To determine the ratio of the number of photons emitted by each source, we need to first understand how the energy of light is related to the number of photons and their wavelength.
The energy \(E\) of a single photon is given by the equation:
\(E = \frac{hc}{\lambda}\)
where:
The power \(P\) of the light source is related to the number of photons emitted per second \(N\) by:
\(P = N \times E = N \times \frac{hc}{\lambda}\)
Since both sources emit light with a power of 200 W, the equation for each source is:
\(200 = N_{1} \times \frac{hc}{300 \times 10^{-9}}\)
and
\(200 = N_{2} \times \frac{hc}{500 \times 10^{-9}}\)
We are tasked with finding the ratio \(\frac{N_{1}}{N_{2}}\):
\(N_{1} = \frac{200 \cdot 300 \times 10^{-9}}{hc}\)
\(N_{2} = \frac{200 \cdot 500 \times 10^{-9}}{hc}\)
\(\frac{N_{1}}{N_{2}} = \left(\frac{200 \cdot 300 \times 10^{-9}}{hc}\right) \div \left(\frac{200 \cdot 500 \times 10^{-9}}{hc}\right)\)
\(\frac{N_{1}}{N_{2}} = \frac{300}{500}\)
\(\frac{N_{1}}{N_{2}} = \frac{3}{5}\)
Thus, the ratio of the number of photons emitted by the two light sources is 3:5. Therefore, the correct answer is 3:5.
Let \( n_1 \) and \( n_2 \) be the number of photons emitted by the sources with wavelengths \( \lambda_1 = 300 \, \text{nm} \) and \( \lambda_2 = 500 \, \text{nm} \), respectively.
Step 1. Calculate the energy of photons for each wavelength: The power emitted by each source is given as 200 W, so:
\(n_1 \times \frac{hc}{\lambda_1} = 200\)
\(n_2 \times \frac{hc}{\lambda_2} = 200\)
Step 2. Formulate the ratio:
\(\frac{n_1}{n_2} = \frac{\lambda_2}{\lambda_1}\)
Substituting values:
\(\frac{n_1}{n_2} = \frac{300}{500}\)
Simplifying, we get:
\(\frac{n_1}{n_2} = \frac{3}{5}\)
Therefore, the ratio of the number of photons emitted by each source is 3 : 5.
The Correct Answer is: 3:5
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Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.

Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: