How the current go through this circuit?

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The discussion focuses on the behavior of inductors and resistors in a circuit when a switch is closed. Initially, the current flows through the resistors, but for a long time, it bypasses the 40-ohm resistor due to the inductor's opposition to rapid changes in current, creating a back-emf. This back-emf causes the inductor to act like an open circuit at the moment the voltage is applied, and it transitions to a short circuit once the current stabilizes. The conversation also contrasts this with capacitors, which behave oppositely by appearing as short circuits at the start and open circuits once fully charged. Understanding these principles is essential for analyzing DC circuits involving inductors and capacitors.
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Homework Statement



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The Attempt at a Solution



I don't understand why at the start, I20 was calculated like that, and why for a long time, IL=I20

Does that mean for the instant the switch was closed, the current just went through the resistors? And for a long time, the current skipped 40 ohm resistor? Why was that?

I think this is a basic knowledge but I can't remember what it is.
 

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machinarium said:
I don't understand why at the start, I20 was calculated like that, and why for a long time, IL=I20

Does that mean for the instant the switch was closed, the current just went through the resistors?

Yes.

And for a long time, the current skipped 40 ohm resistor? Why was that?

Yes.

I think this is a basic knowledge but I can't remember what it is.

Inductors "oppose" rapid changes in current through them. It's analogous to inertia. They produce what's called a back-emf, a voltage that opposes the attempted change in current.

V = L*dI/dt

Once the current stops changing, the back-emf goes to zero. At that point the effective resistance (impedance) of the inductor is zero. Note that this only applies to a constant current situation.

So the rule of thumb for inductors in DC circuits is, they look like open circuits when voltage is first applied (usually at t=0), and like short circuits after a long time ("a long time" can be taken to be more than about 5 time constants for the circuit).

For capacitors the opposite holds. They tend to oppose changes in voltage across them, so they look like short circuits at start-up, and when they settle down to their full charge in the (DC) circuit, they look like open circuits.
 
I understand it. Thank you very much, gneill.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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