This problem requires the calculation of the electrode potential for a hydrogen half-cell under non-standard conditions using the Nernst equation.
The Nernst equation is used to determine the cell potential under non-standard conditions. For a general reduction half-reaction:
\[ \text{Ox} + ne^- \rightarrow \text{Red} \]The Nernst equation is given by:
\[ E = E^\circ - \frac{2.303RT}{nF} \log_{10} Q \]Where:
For the standard hydrogen electrode (SHE), the standard reduction potential \(E^\circ\) is defined as 0 V.
Step 1: Identify the given half-reaction and parameters.
The reduction half-reaction is:
\[ 2\text{H}^+ (\text{aq}) + 2e^- \rightarrow \text{H}_2 (\text{g}) \]From this reaction, the number of electrons transferred is \(n=2\).
The given conditions are:
Step 2: Determine the reaction quotient (\(Q\)).
The expression for the reaction quotient for this half-cell is:
\[ Q = \frac{\text{Products}}{\text{Reactants}} = \frac{P_{\text{H}_2}}{[\text{H}^+]^2} \]Substituting the given values:
\[ Q = \frac{2}{(1)^2} = 2 \]Step 3: Apply the Nernst equation.
The Nernst equation for this half-cell is:
\[ E = E^\circ - \frac{0.06}{n} \log_{10} Q \]Now, substitute the known values into the equation:
\[ E = 0 - \frac{0.06}{2} \log_{10} (2) \]Step 4: Calculate the potential \(E\).
Simplify the expression:
\[ E = -0.03 \times \log_{10} (2) \]Using the given value \( \log 2 = 0.3 \):
\[ E = -0.03 \times 0.3 \] \[ E = -0.009 \, \text{V} \]The problem asks for the answer in the format \( (-) \ldots \times 10^{-2} \, \text{V} \). We need to express our calculated potential in this form.
\[ E = -0.009 \, \text{V} = -0.9 \times 10^{-2} \, \text{V} \]The value to be filled in the blank is 0.9.
The potential for the given half cell is \( (-) 0.9 \times 10^{-2} \, \text{V} \).
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: