**Theory**

The third-order intercept point (TOI) is a property of the device transfer function *O* (see diagram). This transfer function relates the output signal voltage level to the input signal voltage level. We assume a “linear” device having a transfer function whose small signal form may be expressed in terms of a power series containing only odd terms, making the transfer function an odd function of input signal voltage, i.e., *O* = −*O*. Where the signals passing through the actual device are modulated sinusoidal voltage waveforms (e.g., RF amplifier), device nonlinearities can be expressed in terms of how they affect individual sinusoidal signal components. For example, say the input voltage signal is the sine wave

and the device transfer function produces an output of the form

where *G* is the amplifier gain and *D*_{3} is cubic distortion. We may substitute the first equation into the second and, using the trigonometric identity

we obtain the device output voltage waveform as

The output waveform contains the original waveform, cos(*ωt*), plus a new harmonic term, cos(3*ωt*), the *third-order*. The coefficient of the cos(*ωt*) harmonic has two terms, one that varies linearly with *V* and one that varies with the cube of *V*. In fact, the coefficient of cos(*ωt*) has nearly the same form as the transfer function, except for the factor ¾ on the cubic term. In other words, as signal level *V* is increased, the level of the cos(*ωt*) term in the output eventually levels off, similar to how the transfer function levels off. Of course, the coefficients of the higher-order harmonics will increase (with increasing *V*) as the coefficient of the cos(*ωt*) term levels off (the power has to go somewhere).

If we now restrict our attention to that portion of the cos(*ωt*) coefficient which varies linearly with *V*, and then ask ourselves, at what input voltage level, *V*, will the coefficients of the first and third order terms have equal magnitudes (i.e., where the magnitudes intersect), we find that this happens when

which is the Third-Order Intercept Point (TOI). So, we see that the TOI input power level is simply 4/3 times the ratio of the gain and the cubic distortion term in the device transfer function. The smaller the cubic term is in relation to the gain, the more linear the device is and the higher the TOI is, which clearly makes sense. The TOI, being related to the magnitude squared of the input voltage waveform, is a power quantity, typically measured in milliwatts (mW). The TOI is always beyond operational power levels because the output power saturates before reaching this level.

The TOI is closely related to the amplifier's "1 dB compression point," which is defined as that point at which the *total* coefficient of the cos(*ωt*) term is 1 dB below the *linear portion* of that coefficient. We can relate the 1 dB compression point to the TOI as follows. Since 1 dB = 20 log_{10} 1.122, we may say, in a voltage sense, that the 1dB compression point occurs when

or

or

In a power sense (*V*2 is a power quantity), a factor of 0.10875 corresponds to −9.636 dB, so by this approximate analysis, the 1 dB compression point occurs roughly 9.6 dB below the TOI.

*Recall:* decibel figure = 10 dB × log_{10}(power ratio) = 20 dB × log_{10}(voltage ratio).

Read more about this topic: Third-order Intercept Point

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“It is not enough for *theory* to describe and analyse, it must itself be an event in the universe it describes. In order to do this *theory* must partake of and become the acceleration of this logic. It must tear itself from all referents and take pride only in the future. *Theory* must operate on time at the cost of a deliberate distortion of present reality.”

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