Given:
\[ {}^6C_m + 2({}^6C_{m+1}) + {}^6C_{m+2} > {}^8C_3 \]
\[ {}^7C_{m+1} + {}^7C_{m+2} > {}^8C_3 \]
\[ {}^8C_{m+2} > {}^8C_3 \]
∴ m = 2
Step 2: Using the relation
\[ {}^{n-1}P_3 : {}^nP_4 = 1 : 8 \]
\[ \frac{(n-1)(n-2)(n-3)}{n(n-1)(n-2)(n-3)} = \frac{1}{8} \]
∴ n = 8
Step 3:
\[ {}^nP_{m+1} + {}^{n+1}C_m = {}^8P_3 + {}^9C_2 \]
\[ = 8 \times 7 \times 6 + \frac{9 \times 8}{2} \]
\[ = 372 \]
Solve the combination equation. Given:
\[ ^6C_m + 2 \left(^6C_{m+1}\right) + ^6C_{m+2} = 8 \times ^8C_3. \]
First, calculate \( ^8C_3 \):
\[ ^8C_3 = \frac{8!}{3!(8 - 3)!} = \frac{8 \times 7 \times 6}{3 \times 2 \times 1} = 56. \]
So,
\[ ^6C_m + 2(^6C_{m+1}) + ^6C_{m+2} = 8 \times 56 = 448. \]
Using values of \( m \) that satisfy this equation, we find \( m = 2 \).
Solve the permutation ratio equation. Given:
\[ \frac{n-1P_3}{nP_4} = \frac{1}{8}. \]
This implies:
\[ n-1P_3 = \frac{nP_4}{8}. \]
After evaluating this ratio, we find \( n = 8 \).
Calculate \( nP_{m+1} + n^{+1}C_m \). Now, \( m = 2 \) and \( n = 8 \):
\[ nP_{m+1} = ^8P_3 = \frac{8!}{(8 - 3)!} = \frac{8 \times 7 \times 6}{1} = 336. \]
\[ n+1C_m = ^9C_2 = \frac{9 \times 8}{2} = 36. \]
Thus,
\[ nP_{m+1} + n^{+1}C_m = 336 + 36 = 372. \]
Therefore, the answer is: 372
If all the words with or without meaning made using all the letters of the word "KANPUR" are arranged as in a dictionary, then the word at 440th position in this arrangement is:
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
