Step 1: In a single-phase semi-converter, SCRs (Silicon-Controlled Rectifiers) are used for controlled rectification of AC power.
Step 2: The firing angle \( \alpha \) determines when the SCR turns on, and the extinction angle \( \beta \) defines when it turns off.
Step 3: Without a freewheeling diode, the SCR remains conducting until the current naturally falls to zero, which occurs at the extinction angle \( \beta \).
Step 4: The total conduction period of each SCR is given by: \[ \text{Conduction time} = \beta - \alpha \]
Step 5: Evaluating options:
- (A) \( \pi - \alpha \) (Incorrect): This is valid only for continuous conduction mode.
- (B) \( \beta - \alpha \) (Correct): This correctly accounts for the discontinuous conduction mode where conduction stops at \( \beta \).
- (C) \( \alpha \) (Incorrect): The firing angle does not directly indicate conduction time.
- (D) \( \beta \) (Incorrect): The conduction duration is relative to \( \alpha \), not just \( \beta \).
A proton is moving undeflected in a region of crossed electric and magnetic fields at a constant speed of \( 2 \times 10^5 \, \text{m/s} \). When the electric field is switched off, the proton moves along a circular path of radius 2 cm. The magnitude of electric field is \( x \times 10^4 \, \text{N/C} \). The value of \( x \) is \(\_\_\_\_\_\). (Take the mass of the proton as \( 1.6 \times 10^{-27} \, \text{kg} \)).
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: