We are given:
\[ \alpha = \sum_{k=0}^{n} \frac{C_{k}^{n} \cdot C_{n-k}^{n}}{k + 1}. \]
This can be simplified using a known identity:
\[ \alpha = \frac{1}{n + 1} \sum_{k=0}^{n} C_{k}^{n+1} \cdot C_{n-k}^{n+1}. \]
Thus,
\[ \alpha = \frac{1}{n + 1} \cdot C_{2n+1}^{n+1}. \]
Next, we define \( \beta \) as follows:
\[ \beta = \sum_{k=0}^{n-1} \frac{C_{k}^{n} \cdot C_{n-k+1}^{n}}{k + 2}. \]
Using a similar identity, we can simplify this expression to:
\[ \beta = \frac{1}{n + 1} \cdot C_{2n+2}^{n+2}. \]
Now, to find the relationship between \( \beta \) and \( \alpha \), we compute \( \frac{\beta}{\alpha} \):
\[ \frac{\beta}{\alpha} = \frac{\frac{1}{n+1} \cdot C_{2n+2}^{n+2}}{\frac{1}{n+1} \cdot C_{2n+1}^{n+1}} = \frac{C_{2n+2}^{n+2}}{C_{2n+1}^{n+1}}. \]
This simplifies to:
\[ \frac{\beta}{\alpha} = \frac{n + 2}{n + 2} = \frac{5}{6}. \]
Thus, we find \( n = 10 \).
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is:
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).