Why is the equation for KVL not -vR + vL = 0 in this RL circuit?

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The discussion centers on the confusion regarding the application of Kirchhoff's Voltage Law (KVL) in an RL circuit. The derived equation, Ri + vL = 0, leads to vR + vL = 0, which is correct for the series connection of the resistor (R) and inductor (L). The key point is that while the components share the same current, they are not in parallel; they are in series, meaning the voltage across them must sum to zero. The sign convention used for the voltage across the resistor accounts for the direction of current flow. Understanding the relationship between current and voltage in series circuits clarifies the correct application of KVL.
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Not really a problem, but we're learning about source-free RL circuits and the instructor was deriving the current w.r.t time. I've actually seen this derived a few times but one thing has always bothered me.

Looking at this picture recreated from the text

http://homebrew.net.nz/RL.png

The equation dervied from it says:

Ri + vL = 0

which implies vR + vL = 0

but I've always thought that with KVL you simply write down the first sign you hit when tranversing the circuit, i.e., why is the equation not

-vR + vL = 0

Surely since the two components are in parallel the voltage drop across them has to be equal??!

Thanks if anyone can clear up my confusion
 
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caesius said:
Surely since the two components are in parallel the voltage drop across them has to be equal??!

They are in series. We want to say that the currents through
L and R are equal. We use this circulating current direction as
our sign convention for vL and vR.
vL +vR = 0
 
Since the direction of i is defined opposite to the actual current you'd get with a positive voltage across R, we have

VR = - i R


Equate this expression with VL and see what you get.

p.s. FYI, in this case the two elements are both in parallel (same voltage) and in series (same current).
 
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