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JEE Main
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JEE Main
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Physics
Chapter
Electromagnetic Waves

JEE Main · Physics · Electromagnetic Waves

The radiation energy emitted per second by a point source is 100 ~W...

The radiation energy emitted per second by a point source is 100 W100 \mathrm{~W}. If the efficiency of the source is 4%4 \%, then the rms value of the electric field at distance of 2 m2 \mathrm{~m} is [use 14πε0=9×109\frac{1}{4 \pi \varepsilon_0}=9 \times 10^9 in SI unit]The radiation energy emitted per second by a point source is 100 ~W . If the efficiency of the source is 4 \% , thenThe radiation energy emitted per second by a point source is 100 ~W . If the efficiency of the source is 4 \% , thenThe radiation energy emitted per second by a point source is 100 ~W . If the efficiency of the source is 4 \% , then

Options

  1. A60 V/m\sqrt{60} \mathrm{~V} / \mathrm{m}
  2. B30 V/m\sqrt{30} \mathrm{~V} / \mathrm{m}
  3. C50 V/m\sqrt{50} \mathrm{~V} / \mathrm{m}
  4. D40 V/m\sqrt{40} \mathrm{~V} / \mathrm{m}

Correct answer

B. 30 V/m\sqrt{30} \mathrm{~V} / \mathrm{m}

Step-by-step solution

The radiation energy emitted per second by a point source is 100 ~W . If the efficiency of the source is 4 \% , then
The radiation energy emitted per second by a point source is 100 ~W . If the efficiency of the source is 4 \% , then
where, Pavg =P_{\text {avg }}= average power generated by source =4% of 100 W=4100×100 W=4 WA==4 \% \text { of } 100 \mathrm{~W}=\frac{4}{100} \times 100 \mathrm{~W}=4 \mathrm{~W}A= area to which energy is transmitted =4πr2=4π×(2)2=4π×4=16πm2=4 \pi r^2=4 \pi \times(2)^2=4 \pi \times 4=16 \pi \mathrm{m}^2 On putting the values into Eq. (i), we haveThe radiation energy emitted per second by a point source is 100 ~W . If the efficiency of the source is 4 \% , then
where, ε0=\varepsilon_0= permittivity of free space and Erms=E_{\mathrm{rms}}= root mean square (rms)(\mathrm{rms}) value of electric field. c=c= speed of light in vacuum =3×108 m/s=3 \times 10^8 \mathrm{~m} / \mathrm{s} On putting the values into Eq. (iii), we get Iavg=ε0×Erms2×3×108I_{\mathrm{avg}}=\varepsilon_0 \times E_{\mathrm{rms}}^2 \times 3 \times 10^8 On equating both the Eqs. (ii) and (iv), we get 14π=ε0×Erms2×3×108⇒14πε0×3×108=Erms2Erms2=14πε0×13×108=9×109×13×108(∵14πε0=9×109Nm2/C2)=3×10=30 V/m\begin{gathered} \frac{1}{4 \pi}=\varepsilon_0 \times E_{\mathrm{rms}}^2 \times 3 \times 10^8 \Rightarrow \frac{1}{4 \pi \varepsilon_0 \times 3 \times 10^8}=E_{\mathrm{rms}}^2 \\ E_{\mathrm{rms}}^2=\frac{1}{4 \pi \varepsilon_0} \times \frac{1}{3 \times 10^8}=9 \times 10^9 \times \frac{1}{3 \times 10^8} \\ \quad\left(\because \frac{1}{4 \pi \varepsilon_0}=9 \times 10^9 \mathrm{Nm}^2 / \mathrm{C}^2\right) \\ =3 \times 10=\sqrt{30} \mathrm{~V} / \mathrm{m} \end{gathered}
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