Resistors in Series and Parallel Flashcards
if you had three resistors in series and you could measure the current in between each of them, what would you observe
the current would be the same at every part
why would the current be the same, simply put
because of the conservation of charge
what does the conservation of charge state
- the rate at which electrons leave each component must be the same as the rate in which they enter
- as there is nowhere else for them to go
if you put a voltmeter across all of the resistors at once, then more in between the first, second and third resistor, what relationship would all of the those potential differences have
- the first pd reading equals the sum of all the three other readings
- V = V1 + V2 + V3
how would the equation change if you substituted V for the products of its equation
IR = IR1 + IR2 + IR3
how would you use that equation to prove that resistance of resistors in series add up to make a larger sum of a resistance across the whole circuit
- cancel out the current
- leaving you with R = R1 + R2 + R3
- therefore, the resistance across the whole circuit is equal to the sum of each of the resistances the resistors supply
how is the conservation of charge at a junction, lets say with three different routes, written out in an equation
I = I1 + I2 + 13
- where I is the total current and the others are at the three different routes
if you have a resistor in each route, and I = V / R, how can you rewrite that equation to show the resistance in this circuit
V / R = V / R1 + V / R2 + V / R3
how does the potential difference change when it meets a junction and enters different routes
- it doesnt change
- the potential difference is the same in all routes as well as in series
what could you therefore call V in the equation and how would it be written out
- it could be 1
- giving you 1 / R = 1 / R1 + 1 / R2 + 1 / R3
what does this overall mean about how the resistance changes in series and in parallel
- the resistance increases when in series
- but the resistance decreases in parallel