Jahnavi
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The discussion revolves around the behavior of two diodes, specifically a Germanium and a Silicon diode, connected in parallel within a circuit. Participants explore how the applied voltage affects which diode conducts and the potential differences across them under various conditions.
The discussion is active, with participants providing insights into diode behavior and questioning assumptions about voltage distribution in the circuit. There is a mix of agreement and differing interpretations regarding the voltage across the diodes when current is not flowing.
Some participants reference ideal component behavior and Kirchhoff's laws, while others express confusion about the implications of voltage across non-conducting diodes. The conversation highlights the complexities of circuit theory and the instantaneous nature of voltage changes in response to current flow.
Whie I agree with the rest of your explanation, I don't see how we can say 12V will appear across the diodes initially. When the equilibrium charge distribution builds up at the pn junction and surface charge distribution builds up on Ohmic components (resistors, wires), there is no way we can compute voltage across any component. It's all chaos for that very very short time. Even if we assume the diode junctions to be capacitances, I don't think we can say initially all the 12V appear across the junctions. I believe this process is very different, extremely short-lived and hence, can't be described by the steady state quantities like V and I.ehild said:Yes, at the instant the switch gets closed the initial current is zero, and 12 V appears across the diodes, but the diodes and all the circuit do not behave as ideal ones. The p-n junctions of the diodes behave as capacitors and all wires behave as resistors and inductors. There will be some transient current in the circuit (till the equilibrium charge distribution builds up at the p-n junctions) which ends in the stationary voltage drop across the diodes and stationary current in the circuit in a very short time.
Yes, you are right, we can not use the steady-state quantities in the circuit, but the 12 V emf is applied at the instant of switching up. Even the diode have inductance and resistance because of the leads and the bulk of the semiconductor, so not all the voltage drop appears across the pn-junction or even across the diode because of the inductance of all the wires and the resistor.cnh1995 said:Whie I agree with the rest of your explanation, I don't see how we can say 12V will appear across the diodes initially. When the equilibrium charge distribution builds up at the pn junction and surface charge distribution builds up on Ohmic components (resistors, wires), there is no way we can compute voltage across any component. It's all chaos for that very very short time. Even if we assume the diode junctions to be capacitances, I don't think we can say initially all the 12V appear across the junctions. I believe this process is very different, extremely short-lived and hence, can't be described by the steady state quantities like V and I.
Agreed. And the earlier discussion of a 'perfect 12V battery' applied to a 'perfect 0.3V Vf diode' isn't a useful real-world model. It's the same as a 'perfect battery' connected to a 'perfect conductor', or the theoretical infinite force applied to an infinite mass. It is undefined. One or the other has to 'give'.CWatters said:A lot comes down to which model of a diode you are using. The problem statement provides very little information so you have to assume a very crude model, almost an ideal diode but with a defined forward voltage.