Step 1: The general term of an A.P. is given by:
\[ a_n = a_1 + (n - 1)d \]
where \( a_1 \) is the first term and \( d \) is the common difference.
Step 2: The general term of a G.P. is given by:
\[ b_n = b_1 r^{n-1} \]
where \( b_1 \) is the first term and \( r \) is the common ratio.
Step 3: We are given that the first and second terms of both progressions are equal, i.e.,
\[ a_1 = b_1 \quad \text{and} \quad a_2 = b_2. \]
- For A.P., \( a_2 = a_1 + d \). For G.P., \( b_2 = b_1 r \).
Equating these:
\[ a_1 + d = b_1 r \]
Since \( a_1 = b_1 \), we get:
\[ d = b_1 (r - 1) \]
Step 4: Now, for \( n > 2 \), the general terms \( a_n \) and \( b_n \) are:
\[ a_n = a_1 + (n - 1)d = b_1 + (n - 1)b_1(r - 1) = b_1 [1 + (n - 1)(r - 1)] \] \[ b_n = b_1 r^{n-1} \]
Step 5: To compare \( a_n \) and \( b_n \), let’s examine their behavior for large \( n \):
If the sum of the first 10 terms of the series \[ \frac{4 \cdot 1}{1 + 4 \cdot 1^4} + \frac{4 \cdot 2}{1 + 4 \cdot 2^4} + \frac{4 \cdot 3}{1 + 4 \cdot 3^4} + \ldots \] is \(\frac{m}{n}\), where \(\gcd(m, n) = 1\), then \(m + n\) is equal to _____.

A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: