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A wire of length 10 cm and diameter 0.5 mm is used in a bulb. The temperature of the wire is 1727°C and power radiated by the wire is 94.2 W. Its emissivity is $\frac{x}{8}$ where x =……

(Given $\sigma = 6.0 \times 10^{-8}$ W m$^{-2}$ K$^{-4}$, $\pi = 3.14$ and assume that the emissivity of wire material is same at all wavelength.)

Calculating Wire Emissivity Using Radiation Power

This solution explains how to find the emissivity of a wire in a bulb based on its physical characteristics and the power it radiates, using the Stefan-Boltzmann law.

Given Parameters

  • Wire Length, $L = 10 \text{ cm} = 0.1 \text{ m}$
  • Wire Diameter, $d = 0.5 \text{ mm} = 0.5 \times 10^{-3} \text{ m}$
  • Wire Radius, $r = \frac{d}{2} = 0.25 \times 10^{-3} \text{ m}$
  • Temperature, $T_{\circ C} = 1727^{\circ}\text{C}$
  • Power Radiated, $P = 94.2 \text{ W}$
  • Stefan-Boltzmann constant, $\sigma = 6.0 \times 10^{-8} \text{ W m}^{-2} \text{ K}^{-4}$
  • $\pi = 3.14$
  • Emissivity, $\epsilon = \frac{x}{8}$

Step 1: Convert Temperature to Kelvin

The Stefan-Boltzmann law requires temperature in Kelvin.

$ T(\text{K}) = T(^{\circ}\text{C}) + 273 $

$ T = 1727 + 273 = 2000 \text{ K} $

Step 2: Calculate the Surface Area of the Wire

The wire is treated as a cylinder. The surface area ($A$) is calculated using the formula $A = 2 \pi r L$.

$ A = 2 \times \pi \times r \times L $

$ A = 2 \times 3.14 \times (0.25 \times 10^{-3} \text{ m}) \times (0.1 \text{ m}) $

$ A = 6.28 \times 0.025 \times 10^{-3} \text{ m}^2 $

$ A = 0.157 \times 10^{-3} \text{ m}^2 $

Step 3: Apply the Stefan-Boltzmann Law

The power ($P$) radiated by a surface is given by $P = \epsilon \sigma A T^4$. We need to find the emissivity ($\epsilon$).

$ \epsilon = \frac{P}{\sigma A T^4} $

Step 4: Calculate Emissivity ($\epsilon$)

Substitute the known values into the formula:

$ \epsilon = \frac{94.2 \text{ W}}{(6.0 \times 10^{-8} \text{ W m}^{-2} \text{ K}^{-4}) \times (0.157 \times 10^{-3} \text{ m}^2) \times (2000 \text{ K})^4} $

Calculate $T^4$:

$ T^4 = (2000)^4 = (2 \times 10^3)^4 = 16 \times 10^{12} \text{ K}^4 $

Now substitute $T^4$ back into the emissivity equation:

$ \epsilon = \frac{94.2}{(6.0 \times 10^{-8}) \times (0.157 \times 10^{-3}) \times (16 \times 10^{12})} $

$ \epsilon = \frac{94.2}{(6.0 \times 0.157 \times 16) \times 10^{-8 - 3 + 12}} $

$ \epsilon = \frac{94.2}{150.72 \times 10^{1}} $

$ \epsilon = \frac{94.2}{1507.2} \approx 0.625 $

Step 5: Determine the value of x

The problem states that the emissivity is $\epsilon = \frac{x}{8}$. We found $\epsilon \approx 0.625$.

$ \frac{x}{8} = 0.625 $

$ x = 0.625 \times 8 $

$ x = 5 $

The value of $x$ is 5, which lies between 5 and 5.

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Similar Questions

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Important Questions from Physical and Thermal Properties of Bulk Matter

  1. A water drop of radius $1$ cm is broken into eight equal droplets. Surface tension of water is $0.075$ N $m^{-1}$. The gain in surface energy is __________$\times10^{-7}$ J.(Take $\pi = 3.14$)

  2. Two water drops of radius 'r' each coalesce to form a single large drop. If 'T' is the surface tension, then the surface energy released in this process is:
  3. Pressure of an ideal gas, contained in a closed vessel, is increased by $0.4\%$ when heated by $1^\circ C$. Its initial temperature must be:
  4. A gas is kept in a container having walls which are thermally non-conducting. Initially the gas has a volume of $800 \ cm^3$ and temperature $27^{\circ}C$. The change in temperature when the gas is adiabatically compressed to $200 \ cm^3$ is: 

    (Take $\gamma = 1.5$; $\gamma$ is the ratio of specific heats at constant pressure and at constant volume)

  5. Match List - I with List - II.
    List - IList - II
    (A) Heat capacity of body(I) $J kg^{-1}$
    (B) Specific heat capacity of body(II) $J K^{-1}$
    (C) Latent heat(III) $J kg^{-1} K^{-1}$
    (D) Thermal conductivity(IV) $J m^{-1} K^{-1} s^{-1}$
    Choose the correct answer from the options given below :
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