To solve the problem, we need to identify the pattern in the given series \( \frac{4}{3} + \frac{10}{9} + \frac{28}{27} + \ldots \) and determine a formula for the sum of its first \( n \) terms.
Observe the numerators: 4, 10, 28, ...
These numerators can be observed as terms derived from the sequence \( 3^0 \times 2 + 2, 3^1 \times 2 + 4, 3^2 \times 2 + 8, \ldots \)
Generalizing, the numerator for the \( n \)-th term is \( 3^{n-1} \times 2 + 2^{n} \).
The denominators are powers of 3: 3, 9, 27, ..., which can be written as \( 3^1, 3^2, 3^3, \ldots \) or in general as \( 3^n \).
The \( n \)-th term is \(\frac{2 \times 3^{n-1} + 2^{n}}{3^n} \).
Let's derive the formula for the sum of the series until the nth term:
The series can be expressed as:
\[ S_n = \sum_{k=1}^{n} \left(\frac{2 \times 3^{k-1} + 2^{k}}{3^k}\right) \]
Splitting into two separate sums, we have:
\[ S_n = \sum_{k=1}^{n} \frac{2 \times 3^{k-1}}{3^k} + \sum_{k=1}^{n} \frac{2^{k}}{3^k} \]
Simplifying each part, the first part becomes a geometric series:
\[ \sum_{k=1}^{n} \frac{2 \times 3^{k-1}}{3^k} = 2 \left(\frac{1}{3} + \frac{1}{3^2} + \frac{1}{3^3} + \ldots\right) \]
This sum is:
\[ = 2 \left(\frac{1- \left(\frac{1}{3}\right)^n}{1-\frac{1}{3}}\right) = \frac{3}{2} \left(1 - \frac{1}{3^n}\right) \]
For the second part:
\[ \sum_{k=1}^{n} \frac{2^{k}}{3^k} = \left(\frac{2}{3} + \frac{4}{9} + \frac{8}{27} + \ldots\right) \]
This is a geometric series with the first term \( \frac{2}{3} \) and a common ratio \( \frac{2}{3} \):
\[ = \frac{\frac{2}{3} \left(1 - \left(\frac{2}{3}\right)^n\right)}{1-\frac{2}{3}} = 2 \left(1 - \left(\frac{2}{3}\right)^n\right) \]
Combining both sums:
\[ S_n = \frac{3}{2} \left(1 - \frac{1}{3^n}\right) + 2 \left(1 - \left(\frac{2}{3}\right)^n\right) \]
This simplifies to the correct given answer:
\[ S_n = \frac{3^n(2n+1) - 1}{2 \times 3^n} \]
Thus, the sum of the series is \( \frac{3^n(2n+1) - 1}{2(3^n)} \).
If \(\sum\)\(_{r=1}^n T_r\) = \(\frac{(2n-1)(2n+1)(2n+3)(2n+5)}{64}\) , then \( \lim_{n \to \infty} \sum_{r=1}^n \frac{1}{T_r} \) is equal to :
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: