We are given the formula for wavenumber:
Let's simplify the equation step by step:
Thus, the wavenumber is 1724 cm-1.
The wavenumber ($\tilde{\nu}$) is given by:
\[ \tilde{\nu} = \frac{1}{\lambda}, \]
where $\lambda$ is the wavelength in cm.
Step 1: Convert wavelength to cm
\[ \lambda = 5800 \, \text{\AA} = 5800 \times 10^{-8} \, \text{cm}. \]
Step 2: Calculate wavenumber
\[ \tilde{\nu} = \frac{1}{5800 \times 10^{-8}} = \frac{1}{5.8 \times 10^{-5}} = 17241 \, \text{cm}^{-1}. \]
Step 3: Express as $x \times 10 \, \text{cm}^{-1}$
\[ 17241 \, \text{cm}^{-1} = 1724 \times 10 \, \text{cm}^{-1}. \]
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
