To find the potential at the center of a half ring of radius \( R = 10 \, \text{cm} \) with a linear charge density \( \lambda = 4 \, \text{nC} \, \text{m}^{-1} \), we use the formula for the electric potential due to a charged arc: \( V = \frac{k \lambda L}{R} \), where \( k \) is Coulomb's constant \( \left( 8.99 \times 10^9 \, \text{Nm}^2/\text{C}^2 \right) \), \( L \) is the arc length of the half ring, and \( R \) is the radius. The arc length \( L \) for a half ring is \( \pi R \).
First, convert the given linear charge density to coulombs per meter: \( \lambda = 4 \times 10^{-9} \, \text{C/m} \). The radius is \( R = 0.1 \, \text{m} \).
The arc length \( L = \pi R = \pi \times 0.1 \, \text{m} = 0.1\pi \, \text{m} \).
Substituting the values into the potential formula, we have:
\( V = \frac{(8.99 \times 10^9) \times (4 \times 10^{-9}) \times (0.1\pi)}{0.1} \).
Simplifying, \( V = 8.99 \times 4 \times \pi \).
Calculating gives \( V = 35.96\pi \, \text{V} \).
We identify \( V = x\pi \) and solve for \( x \), yielding \( x = 35.96 \).
Round \( x \) to the nearest whole number: \( x = 36 \).
This solution fits within the expected range of 36,36.
The potential at the center of a half-ring is given by:
\( V = \frac{KQ}{R} \)
where:
Substituting:
\( V = \frac{K \lambda \pi R}{R} \)
\( V = K \lambda \pi \)
Given:
\( V = 9 \times 10^9 \cdot 4 \times 10^{-9} \cdot \pi \)
\( V = 36\pi \, \text{V} \)
Thus, \( x = 36 \).
Final Answer: \( x = 36 \).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,


What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)