In a radiation field with electrical & magnetic field (E,, B,), we put an electron into this radiation field, the electron would experience the Lorentz force and thus be accelerated via Newton's second law: mã = f = -e(E, +ü x B.). Since B, - LE, the Lorentz force due to the magnetic component B, can be neglected for slow motion (i.e. v/c < 1). After the electron is accelerated, it will irradiate to generate a radiation field. Assuming E, = E0 Cos(wt +a). Please answer the following questions:
In a radiation field with electrical & magnetic field (E,, B,), we put an electron into this radiation field, the electron would experience the Lorentz force and thus be accelerated via Newton's second law: mã = f = -e(E, +ü x B.). Since B, - LE, the Lorentz force due to the magnetic component B, can be neglected for slow motion (i.e. v/c < 1). After the electron is accelerated, it will irradiate to generate a radiation field. Assuming E, = E0 Cos(wt +a). Please answer the following questions:
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