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QJEEM19Phf7e1: JEE Main 2019 Physics - Class 12 JEEM19Phf7e1 Solution: The magnetic field of an electromagnetic wave is given by :-…

The magnetic field of an electromagnetic wave is given by :-

B→=1.6×10−6cos⁡(2×107z+6×1015t)(2i∧+j∧)Wbm2\mathop B\limits^ \to = 1.6 \times {10^{ - 6}}\cos \left( {2 \times {{10}^7}z + 6 \times {{10}^{15}}t} \right)\left( {2\mathop i\limits^ \wedge + \mathop j\limits^ \wedge } \right){{Wb} \over {{m^2}}}

The associated electric field will be :-

Multiple Choice Options

  • A E→=4.8×102cos⁡(2×107z−6×1015t)(−2i∧+j∧)Vm\mathop E\limits^ \to = 4.8 \times {10^2}\cos \left( {2 \times {{10}^7}z - 6 \times {{10}^{15}}t} \right)\left( -2{\mathop i\limits^ \wedge + \mathop {j}\limits^ \wedge } \right){V \over m}
  • B E→=4.8×102cos⁡(2×107z−6×1015t)(2i∧+j∧)Vm\mathop E\limits^ \to = 4.8 \times {10^2}\cos \left( {2 \times {{10}^7}z - 6 \times {{10}^{15}}t} \right)\left( 2{\mathop i\limits^ \wedge + \mathop {j}\limits^ \wedge } \right){V \over m}
  • C E→=4.8×102cos⁡(2×107z+6×1015t)(i∧−2j∧)Vm\mathop E\limits^ \to = 4.8 \times {10^2}\cos \left( {2 \times {{10}^7}z + 6 \times {{10}^{15}}t} \right)\left( {\mathop i\limits^ \wedge - \mathop {2j}\limits^ \wedge } \right){V \over m}
  • D E→=4.8×102cos⁡(2×107z+6×1015t)(−i∧+2j∧)Vm\mathop E\limits^ \to = 4.8 \times {10^2}\cos \left( {2 \times {{10}^7}z + 6 \times {{10}^{15}}t} \right)\left( -{\mathop i\limits^ \wedge + \mathop {2j}\limits^ \wedge } \right){V \over m}

Step-by-Step Verified Solution

If we use that direction of light propagation will be along E→×B→\overrightarrow E \times \overrightarrow B . Then (A) option is correct.
Magnitude of E = CB

E = 3 × 108 × 1.6 × 10–6 × 5\sqrt 5

E = 4.8 × 1025{10^{2\sqrt 5 }}

E→\overrightarrow E and B→\overrightarrow B are perpendicular to each other

⇒E→.B→=0\Rightarrow \overrightarrow E .\overrightarrow B = 0

⇒\Rightarrow Either direction of E→\overrightarrow E i^−2j^\widehat i - 2\widehat j or −i^+2j^-\widehat i + 2\widehat j from given option

Also wave propagation direction is parallel to E→×B→\overrightarrow E \times \overrightarrow B which is −k^- \widehat k

⇒\Rightarrow E→\overrightarrow E is along ( −i^+2j^-\widehat i + 2\widehat j )

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