A pane electromagnetic wave travelling along the positive x-direction has a wavelength of 3mm . The variation in the electric field occurs in the y – direction with an amplitude 66 V/m . The equations for the electric and magnetic fields as a function of x and t are respectively . 𝐸_𝑦 = 66 cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑧 = 1.1x 〖10〗^(−7) cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) 𝐸_𝑦 =11 cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑦 = 11x 〖10〗^(−7) cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) 𝐸_𝑥 = 66 cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑥 = 2.2 x 〖10〗^(−7) cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) 𝐸_𝑦 = 66 cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑧 = 2.2 x 〖10〗^(−7) cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 )

A pane electromagnetic wave travelling along the positive x-direction has a wavelength of 3mm . The variation in the electric field occurs in the y – direction with an amplitude 66 V/m . The equations for the electric and magnetic fields as a function of x and t are respectively . 𝐸_𝑦 = 66 cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑧 = 1.1x 〖10〗^(−7) cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) 𝐸_𝑦 =11 cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑦 = 11x 〖10〗^(−7) cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) 𝐸_𝑥 = 66 cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑥 = 2.2 x 〖10〗^(−7) cos 𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) 𝐸_𝑦 = 66 cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 ) , 𝐵_𝑧 = 2.2 x 〖10〗^(−7) cos 2𝜋 x 〖10〗^11(t - 𝑥/𝑐 )

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