The least count (LC) of a vernier caliper is given by: \[ \text{LC} = 1 \text{ main scale division} - 1 \text{ vernier scale division} \]
Given that the least count is \(\frac{1}{20N}\) cm and one main scale division is 1 mm = 0.1 cm, we can write:
\[\frac{1}{20N} \text{ cm} = 0.1 \text{ cm} - \frac{N}{x} \text{ cm}\]
where 'x' represents the total number of vernier scale divisions.
We can assume that 'x' vernier scale divisions are equal to N main scale divisions. Thus, \(\frac{N}{x} \text{ cm}\) represents the length of N vernier divisions. Solving for \(\frac{N}{x}\), we get:
\[\frac{N}{x} = 0.1 - \frac{1}{20N} = \frac{2N - 1}{20N} \text{ cm}\]
Now, we know that N vernier scale divisions coincide with (n) main scale divisions. Then, the length of N vernier divisions equals the length of n main scale divisions:
\[\frac{N}{x} \text{ cm} = n \times 0.1 \text{ cm}\]
Therefore:
\[n = \frac{N}{x} \times \frac{1}{0.1} = \frac{2N - 1}{20N} \times 10 = \frac{2N - 1}{2}\]
Thus, the number of main scale divisions that coincide with N vernier scale divisions is \(\frac{2N - 1}{2}\).
The ratio of the power of a light source \( S_1 \) to that of the light source \( S_2 \) is 2. \( S_1 \) is emitting \( 2 \times 10^{15} \) photons per second at 600 nm. If the wavelength of the source \( S_2 \) is 300 nm, then the number of photons per second emitted by \( S_2 \) is ________________ \( \times 10^{14} \).
Match the LIST-I with LIST-II
LIST-I | LIST-II | ||
---|---|---|---|
A. | Boltzmann constant | I. | \( \text{ML}^2\text{T}^{-1} \) |
B. | Coefficient of viscosity | II. | \( \text{MLT}^{-3}\text{K}^{-1} \) |
C. | Planck's constant | III. | \( \text{ML}^2\text{T}^{-2}\text{K}^{-1} \) |
D. | Thermal conductivity | IV. | \( \text{ML}^{-1}\text{T}^{-1} \) |
Choose the correct answer from the options given below :