Ratio of specific heat of gas at constant volume to the specific heat of gas at constant pressure :
Specific heat of gas constant volume : \(C_v = \frac{nR}2\)
Again, Specific heat of gas at constant pressure : \(C_p = \frac{nR}{2+R}\)
\(⇒ \frac{C_v}{C_p}\)
= \(\frac{\frac{nR}{2}}{\frac{nR}{2+R}}\)
= \(\frac{n}{n+2}\)
Hence, the correct option is (A): \(\frac{n}{n+2}\)
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
The gas laws were developed at the end of the 18th century, when scientists began to realize that relationships between pressure, volume and temperature of a sample of gas could be obtained which would hold to approximation for all gases.