No way man! Educate me at least, I want to know more.
Well, ok, but YOU asked for it!
First thing to understand is that impedance is related, but
distinctly different to resistance. Resistance is only for DC voltages, impedance is for AC voltages. Audio signals are AC voltages, hence, we deal with impedance. Impedance is also frequency dependent, so it can vary depending on the frequency of the input signal - in fact, different frequency components making up a signal will "see" different impedances. Thus, impedance is
never completely constant over a range of frequencies.
So, when a manufacturer gives a single value as an input impedance, it is actually a nominal or average value of the measured impedance over a range of frequencies. The true impedance over a range of frequencies can only be properly represented by a a graph of impedance vs. frequency. But this is very rarely, if ever given, especially in the context of musical equipment.
Input impedance is in parallel with the signal - Output impedance is in series with the signal. Below is an amplifier, with an input and output impedance represented by resistors.
Code:
|\ ___
--o--| >--|___|--
| |/
.-.
| |
| |
'-'
|
|
===
GND
For most audio applications the ideal is to have a very high input impedance, and a very low output impedance - this gives the best transfer of voltage from one stage to the next. A high input impedance means that more of the signal will pass directly into the amplifier, rather than being 'lost' to ground via the impedance. A low output impedance means the amplifier can produce a stronger output signal before it reaches the limits of it's operation. Notice how the high input impedance is in parallel with the signal - stopping the signal from being 'lost' to ground. Also note how the low output impedance is in series with the signal, directly 'impeding' it's passage through the circuit. Already you can see
why it's important to have a high input and low output impedance.
Now, I could blather on all day, but the important thing for most of us to understand is how impedances interact. So, let's put two amplifiers together.
Code:
|\ ___ |\ ___
--o--| >--|___|-------| >--|___|-
| |/ | |/
.-. .-.
| | | |
| | | |
'-' '-'
| |
| |
=== ===
GND GND
Notice now that the output impedance of the first amp is connected directly to the input impedance of the second amp. The first amplifier is generating the signal, the signal on it's way to the next stage passes through the output impedance, and then encounters the next stages input impedance, before entering the 2nd amplifier. This can be represented like this:
Code:
SIGNAL
o
|
.-.
| |
| |
'-'
|
o-----o TO NEXT STAGE
|
.-.
| |
| |
'-'
|
|
===
GND
This arrangement looks just like a thing called a voltage divider - which literally 'divides' a given voltage by the ratio of the two resistances. This is the crux of the whole matter, so PAY ATTENTION!!!
Lets look at the ideal situation; the output impedance (top resistor) is 0 ohms - in other words, it's not even there, it's a short circuit, or just a piece of wire. The input impedance (bottom resistor) is infinitely high - or in other words, it's not there either, as if it's been removed from the circuit - an 'open circuit.' So, what you end up with is just a wire direct from output to input - the resistors effectively do not exist and ALL of the signal passes to the next stage.
The voltage divider ratio in this case is calculated as infinity divided by infitiy+0, which is equal to 1. The next stage see the input signal times the divider ratio (ie; input x 1 = output)
Sadly, this ideal situation does not exist in reality, it's purely theoretical. In reality you might have, for example, an output impedance of 100 ohms, and an input impedance of 10,000 ohms. The ratio of this arrangement is 10,000 divided by 10,000+100, which is 0.99. This is still a very good result as the output equals 0.99 of the input (ie; output = input x 0.99).
10,000 / (10,000 + 100) = 0.99
Now lets imagine we replace the first amplifier stage with a passive bass guitar pickup. Passive pickups by design have a very high output impedance - maybe something like 2,000 ohms. Now the ratio is;
10,000 / (10,000 + 2000) = 0.83
output = 0.83 x input
Suddenly, it's not looking quite as good. Reducing the input impedance has a similar effect. Lets go back to a 100 ohm output impedance, but lets reduce the input impedance to 1,000 ohms.
1,000 / (1,000 + 100) = 0.91
Now, imagine the worst of both, so input impedance is 1,000 ohms, output impedance is 2,000 ohms - notice now the output impedance is higher than the input impedance.
1,000 / (1,000 + 2,000) = 0.33
Ick! 2/3 of your signal is being lost, shunted to ground, gone forever.
Hopefully that's just enough to illustrate the concept for you. Keep in mind that all of this is frequency dependent, so just knowing a devices average input impedance doesn't necessarily mean it will respond equally to all frequencies.