To find the depth at which the volume of a rubber ball decreases by 0.02%, we use the formula for bulk modulus \(B\):
\[ B = -\frac{\Delta P}{\frac{\Delta V}{V}} \]
where \(\Delta P\) is the change in pressure, and \(\frac{\Delta V}{V}\) is the fractional change in volume.
Given \(\frac{\Delta V}{V} = 0.02\% = \frac{0.02}{100} = 0.0002\).
Rearranging the formula gives:
\[ \Delta P = -B \cdot \frac{\Delta V}{V} \]
Substitute \(B = 9 \times 10^8 \, \text{N m}^{-2}\):
\[ \Delta P = -9 \times 10^8 \times 0.0002 = -1.8 \times 10^5 \, \text{N m}^{-2} \]
The pressure difference \(\Delta P\) is also given by the hydrostatic pressure:\[ \Delta P = \rho g h \]
where \(\rho = 10^3 \, \text{kg m}^{-3}\), \(g = 10 \, \text{m s}^{-2}\), and \(h\) is the depth.
Equating the expressions for \(\Delta P\):
\[ \rho g h = 1.8 \times 10^5 \]
Substituting the known values:
\[ 10^3 \times 10 \times h = 1.8 \times 10^5 \]
\[ 10^4 h = 1.8 \times 10^5 \]
\[ h = \frac{1.8 \times 10^5}{10^4} = 18 \, \text{m} \]
This computed depth of 18 m is within the provided range (18, 18), confirming the solution. Therefore, the depth below the surface of the sea is \(18 \, \text{m}\).
Given:
\[ \beta = -\frac{\Delta P}{\Delta V / V} \] \[ \Delta P = -\beta \frac{\Delta V}{V} \]Pressure difference due to sea water:
\[ \rho g h = -\beta \frac{\Delta V}{V} \]Substituting the given values:
\[ 10^3 \times 10 \times h = -9 \times 10^8 \times \left(-\frac{0.02}{100}\right) \]Simplifying:
\[ h = 18 \, \text{m} \]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 : \(A_2 \rightleftharpoons 2A\)