Re: Quick quiestion on External Cabnets
Lot of variables involved. Technically, by adding a 1x12, you're cutting the power each speaker receives in half, but doubling the total surface area of the speaker cones pushing air. Considering just these two things, it's a wash.
However, all things are not equal. One other major thing that changes is the total impedance of your speaker system. By adding a second cabinet in parallel, you reduce the impedance of the speaker circuit, therefore given the same voltage produced by the amplifier, more current (and thus more power) flows to the speakers. If both speakers are the same impedance (say 16 ohms), adding the second one cuts impedance in half (1/Rt = 1/R1 + 1/R2, so 1/16 + 1/16 = 1/8), so ideally given the same voltage, double the current flows, and watts equals volts times amps so we get double the power. In reality it's not quite double, but it's close enough to say that you can expect about a 3dB increase in volume by adding a second cabinet of equal speaker surface area and impedance to your existing rig.
So really, what you're doing by taking a 5W 1x12 guitar combo and running it through an additional 1x12 is turning it into a 10W head (or, if the amp was rated 5W at 8 ohms and you had been running it at 16ohms, you're turning a 2.5W head into 5W).
Another huge variable is speaker sensitivity. This is a measure of how efficiently the speaker will transform the power you give it into acoustic sound waves. The number you get is the sound pressure level you'd experience standing one meter away from the speaker while it is being given a signal of 1WRMS power at the speaker's resonant peak frequency. Double the wattage, you get a 3dB increase in SPL all other things being equal. Double the distance, you get a 6dB decrease. This means that a 97dB-sensitivity speaker sounds half as loud as a 107dB-sensitivity speaker. If the speaker cabinet you add is more sensitive than the one in the first cabinet, volume will increase by more than 3dB because the speaker is more efficiently transforming the power it gets into sound.
Lastly, sensitivity isn't constant. As guitarists, we're familiar with the concept of "peaking" or "clipping". Typically we think of this being a property of the transistors (tubes or solid-state) in the amplifier, where given a stronger input the output does not increase by a proportional amount, because the transistor simply cannot provide it. However, a similar thing happens with speakers; as the power increases, the forces within the speaker chassis designed to keep the voice coil from shooting the cone out into the audience begin hindering the cone's movement and so the marginal increase in volume doesn't match the marginal increase in power. This is more of an issue when running speakers much closer to their peak power rating than you'd ever get with a 5W amp and a garden-variety Eminence or Celestion, but even at lower power levels, if double the power doesn't equal double the volume, then spreading that power across more cones will get you more volume than trying to push it all through one cone.
Originally posted by TRex
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However, all things are not equal. One other major thing that changes is the total impedance of your speaker system. By adding a second cabinet in parallel, you reduce the impedance of the speaker circuit, therefore given the same voltage produced by the amplifier, more current (and thus more power) flows to the speakers. If both speakers are the same impedance (say 16 ohms), adding the second one cuts impedance in half (1/Rt = 1/R1 + 1/R2, so 1/16 + 1/16 = 1/8), so ideally given the same voltage, double the current flows, and watts equals volts times amps so we get double the power. In reality it's not quite double, but it's close enough to say that you can expect about a 3dB increase in volume by adding a second cabinet of equal speaker surface area and impedance to your existing rig.
So really, what you're doing by taking a 5W 1x12 guitar combo and running it through an additional 1x12 is turning it into a 10W head (or, if the amp was rated 5W at 8 ohms and you had been running it at 16ohms, you're turning a 2.5W head into 5W).
Another huge variable is speaker sensitivity. This is a measure of how efficiently the speaker will transform the power you give it into acoustic sound waves. The number you get is the sound pressure level you'd experience standing one meter away from the speaker while it is being given a signal of 1WRMS power at the speaker's resonant peak frequency. Double the wattage, you get a 3dB increase in SPL all other things being equal. Double the distance, you get a 6dB decrease. This means that a 97dB-sensitivity speaker sounds half as loud as a 107dB-sensitivity speaker. If the speaker cabinet you add is more sensitive than the one in the first cabinet, volume will increase by more than 3dB because the speaker is more efficiently transforming the power it gets into sound.
Lastly, sensitivity isn't constant. As guitarists, we're familiar with the concept of "peaking" or "clipping". Typically we think of this being a property of the transistors (tubes or solid-state) in the amplifier, where given a stronger input the output does not increase by a proportional amount, because the transistor simply cannot provide it. However, a similar thing happens with speakers; as the power increases, the forces within the speaker chassis designed to keep the voice coil from shooting the cone out into the audience begin hindering the cone's movement and so the marginal increase in volume doesn't match the marginal increase in power. This is more of an issue when running speakers much closer to their peak power rating than you'd ever get with a 5W amp and a garden-variety Eminence or Celestion, but even at lower power levels, if double the power doesn't equal double the volume, then spreading that power across more cones will get you more volume than trying to push it all through one cone.
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