In optical communication using silica optical fiber, 1 nm spectral width at 1300 nm corresponds to a bandwidth of (assume refractive index of silica optical fiber = 1.5)
120 GHz
In optical communication systems, understanding the relationship between spectral width and bandwidth is crucial. Spectral width refers to the range of wavelengths present in a light source, while bandwidth refers to the range of frequencies. These two quantities are inversely related, meaning a smaller spectral width corresponds to a larger bandwidth, and vice-versa.
We are provided with the following parameters for the silica optical fiber:
| Parameter | Symbol | Value |
|---|---|---|
| Spectral Width | $\Delta\lambda$ | 1 nm |
| Central Wavelength | $\lambda$ | 1300 nm |
| Refractive Index of Silica Optical Fiber | n | 1.5 |
We also know the speed of light in vacuum, which is $c = 3 \times 10^8$ m/s.
The relationship between the speed of light ($v$), frequency ($f$), and wavelength ($\lambda$) in a medium is given by the formula:
$$f = \frac{v}{\lambda}$$
Where $v$ is the speed of light in the specific medium. Since the light is propagating through a silica optical fiber, we must first calculate the speed of light within this fiber using its refractive index. The speed of light in a medium is given by:
$$v = \frac{c}{n}$$
Substituting the values:
$$v = \frac{3 \times 10^8 \text{ m/s}}{1.5} = 2 \times 10^8 \text{ m/s}$$
To find the bandwidth ($\Delta f$) corresponding to a given spectral width ($\Delta\lambda$), we can differentiate the frequency-wavelength relationship with respect to wavelength:
$$f = \frac{v}{\lambda}$$
Taking the derivative of $f$ with respect to $\lambda$:
$$\frac{df}{d\lambda} = -\frac{v}{\lambda^2}$$
For small changes, the magnitude of the bandwidth ($\Delta f$) can be approximated as:
$$\Delta f = \left| \frac{df}{d\lambda} \right| \Delta\lambda = \frac{v}{\lambda^2} \Delta\lambda$$
Let's convert the given wavelengths from nanometers (nm) to meters (m):
Now, substitute the values into the derived formula:
$$\Delta f = \frac{2 \times 10^8 \text{ m/s}}{(1.3 \times 10^{-6} \text{ m})^2} \times (1 \times 10^{-9} \text{ m})$$
First, calculate the square of the wavelength:
$$(1.3 \times 10^{-6} \text{ m})^2 = 1.69 \times 10^{-12} \text{ m}^2$$
Now, substitute this back into the equation for $\Delta f$:
$$\Delta f = \frac{2 \times 10^8}{1.69 \times 10^{-12}} \times 10^{-9}$$
$$\Delta f = \frac{2}{1.69} \times 10^{8 + 12 - 9}$$
$$\Delta f = \frac{2}{1.69} \times 10^{11} \text{ Hz}$$
$$\Delta f \approx 1.1834 \times 10^{11} \text{ Hz}$$
To convert this frequency to Gigahertz (GHz), we divide by $10^9$ (since 1 GHz = $10^9$ Hz):
$$\Delta f \approx 1.1834 \times 10^{11} \times 10^{-9} \text{ GHz}$$
$$\Delta f \approx 118.34 \text{ GHz}$$
Rounding this value to the nearest option, we get approximately 120 GHz.
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