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http://en.wikipedia.org/wiki/Euler's_identity
OMGWTFBBQ?!?!?!?!?!?!?!??!!??!!!!!!!!!!!!!!!!!!!!!!!!!!!
OMGWTFBBQ?!?!?!?!?!?!?!??!!??!!!!!!!!!!!!!!!!!!!!!!!!!!!
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I haven't seen "i" since learning about it. Proving it's retarded nature of existance.
/ignorance
No, seeing as it is only made up of 5 known (give or take) constants. But it's pretty crazy.So does this equation have any practical applications?
I haven't seen "i" since learning about it. Proving it's retarded nature of existance.
/ignorance
No, seeing as it is only made up of 5 known (give or take) constants. But it's pretty crazy.
Electrical Engineers use them all the time to calculate imaginary resistances and powers .
?imaginary resistances and powers .
In DC circuits, you can get away with using Ohm's Law: V=IR where V, I and R are all real numbers. When you use AC current (which is like a wave) Ohm's law becomes V=IZ where V, I and Z are all complex numbers (of the form a+ib or r*e^iθ).
Z is based on the components of the circuit. Z for plain resistor is just R, Z for capacitor is 1/iwC (= -i/wc), Z for and inductor is iwL.
If you use Euler's Identity you can easily determine the relationship between V and I. For example, in a circuit with only an inductor and an AC power source:
Z=iwL = wL*e^i(pi/2).
I=I(0)e^iwt
V=IZ = [I(0)e^iwt][wL*e^i(pi/2)]
= I(0)wL*e^i(wt+pi/2)
{as (e^a)*(e^b) = e^(a+b)}
Therefore the voltage leads the current by pi/2.
Alternatively you can use Phasor Diagrams to do the same thing, but the way I just did it is far easier and more direct.
I don't expect you to understand any of this, just know that Euler's Identity definitely does have its uses.
http://en.wikipedia.org/wiki/Euler's_identity
OMGWTFBBQ?!?!?!?!?!?!?!??!!??!!!!!!!!!!!!!!!!!!!!!!!!!!!
Hah, just what I'm studying. Glad to see I'm not alone.In DC circuits, you can get away with using Ohm's Law: V=IR where V, I and R are all real numbers. When you use AC current (which is like a wave) Ohm's law becomes V=IZ where V, I and Z are all complex numbers (of the form a+ib or r*e^iθ).
Z is based on the components of the circuit. Z for plain resistor is just R, Z for capacitor is 1/iwC (= -i/wc), Z for and inductor is iwL.
If you use Euler's Identity you can easily determine the relationship between V and I. For example, in a circuit with only an inductor and an AC power source:
Z=iwL = wL*e^i(pi/2).
I=I(0)e^iwt
V=IZ = [I(0)e^iwt][wL*e^i(pi/2)]
= I(0)wL*e^i(wt+pi/2)
{as (e^a)*(e^b) = e^(a+b)}
Therefore the voltage leads the current by pi/2.
Alternatively you can use Phasor Diagrams to do the same thing, but the way I just did it is far easier and more direct.
I don't expect you to understand any of this, just know that Euler's Identity definitely does have its uses.
just know that Euler's Identity definitely does have its uses.
In DC circuits, you can get away with using Ohm's Law: V=IR where V, I and R are all real numbers. When you use AC current (which is like a wave) Ohm's law becomes V=IZ where V, I and Z are all complex numbers (of the form a+ib or r*e^iθ).
Z is based on the components of the circuit. Z for plain resistor is just R, Z for capacitor is 1/iwC (= -i/wc), Z for and inductor is iwL.
If you use Euler's Identity you can easily determine the relationship between V and I. For example, in a circuit with only an inductor and an AC power source:
Z=iwL = wL*e^i(pi/2).
I=I(0)e^iwt
V=IZ = [I(0)e^iwt][wL*e^i(pi/2)]
= I(0)wL*e^i(wt+pi/2)
{as (e^a)*(e^b) = e^(a+b)}
Therefore the voltage leads the current by pi/2.
Alternatively you can use Phasor Diagrams to do the same thing, but the way I just did it is far easier and more direct.
I don't expect you to understand any of this, just know that Euler's Identity definitely does have its uses.