To solve \(8 = 3 + \frac{1}{4}(3 + p) + \frac{1}{4^2}(3 + 2p) + \frac{1}{4^3}(3 + 3p) + \ldots\), we recognize a geometric series involving the common ratio \( \frac{1}{4} \). Let the series be \( S \), where \( S = 3 + \sum_{n=1}^{\infty} \frac{1}{4^n}(3+np) \). We split it into two separate series: \[ S = 3 + \sum_{n=1}^{\infty} \frac{3}{4^n} + \sum_{n=1}^{\infty} \frac{np}{4^n} \] The first series is geometric with first term \( a = \frac{3}{4} \) and common ratio \( r = \frac{1}{4} \). The sum of this infinite geometric series is: \[ \sum_{n=1}^{\infty} \frac{3}{4^n} = \frac{\frac{3}{4}}{1 - \frac{1}{4}} = \frac{3}{4} \times \frac{4}{3} = 1 \] The second series is an arithmetico-geometric series. Its sum can be found using the formula: \[ \sum_{n=1}^{\infty} \frac{n}{r^n} = \frac{r}{(1-r)^2} \text{, for } x = \frac{1}{4} \] Plugging in, we get: \[ \sum_{n=1}^{\infty} \frac{np}{4^n} = \frac{\frac{1}{4}}{(1 - \frac{1}{4})^2} \times p = \frac{\frac{1}{4}}{\frac{9}{16}} \times p = \frac{4}{9}p \] Substituting back into the equation, the series sum becomes: \[ S = 3 + 1 + \frac{4}{9}p = 8 \] Simplifying gives us: \[ 4 + \frac{4}{9}p = 8 \] \[ \frac{4}{9}p = 4 \] \[ p = 9 \] Thus, the value of \( p \) is 9. This value falls within the given range \([9,9]\), confirming our solution is correct.
The sum $ 1 + \frac{1 + 3}{2!} + \frac{1 + 3 + 5}{3!} + \frac{1 + 3 + 5 + 7}{4!} + ... $ upto $ \infty $ terms, is equal to
If $ \frac{1}{1^4} + \frac{1}{2^4} + \frac{1}{3^4} + ... \infty = \frac{\pi^4}{90}, $ $ \frac{1}{1^4} + \frac{1}{3^4} + \frac{1}{5^4} + ... \infty = \alpha, $ $ \frac{1}{2^4} + \frac{1}{4^4} + \frac{1}{6^4} + ... \infty = \beta, $ then $ \frac{\alpha}{\beta} $ is equal to:
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 