To determine the fractional compression \( \frac{\Delta V}{V} \) of water at the bottom of the ocean, we start by understanding the relationship given by the definition of the bulk modulus \( B \), which is:
Bulk Modulus Equation:
\( B = -\frac{\Delta P}{\frac{\Delta V}{V}} \)
Where:
We first need to determine the pressure increase \( \Delta P \) at the bottom of the ocean due to the water column. Using the hydrostatic pressure formula, we have:
Hydrostatic Pressure:
\( \Delta P = \rho g h \)
Where:
Substitute the known values:
\[ \Delta P = 1000 \times 10 \times 4000 = 4 \times 10^7 \, \text{N/m}^2 \]
Using the bulk modulus equation, we solve for the fractional change in volume:
\[ \frac{\Delta V}{V} = -\frac{\Delta P}{B} \]
Substitute \( \Delta P \) and \( B \) values:
\[ \frac{\Delta V}{V} = -\frac{4 \times 10^7}{2 \times 10^9} = -0.02 \]
Expressing this in the given format \( \alpha \times 10^{-2} \), we find:
\[ \alpha = 2 \]
Verification:
The computed value of \( \alpha = 2 \) falls within the given range of 2,2, confirming the solution is correct.
The fractional compression \(\frac{\Delta V}{V}\) is given by:
\[ \frac{\Delta V}{V} = -\frac{\Delta P}{B} \]
The pressure \(\Delta P\) at the bottom of the ocean is:
\[ \Delta P = \rho gh = 1000 \times 10 \times 4000 = 4 \times 10^7 \, \text{Pa} \]
Thus,
\[ \frac{\Delta V}{V} = -\frac{4 \times 10^7}{2 \times 10^9} = -2 \times 10^{-2} \]
Therefore, \(\alpha = 2\).
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 : \(A_2 \rightleftharpoons 2A\)