We are given that the force experienced by the electron is proportional to the velocity, and the velocity of the electron is related to the kinetic energy. The kinetic energy is given by the potential difference through which the electron is accelerated. The force is directly proportional to the velocity in a uniform magnetic field.
Step 1: The kinetic energy acquired by the electron is given by: \[ KE = eV_1 \] where \( e \) is the charge of the electron, and \( V_1 \) is the initial potential difference. The velocity of the electron is: \[ v_1 = \sqrt{\frac{2eV_1}{m}}. \] The force \( F \) experienced by the electron in the magnetic field is given by: \[ F = evB. \]
Step 2: For the second potential difference \( V_2 \), the velocity becomes: \[ v_2 = \sqrt{\frac{2eV_2}{m}}. \] The force experienced by the electron is: \[ F_2 = ev_2B = e\sqrt{\frac{2eV_2}{m}}B. \] We are given that \( F_2 = 2F \), so: \[ 2F = F_2 = ev_2B. \]
Step 3: Now, using the ratio of forces: \[ \frac{F_2}{F} = \frac{v_2}{v_1} = \frac{\sqrt{\frac{2eV_2}{m}}}{\sqrt{\frac{2eV_1}{m}}} = \sqrt{\frac{V_2}{V_1}}. \] Since \( F_2 = 2F \), we have: \[ \sqrt{\frac{V_2}{V_1}} = 2. \] Squaring both sides gives: \[ \frac{V_2}{V_1} = 4. \] Thus, the ratio of potential differences is \( \frac{V_2}{V_1} = 4 : 1 \).
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