500000000 \] \[ (300)^4 = 8100000000 \] Thus, \[ (500)^4 - (300)^4 = 62500000000 - 8100000000 = 54400000000 \] ### Step 5: Substitute back into the formula Now substituting this back into the formula: \[ \frac{dT}{dt} = -\frac{(5.8 \times 10^{-8}) \cdot (0.0804) \cdot (54400000000)}{10 \cdot 378} \] ### Step 6: Calculate the numerator and denominator Calculating the numerator: \[ 5.8 \times 10^{-8} \times 0.0804 \times 54400000000 \approx 0.252 \] Calculating the denominator: \[ 10 \cdot 378 = 3780 \] ### Step 7: Final calculation Now, substituting these values: \[ \frac{dT}{dt} = -\frac{0.252}{3780} \approx -0.0000667 \, K/s \] ### Step 8: Convert to Celsius per second Since the change in temperature in Kelvin is equivalent to Celsius, we have: \[ \frac{dT}{dt} \approx -0.0667 \, ^\circ C/s \] ### Final Answer The maximum rate at which the temperature of the metallic sphere will fall is approximately: \[ \frac{dT}{dt} \approx -0.0667 \, ^\circ C/s \]

To find the maximum rate at which the temperature of the metallic sphere will fall, we can use the Stefan-Boltzmann law for radiation. The formula for the rate of cooling is given by: \[ \frac{dT}{dt} = -\frac{\sigma \cdot e \cdot A \cdot (T^4 - T_w^4)}{m \cdot s} \] Where: - \(\sigma\) is the Stefan-Boltzmann constant, ...
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