To solve the problem, we need to balance the magnetic force with the electric force to ensure the electron continues in a straight line. The equation for magnetic force is \(F_{\text{magnetic}}=qvB\) and for electric force is \(F_{\text{electric}}=qE\). Setting \(F_{\text{magnetic}}=F_{\text{electric}}\), we get \(qvB=qE\), thus \(E=vB\).
First, we find the velocity \(v\) of the electron using its kinetic energy:
\(K.E.=\frac{1}{2}mv^2=5 \, \text{eV}=5 \times 1.6 \times 10^{-19} \, \text{J}\).
Rearranging gives:
\(v^2=\frac{2 \times 5 \times 1.6 \times 10^{-19}}{9 \times 10^{-31}}\)
Calculating \(v\), we find:
\(v=\sqrt{\frac{16 \times 10^{-19}}{9 \times 10^{-31}}}\approx1.32 \times 10^6 \, \text{ms}^{-1}\)
Now calculate \(E\) using \(E=vB\) with \(B=3 \, \mu\text{T}=3 \times 10^{-6} \, \text{T}\):
\(E=1.32 \times 10^6 \times 3 \times 10^{-6}=3.96 \, \text{NC}^{-1}\)
The calculated electric field \(E\approx3.96 \, \text{NC}^{-1}\) falls within the given range 4,4, confirming it is acceptable. The electromagnetic forces are balanced, indicating the electron continues its path undeviated.
For the given condition of moving undeflected, the net force should be zero:
\[qE = qvB \implies E = vB\]
The velocity $v$ can be expressed in terms of kinetic energy:
\[v = \sqrt{\frac{2KE}{m}}\]
Substituting this into the expression for $E$:
\[E = \sqrt{\frac{2KE}{m}} \cdot B\]
Substituting the given values:
\[E = \sqrt{\frac{2 \cdot 5 \cdot 1.6 \times 10^{-19}}{9 \times 10^{-31}}} \cdot 3 \times 10^{-6}\]
Calculating:
\[E = \sqrt{\frac{16 \times 10^{-19}}{9 \times 10^{-31}}} \cdot 3 \times 10^{-6}\]
\[E = \sqrt{\frac{1.6 \times 10^{12}}{9}} \cdot 3 \times 10^{-6}\]
\[E = \sqrt{1.78 \times 10^{12}} \cdot 3 \times 10^{-6}\]
\[E = 4 \, \text{N/C}\]
Final Answer: $E = 4 \, \text{N/C}$.
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,

| List I | List II |
|---|---|
| A. \( \oint \vec{B} \cdot d\vec{l} = \mu_0 i_c + \mu_0 \epsilon_0 \frac{d\phi_E}{dt} \) | I. Gauss' law for electricity |
| B. \( \oint \vec{E} \cdot d\vec{l} = -\frac{d\phi_B}{dt} \) | II. Gauss' law for magnetism |
| C. \( \oint \vec{E} \cdot d\vec{A} = \frac{Q}{\epsilon_0} \) | III. Faraday law |
| D. \( \oint \vec{B} \cdot d\vec{A} = 0 \) | IV. Ampere – Maxwell law |

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 : \(A_2 \rightleftharpoons 2A\)