Step 1: Power radiated as electromagnetic waves
The total power of the bulb is given as: \[ P = 60 W \] Since the efficiency of the bulb is \( 16\% \), the power converted into electromagnetic radiation is: \[ P_{\text{em}} = 0.16 \times 60 = 9.6 W \]
Step 2: Intensity of the electromagnetic waves
The intensity (\( I \)) of the electromagnetic radiation at a distance \( r \) from the source is given by: \[ I = \frac{P_{\text{em}}}{4 \pi r^2} \] Substituting the values: \[ I = \frac{9.6}{4 \pi (2)^2} \] \[ = \frac{9.6}{16 \pi} \] \[ = \frac{0.6}{\pi} \text{ W/m}^2 \]
Step 3: Relation between intensity and peak electric field
The intensity of an electromagnetic wave is related to the peak electric field \( E_0 \) by: \[ I = \frac{1}{2} \epsilon_0 c E_0^2 \] where: - \( \epsilon_0 = 8.85 \times 10^{-12} \text{ C}^2 \text{N}^{-1} \text{m}^{-2} \), - \( c = 3 \times 10^8 \) m/s. Rearranging for \( E_0 \): \[ E_0 = \sqrt{\frac{2I}{\epsilon_0 c}} \] Substituting values: \[ E_0 = \sqrt{\frac{2 \times \frac{0.6}{\pi}}{(8.85 \times 10^{-12}) (3 \times 10^8)}} \] Approximating: \[ E_0 \approx 12 \text{ V/m} \] Thus, the peak value of the electric field is 12 V/m.
When \( |x| < 2 \), the coefficient of \( x^2 \) in the power series expansion of
\[ \frac{x}{(x-2)(x-3)} \]
is:
If the function
\[ f(x) = \begin{cases} \frac{(e^x - 1) \sin kx}{4 \tan x}, & x \neq 0 \\ P, & x = 0 \end{cases} \]
is differentiable at \( x = 0 \), then:
If
\[ A = \{ P(\alpha, \beta) \mid \text{the tangent drawn at P to the curve } y^3 - 3xy + 2 = 0 \text{ is a horizontal line} \} \]
and
\[ B = \{ Q(a, b) \mid \text{the tangent drawn at Q to the curve } y^3 - 3xy + 2 = 0 \text{ is a vertical line} \} \]
then \( n(A) + n(B) = \)