To solve the problem of finding the value of the series \( \frac{1}{2!} + \frac{2}{3!} + \frac{3}{4!} + \ldots + \frac{99}{100!} \), we can recognize a pattern in how each term is constructed.
Each term in the series can be expressed as follows:
\(\frac{k}{(k+1)!} = \frac{k+1-1}{(k+1)!} = \frac{k+1}{(k+1)!} - \frac{1}{(k+1)!}\)
This identity simplifies to:
\(\frac{k}{(k+1)!} = \frac{1}{k!} - \frac{1}{(k+1)!}\)
Using this transformation, the series becomes a telescoping series:
\(\left(\frac{1}{1!} - \frac{1}{2!}\right) + \left(\frac{1}{2!} - \frac{1}{3!}\right) + \dots + \left(\frac{1}{99!} - \frac{1}{100!}\right)\)
Observe that all intermediate terms cancel each other out, leaving:
\(\frac{1}{1!} - \frac{1}{100!}\)
Therefore, the sum of the series is:
\(1 - \frac{1}{100!}\)
To express this sum in the form of a single fraction:
\(1 - \frac{1}{100!} = \frac{100!}{100!} - \frac{1}{100!} = \frac{100! - 1}{100!}\)
Thus, the value of the series is \( \frac{100! - 1}{100!} \).
The correct answer is therefore:
\( \frac{100! - 1}{100!} \)
The given series is:
\(\frac{1}{2!} + \frac{2}{3!} + \frac{3}{4!} + \cdots + \frac{99}{100!}\)
We can denote this sum by \( S \):
\( S = \sum_{n=2}^{100} \frac{n-1}{n!} \)
Rewriting each term:
\(\frac{n-1}{n!} = \frac{n}{n!} - \frac{1}{n!} = \frac{1}{(n-1)!} - \frac{1}{n!}\)
Substitute this expression back into the sum:
\( S = \sum_{n=2}^{100} \left( \frac{1}{(n-1)!} - \frac{1}{n!} \right) \)
This is a telescoping series. Most terms will cancel out, leaving:
\( S = 1 - \frac{1}{100!} \)
By simplifying, we have:
\( S = \frac{100!}{100!} - \frac{1}{100!} = \frac{100! - 1}{100!} \)
Thus, the value of the series is \(\frac{100! - 1}{100!}\)
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: