Based on Heisenberg's uncertainty principle, the uncertainty in the velocity of the electron to be found within an atomic nucleus of diameter \( 10^{-15} \, \text{m} \) is \( \dots \dots \times 10^9 \, \text{ms}^{-1} \) (nearest integer). \[ \text{[Given: mass of electron} = 9.1 \times 10^{-31} \, \text{kg, Planck's constant (} h \text{)} = 6.626 \times 10^{-34} \, \text{Js]} \] \[ \text{(Value of } \pi = 3.14) \]
To find the uncertainty in the velocity of an electron within an atomic nucleus using Heisenberg's uncertainty principle, we have: \[\Delta x \cdot \Delta p \geq \frac{h}{4\pi}\] where \(\Delta x\) is the uncertainty in position and \(\Delta p\) is the uncertainty in momentum. Given \(\Delta x = 10^{-15} \, \text{m}\), we want to find \(\Delta v\), the uncertainty in velocity. \(\Delta p = m \cdot \Delta v\), where \(m\) is the mass of the electron.
Plug in the known values: \[\Delta x \cdot m \cdot \Delta v \geq \frac{h}{4\pi}\] \[10^{-15} \cdot 9.1 \times 10^{-31} \cdot \Delta v \geq \frac{6.626 \times 10^{-34}}{4 \times 3.14}\]
Calculate the right-hand side: \[\frac{6.626 \times 10^{-34}}{12.56} \approx 5.274 \times 10^{-35}\]
Substitute and solve for \(\Delta v\): \[10^{-15} \cdot 9.1 \times 10^{-31} \cdot \Delta v \geq 5.274 \times 10^{-35}\]
Rearrange to solve for \(\Delta v\): \[\Delta v \geq \frac{5.274 \times 10^{-35}}{9.1 \times 10^{-46}}\] \[\Delta v \geq 5.796 \times 10^{10} \, \text{m/s}\]
Express \(\Delta v\) in scientific notation to the nearest integer: \[5.796 \times 10^{10} \approx 58 \times 10^9 \, \text{m/s}\]
Thus, the uncertainty in the velocity of the electron is \(58 \times 10^9 \, \text{ms}^{-1}\). Verifying this value falls within the expected range, we conclude the calculation aligns perfectly with the expected outcome.
From Heisenberg's uncertainty principle:
\[ \Delta x \cdot m_e \cdot \Delta v \geq \frac{h}{4\pi} \]
Here:
\[ \Delta x = 10^{-15} \, \text{m}, \quad m_e = 9.1 \times 10^{-31} \, \text{kg}, \quad h = 6.626 \times 10^{-34} \, \text{Js}. \]
Rearranging for the uncertainty in velocity ($\Delta v$):
\[ \Delta v \geq \frac{h}{4\pi \cdot \Delta x \cdot m_e} \]
Substitute the values:
\[ \Delta v \geq \frac{6.626 \times 10^{-34}}{4 \cdot 3.14 \cdot (10^{-15}) \cdot (9.1 \times 10^{-31})} \]
Simplify the denominator:
\[ 4 \cdot 3.14 \cdot 10^{-15} \cdot 9.1 \times 10^{-31} = 1.143 \times 10^{-44} \]
Substitute back:
\[ \Delta v \geq \frac{6.626 \times 10^{-34}}{1.143 \times 10^{-44}} = 5.8 \times 10^{10} \, \text{ms}^{-1} \]
Uncertainty in velocity:
\[ \Delta v = 58 \times 10^9 \, \text{ms}^{-1} \]
Final Answer: 58.
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 : \(A_2 \rightleftharpoons 2A\)

Cobalt chloride when dissolved in water forms pink colored complex $X$ which has octahedral geometry. This solution on treating with cone $HCl$ forms deep blue complex, $\underline{Y}$ which has a $\underline{Z}$ geometry $X, Y$ and $Z$, respectively, are
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 : \(A_2 \rightleftharpoons 2A\)
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,