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The filament of a light bulb has surface...

The filament of a light bulb has surface has area `64mm^(2)`. The filament can considered as a black body at temperature 2500 K emitting radiation like a point source when viewed form far. At night the light bulb is observed from a distance of 100 m. Assume the pupil of the eyes of the observer to be circular with radius 3 mm. Then (Take Stefan-Boltzman constant `=5.67xx10^(-8)" Wm"^(-2)K^(-4)`, Wien's displacement constant `=2.90xx10^(-3)` m-k, Planck's constant `=6.63xx10^(-8)Wm^(-2)K^(-4)`, Wien's displacement constant `=2.90xx10^(-3)`m-K, Planck's constant `=6.63xx10^*-34)` js, speed of light in vacumm `=3.00xx10^(8)ms^(-1)`)

A

power radiated by the filament is in the range 642 W to 645 W

B

radiated power entering into one of range 642 W to `3.25xx10^(-8)W`

C

the wavelength corresponding to maximum intensity is 1160 nm

D

taking the average wavelength of emitted radiation to be 1740 nm, the number of photons entering per second into one eye of the observer is in the range `2.75xx10^(11)` to `2.85xx10^(11)`

Text Solution

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The correct Answer is:
To solve the problem step by step, we will follow the outlined procedure: ### Step 1: Convert the Surface Area to SI Units The surface area of the filament is given as \(64 \, \text{mm}^2\). We need to convert this to square meters. \[ A = 64 \, \text{mm}^2 = 64 \times 10^{-6} \, \text{m}^2 \] ### Step 2: Calculate the Power Radiated by the Filament Using the Stefan-Boltzmann law, the power radiated by a black body is given by: \[ P = \varepsilon A \sigma T^4 \] For a black body, the emissivity \(\varepsilon = 1\). Thus, we have: \[ P = A \sigma T^4 \] Substituting the values: - \(A = 64 \times 10^{-6} \, \text{m}^2\) - \(\sigma = 5.67 \times 10^{-8} \, \text{W/m}^2\text{K}^4\) - \(T = 2500 \, \text{K}\) Calculating \(T^4\): \[ T^4 = (2500)^4 = 3.90625 \times 10^{13} \, \text{K}^4 \] Now substituting into the power formula: \[ P = (64 \times 10^{-6}) \times (5.67 \times 10^{-8}) \times (3.90625 \times 10^{13}) \] Calculating \(P\): \[ P \approx 141.75 \, \text{W} \] ### Step 3: Calculate the Intensity of the Light at a Distance The intensity \(I\) at a distance \(d\) from a point source is given by: \[ I = \frac{P}{4 \pi d^2} \] Given \(d = 100 \, \text{m}\): \[ I = \frac{141.75}{4 \pi (100)^2} \] Calculating \(I\): \[ I \approx \frac{141.75}{12566.37} \approx 0.01129 \, \text{W/m}^2 \] ### Step 4: Calculate the Power Entering the Observer's Eye The area of the observer's pupil is given by: \[ A_{pupil} = \pi r^2 \] Where \(r = 3 \, \text{mm} = 3 \times 10^{-3} \, \text{m}\): \[ A_{pupil} = \pi (3 \times 10^{-3})^2 \approx 2.827 \times 10^{-5} \, \text{m}^2 \] The power \(P'\) entering the observer's eye is given by: \[ P' = I \cdot A_{pupil} \] Substituting the values: \[ P' = 0.01129 \times 2.827 \times 10^{-5} \approx 3.18 \times 10^{-7} \, \text{W} \] ### Step 5: Convert Power to a Suitable Format To express this in a more standard form: \[ P' \approx 3.18 \times 10^{-8} \, \text{W} \] ### Step 6: Calculate the Number of Photons Entering the Eye Using the average wavelength \(\lambda = 1740 \, \text{nm} = 1740 \times 10^{-9} \, \text{m}\): The energy of a single photon is given by: \[ E = \frac{hc}{\lambda} \] Where \(h = 6.63 \times 10^{-34} \, \text{Js}\) and \(c = 3 \times 10^{8} \, \text{m/s}\). Calculating \(E\): \[ E = \frac{(6.63 \times 10^{-34})(3 \times 10^{8})}{1740 \times 10^{-9}} \approx 1.14 \times 10^{-19} \, \text{J} \] Now, the number of photons \(n\) entering the eye per second is given by: \[ n = \frac{P'}{E} \] Substituting the values: \[ n = \frac{3.18 \times 10^{-8}}{1.14 \times 10^{-19}} \approx 2.79 \times 10^{11} \] ### Final Answers 1. The power entering the observer's eye is approximately \(3.18 \times 10^{-8} \, \text{W}\). 2. The number of photons entering the observer's eye per second is approximately \(2.79 \times 10^{11}\).

To solve the problem step by step, we will follow the outlined procedure: ### Step 1: Convert the Surface Area to SI Units The surface area of the filament is given as \(64 \, \text{mm}^2\). We need to convert this to square meters. \[ A = 64 \, \text{mm}^2 = 64 \times 10^{-6} \, \text{m}^2 \] ...
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