# A Quadrature Signals Tutorial: Complex, But Not Complicated

**Introduction**

Quadrature signals are based on the notion of complex numbers and perhaps no other topic causes more heartache for newcomers to DSP than these numbers and their strange terminology of *j operator*, *complex*, *imaginary*, *real*, and *orthogonal*. If you're a little unsure of the physical meaning of complex numbers and the j = √-1 operator, don't feel bad because you're in good company. Why even Karl Gauss, one the world's greatest mathematicians, called the j operator the "shadow of shadows". Here we'll shine some light on that shadow so you'll never have to call the Quadrature Signal Psychic Hotline for help.

Quadrature signal processing is used in many fields of science and engineering, and quadrature signals are necessary to describe the processing and implementation that takes place in modern digital communications systems. In this tutorial we'll review the fundamentals of complex numbers and get comfortable with how they're used to represent quadrature signals. Next we examine the notion of negative frequency as it relates to quadrature signal algebraic notation, and learn to speak the language of quadrature processing. In addition, we'll use three-dimensional time and frequency-domain plots to give some physical meaning to quadrature signals. This tutorial concludes with a brief look at how a quadrature signal can be generated by means of *quadrature-sampling*.

__ Why Care About Quadrature Signals?__ Quadrature signal formats, also called

*complex*signals, are used in many digital signal processing applications such as:

- digital communications systems,

- radar systems,

- time difference of arrival processing in radio direction finding schemes

- coherent pulse measurement systems,

- antenna beamforming applications,

- single sideband modulators,

- etc.

These applications fall in the general category known as *quadrature processing*, and they provide additional processing power through the coherent measurement of the phase of sinusoidal signals.

A quadrature signal is a two-dimensional signal whose value at some instant in time can be specified by a single *complex number* having two parts; what we call the *real* part and the *imaginary* part. (The words real and imaginary, although traditional, are unfortunate because of their meanings in our every day speech. Communications engineers use the terms *in-phase* and *quadrature* phase. More on that later.) Let's review the mathematical notation of these complex numbers.

**The Development and Notation of Complex Numbers**

To establish our terminology, we define a *real* number to be those numbers we use in every day life, like a voltage, a temperature on the Fahrenheit scale, or the balance of your checking account. These one-dimensional numbers can be either positive or negative as depicted in Figure 1(a). In that figure we show a one-dimensional axis and say that a single real number can be represented by a point on that axis. Out of tradition, let's call this axis, the *Real axis*.

**Figure 1.** An graphical interpretation of a real number and a complex number.

A complex number, c, is shown in Figure 1(b) where it's also represented as a point. However, complex numbers are not restricted to lie on a one-dimensional line, but can reside anywhere on a two-dimensional plane. That plane is called the complex plane (some mathematicians like to call it an Argand diagram), and it enables us to represent complex numbers having both real and imaginary parts. For example in Figure 1(b), the complex number c = 2.5 + j2 is a point lying on the complex plane on neither the real nor the imaginary axis. We locate point c by going +2.5 units along the real axis and up +2 units along the imaginary axis. Think of those real and imaginary axes exactly as you think of the East-West and North-South directions on a road map.

We'll use a geometric viewpoint to help us understand some of the arithmetic of complex numbers. Taking a look at Figure 2, we can use the trigonometry of right triangles to define several different ways of representing the complex number c.

**Figure 2** The phasor representation of complex number c = a + jb on the complex plane.

Our complex number c is represented in a number of different ways in the literature, such as:

Eqs. (3) and (4) remind us that c can also be considered the tip of a phasor on the complex plane, with magnitude M, oriented in the direction of φ radians relative to the positive real axis as shown in Figure 2. Keep in mind that c is a complex number and the variables a, b, M, and φ are all real numbers. The magnitude of c, sometimes called the modulus of c, is

[Trivia question: In what 1939 movie, considered by many to be the greatest movie ever made, did a main character attempt to quote Eq. (5)?]

OK, back to business. The phase angle φ, or argument, is the arctangent of the ratio , or

If we set Eq. (3) equal to Eq. (2), Me^{jφ} = M[cos(φ) + jsin(φ)] , we can state what's named in his honor and now called one of Euler's identities as:

The suspicious reader should now be asking, "Why is it valid to represent a complex number using that strange expression of the base of the natural logarithms, e, raised to an imaginary power?" We can validate Eq. (7) as did the world's greatest expert on infinite series, Herr Leonard Euler, by plugging jφ in for z in the series expansion definition of e^{z} in the top line of Figure 3. That substitution is shown on the second line. Next we evaluate the higher orders of j to arrive at the series in the third line in the figure. Those of you with elevated math skills like Euler (or those who check some math reference book) will recognize that the alternating terms in the third line are the series expansion definitions of the cosine and sine functions.

**Figure 3** One derivation of Euler's equation using series expansions for e^{z}, cos(φ), and sin(φ).

Figure 3 verifies Eq. (7) and our representation of a complex number using the Eq. (3) polar form: Me^{jφ}. If you substitute -jφ for z in the top line of Figure 3, you'd end up with a slightly different, and very useful, form of Euler's identity:

The polar form of Eqs. (7) and (8) benefits us because:

- It simplifies mathematical derivations and analysis,

-- turning trigonometric equations into the simple algebra of exponents,

-- math operations on complex numbers follow exactly the same rules as real numbers.

- It makes adding signals merely the addition of complex numbers (vector addition),

- It's the most concise notation,

- It's indicative of how digital communications system are implemented, and described in the literature.

We'll be using Eqs. (7) and (8) to see why and how quadrature signals are used in digital communications applications. But first, let’s take a deep breath and enter the Twilight Zone of that 'j' operator.

You've seen the definition j = √-1 before. Stated in words, we say that j represents a number when multiplied by itself results in a negative one. Well, this definition causes difficulty for the beginner because we all know that any number multiplied by itself always results in a positive number.

* Unfortunately DSP textbooks often define the symbol j and then, with justified haste, swiftly carry on with all the ways that the j operator can be used to analyze sinusoidal signals. Readers soon forget about the question: What does j = √-1 actually mean? *

Well, √-1 had been on the mathematical scene for some time, but wasn't taken seriously until it had to be used to solve cubic equations in the sixteenth century. [1], [2] Mathematicians reluctantly began to accept the abstract concept of 1, without having to visualize it, because its mathematical properties were consistent with the arithmetic of normal real numbers.

It was Euler's equating complex numbers to real sines and cosines, and Gauss' brilliant introduction of the complex plane, that finally legitimized the notion of √-1 to Europe's mathematicians in the eighteenth century. Euler, going beyond the province of real numbers, showed that complex numbers had a clean consistent relationship to the well-known real trigonometric functions of sines and cosines. As Einstein showed the equivalence of mass and energy, Euler showed the equivalence of real sines and cosines to complex numbers. Just as modern-day physicists don’t know what an electron is but they understand its properties, we’ll not worry about what 'j' is and be satisfied with understanding its behavior. For our purposes, the j operator means rotate a complex number by 90^{o} counterclockwise. (For you good folk in the UK, counterclockwise means anti-clockwise.) Let's see why.

We'll get comfortable with the complex plane representation of imaginary numbers by examining the mathematical properties of the j = √-1 operator as shown in Figure 4.

**Figure 4.** What happens to the real number 8 when you start multiplying it by j.

Multiplying any number on the real axis by j results in an imaginary product that lies on the imaginary axis. The example in Figure 4 shows that if +8 is represented by the dot lying on the positive real axis, multiplying +8 by j results in an imaginary number, +j8, whose position has been rotated 90^{o} counterclockwise (from +8) putting it on the positive imaginary axis. Similarly, multiplying +j8 by j results in another 90^{o} rotation yielding the -8 lying on the negative real axis because j^{2} = -1. Multiplying -8 by j results in a further 90^{o} rotation giving the -j8 lying on the negative imaginary axis. Whenever any number represented by a dot is multiplied by j, the result is a counterclockwise rotation of 90^{o}. (Conversely, multiplication by -j results in a clockwise rotation of -90^{o} on the complex plane.)

If we let φ = π/2 in Eq. 7, we can say that

Here's the point to remember. If you have a single complex number, represented by a point on the complex plane, multiplying that number by j or by e^{jπ/2} will result in a new complex number that's rotated 90^{o} counterclockwise (CCW) on the complex plane. Don't forget this, as it will be useful as you begin reading the literature of quadrature processing systems!

Let's pause for a moment here to catch our breath. Don't worry if the ideas of imaginary numbers and the complex plane seem a little mysterious. It's that way for everyone at first—you'll get comfortable with them the more you use them. (Remember, the j-operator puzzled Europe's heavyweight mathematicians for hundreds of years.) Granted, not only is the mathematics of complex numbers a bit strange at first, but the terminology is almost bizarre. While the term *imaginary* is an unfortunate one to use, the term *complex* is downright weird. When first encountered, the phrase complex numbers makes us think 'complicated numbers'. This is regrettable because the concept of complex numbers is not really all that complicated. Just know that the purpose of the above mathematical rigmarole was to validate Eqs. (2), (3), (7), and (8). Now, let's (finally!) talk about time-domain signals.

**Representing Real Signals Using Complex Phasors**

OK, we now turn our attention to a complex number that is a function time. Consider a number whose magnitude is one, and whose phase angle increases with time. That complex number is the e^{j2πfot} point shown in Figure 5(a). (Here the 2πf_{o} term is frequency in radians/second, and it corresponds to a frequency of fo cycles/second where fo is measured in Hertz.) As time t gets larger, the complex number's phase angle increases and our number orbits the origin of the complex plane in a CCW direction. Figure 5(a) shows the number, represented by the black dot, frozen at some arbitrary instant in time. If, say, the frequency fo = 2 Hz, then the dot would rotate around the circle two times per second. We can also think of another complex number e^{-j2πfot} (the white dot) orbiting in a clockwise direction because its phase angle gets more negative as time increases.

**Figure 5.** A snapshot, in time, of two complex numbers whose exponents change with time.

Let's now call our two e^{j2πfot} and e^{-j2πfot} complex expressions *quadrature signals*. They each have quadrature real and imaginary parts, and they are both functions of time. Those e^{j2πfot} and e^{-j2πfot} expressions are often called *complex exponentials* in the literature.

We can also think of those two quadrature signals, e^{j2πfot} and e^{-j2πfot}, as the tips of two phasors rotating in opposite directions as shown in Figure 5(b). We're going to stick with this phasor notation for now because it'll allow us to achieve our goal of representing real sinusoids in the context of the complex plane. Don't touch that dial!

To ensure that we understand the behavior of those phasors, Figure 6(a) shows the three-dimensional path of the e^{j2πfot} phasor as time passes. We've added the time axis, coming out of the page, to show the spiral path of the phasor. Figure 6(b) shows a continuous version of just the tip of the e^{j2πfot} phasor. That e^{j2πfot} complex number, or if you wish, the phasor's tip, follows a corkscrew path spiraling along, and centered about, the time axis. The real and imaginary parts of e^{j2πfot} are shown as the sine and cosine projections in Figure 6(b).

**Figure 6.** The motion of the e^{j2πfot} phasor (a), and phasor 's tip (b).

Return to Figure 5(b) and ask yourself: "Self, what's the vector sum of those two phasors as they rotate in opposite directions?" Think about this for a moment... That's right, the phasors' real parts will always add constructively, and their imaginary parts will always cancel. This means that the summation of these e^{j2πfot} and e^{-j2πfot} phasors will always be a purely real number. Implementations of modern-day digital communications systems are based on this property!

To emphasize the importance of the real sum of these two *complex sinusoids* we'll draw yet another picture. Consider the waveform in the three-dimensional Figure 7 generated by the sum of two half-magnitude complex phasors, e^{j2πfot}/2 and e^{-j2πfot}/2, rotating in opposite directions around, and moving down along, the time axis.

**Figure 7.** A cosine represented by the sum of two rotating complex phasors.

Thinking about these phasors, it's clear now why the cosine wave can be equated to the sum of two complex exponentials by

Eq. (10), a well-known and important expression, is also called one of Euler's identities. We could have derived this identity by solving Eqs. (7) and (8) for jsin(φ), equating those two expressions, and solving that final equation for cos(φ). Similarly, we could go through that same algebra exercise and show that a real sine wave is also the sum of two complex exponentials as

Look at Eqs. (10) and (11) carefully. They are the standard expressions for a cosine wave and a sine wave, using complex notation, seen throughout the literature of quadrature communications systems. To keep the reader's mind from spinning like those complex phasors, please realize that the sole purpose of Figures 5 through 7 is to validate the complex expressions of the cosine and sine wave given in Eqs. (10) and (11). Those two equations, along with Eqs. (7) and (8), are the Rosetta Stone of quadrature signal processing.

We can now easily translate, back and forth, between real sinusoids and complex exponentials. Again, we are learning how real signals, that can be transmitted down a coax cable or digitized and stored in a computer's memory, can be represented in complex number notation. Yes, the constituent parts of a complex number are each real, but we're treating those parts in a special way - we're treating them in *quadrature*.

**Representing Quadrature Signals In the Frequency Domain**

Now that we know something about the time-domain nature of quadrature signals, we're ready to look at their frequency-domain descriptions. This material is critical because we’ll add a third dimension, time, to our normal two-dimensional frequency domain plots. That way none of the phase relationships of our quadrature signals will be hidden from view. Figure 8 tells us the rules for representing complex exponentials in the frequency domain.

**Figure 8.** Interpretation of complex exponentials.

We'll represent a single complex exponential as a narrowband impulse located at the frequency specified in the exponent. In addition, we'll show the phase relationships between the spectra of those complex exponentials along the real and imaginary axes of our complex frequency domain representation. With all that said, take a look at Figure 9.

**Figure 9.** Complex frequency domain representation of a cosine wave and sine wave.

See how a real cosine wave and a real sine wave are depicted in our complex frequency domain representation on the right side of Figure 9. Those bold arrows on the right of Figure 9 are __not__ rotating phasors, but instead are frequency-domain impulse symbols indicating a single spectral line for a single complex exponential e^{j2πfot}. The directions in which the spectral impulses are pointing merely indicate the relative phases of the spectral components. The amplitude of those spectral impulses are 1/2. OK ... why are we bothering with this 3-D frequency-domain representation? Because it's the tool we'll use to understand the generation (modulation) and detection (demodulation) of quadrature signals in digital (and some analog) communications systems, and those are two of the goals of this tutorial. However, before we consider those processes let's validate this frequency-domain representation with a little example.

Figure 10 is a straightforward example of how we use the complex frequency domain. There we begin with a real sine wave, apply the j operator to it, and then add the result to a real cosine wave of the same frequency. The final result is the single complex exponential e^{j2πfot} illustrating graphically Euler's identity that we stated mathematically in Eq. (7).

**Figure 10.** Complex frequency-domain view of Euler's: e^{j2πfot} = cos(2πf_{o}t) + jsin(2πf_{o}t).

On the frequency axis, the notion of negative frequency is seen as those spectral impulses located at -2πf_{o} radians/sec on the frequency axis. This figure shows the big payoff: *When we use complex notation, generic complex exponentials like* e^{j2πft} *and* e^{-j2πft} *are the fundamental constituents of the real sinusoids* sin(2πft) or cos(2πft). That's because both sin(2πft) and cos(2πft) are made up of e^{j2πft} and e^{-j2πft} components. If you were to take the discrete Fourier transform (DFT) of discrete time-domain samples of a sin(2πf_{o}t) sine wave, a cos(2πf_{o}t) cosine wave, or a e^{j2πfot} complex sinusoid and plot the complex results, you'd obtain exactly those narrowband impulses in Figure 10.

If you understand the notation and operations in Figure 10, pat yourself on the back because you know a great deal about the nature and mathematics of quadrature signals.

**Bandpass Quadrature Signals In the Frequency Domain**

In quadrature processing, by convention, the real part of the spectrum is called the *in-phase* component and the imaginary part of the spectrum is called the *quadrature* component. The signals whose complex spectra are in Figure 11(a), (b), and (c) are real, and in the time domain they can be represented by amplitude values that have nonzero real parts and zero-valued imaginary parts. We're not forced to use complex notation to represent them in the time domain—the signals are real.

Real signals always have positive and negative frequency spectral components. For any real signal, the positive and negative frequency components of its in-phase (real) spectrum always have even symmetry around the zero-frequency point. That is, the in-phase part's positive and negative frequency components are mirror images of each other. Conversely, the positive and negative frequency components of its quadrature (imaginary) spectrum are always negatives of each other. This means that the phase angle of any given positive quadrature frequency component is the negative of the phase angle of the corresponding quadrature negative frequency component as shown by the thin solid arrows in Figure 11(a). This 'conjugate symmetry' is the invariant nature of real signals when their spectra are represented using complex notation.

**Figure 11.** Quadrature representation of signals: (a) Real sinusoid cos(2πf_{o}t + φ), (b) Real bandpass signal containing six sinusoids over bandwidth B; (c) Real bandpass signal containing an infinite number of sinusoids over bandwidth B Hz; (d) Complex bandpass signal of bandwidth B Hz.

Let's remind ourselves again, those bold arrows in Figure 11(a) and (b) are __not__ rotating phasors. They're frequency-domain impulse symbols indicating a single complex exponential e^{j2πft}. The directions in which the impulses are pointing show the relative phases of the spectral components.

There's an important principle to keep in mind before we continue. Multiplying a time signal by the complex exponential e^{j2πfot}, what we can call *quadrature mixing* (also called *complex mixing*), shifts that signal's spectrum upward in frequency by f_{o} Hz as shown in Figure 12 (a) and (b). Likewise, multiplying a time signal by e^{-j2πfot} shifts that signal's spectrum down in frequency by f_{o} Hz.

**Figure 12.** Quadrature mixing of a signal: (a) Spectrum of a complex signal x(t), (b) Spectrum of x(t)e^{j2πfot}, (c) Spectrum of x(t)e^{-j2πfot}.

**A Quadrature-Sampling Example**

We can use all that we've learned so far about quadrature signals by exploring the process of quadrature-sampling. Quadrature-sampling is the process of digitizing a continuous (analog) bandpass signal and translating its spectrum to be centered at zero Hz. Let's see how this popular process works by thinking of a continuous bandpass signal, of bandwidth B, centered about a carrier frequency of f_{c} Hz.

**Figure 13.** The 'before and after' spectra of a quadrature-sampled signal.

Our goal in quadrature-sampling is to obtain a digitized version of the analog bandpass signal, but we want that digitized signal's discrete spectrum centered about zero Hz, not f_{c} Hz. That is, we want to mix a time signal with e^{-j2πfct} to perform complex down-conversion. The frequency f_{s} is the digitizer's sampling rate in samples/second. We show replicated spectra at the bottom of Figure 13 just to remind ourselves of this effect when A/D conversion takes place.

OK, ... take a look at the following quadrature-sampling block diagram known as I/Q demodulation (or 'Weaver demodulation' for those folk with experience in communications theory) shown at the top of Figure 14. That arrangement of two sinusoidal oscillators, with their relative 90^{o} phase difference, is often called a *quadrature-oscillator*.

Those e^{j2πfct} and e^{-j2πfct} terms in that busy Figure 14 remind us that the constituent complex exponentials comprising a real cosine duplicates each part of the X_{bp}(f) spectrum to produce the X_{i}(f) spectrum. The Figure shows how we get the filtered continuous in-phase portion of our desired complex quadrature signal. By definition, those X_{i}(f) and I(f) spectra are treated as 'real only'.

**Figure 14.** Quadrature-sampling block diagram and spectra within the in-phase (upper) signal path.

Likewise, Figure 15 shows how we get the filtered continuous quadrature phase portion of our complex quadrature signal by mixing x_{bp}(t) with sin(2πf_{c}t).

**Figure 15.** Spectra within the quadrature phase (lower) signal path of the block diagram.

Here's where we're going: I(f) jQ(f) is the spectrum of a complex replica of our original bandpass signal x_{bp}(t). We show the addition of those two spectra in Figure 16.

**Figure 16.** Combining the I(f) and Q(f) spectra to obtain the desired 'I(f) jQ(f)' spectra.

This typical depiction of quadrature-sampling seems like mumbo jumbo until you look at this situation from a three-dimensional standpoint, as in Figure 17, where the j factor rotates the 'imaginary-only' Q(f) by 90^{o}, making it 'real-only'. This jQ(f) is then added to I(f).

**Figure 17.** 3-D view of combining the I(f) and Q(f) spectra to obtain the I(f) jQ(f) spectra.

The complex spectrum at the bottom Figure 18 shows what we wanted¬, a digitized version of the complex bandpass signal centered about zero Hz.

**Figure 18.** The continuous complex signal i(t) q(t) is digitized to obtain discrete i(n) jq(n).

Some advantages of this quadrature-sampling scheme are:

- Each A/D converter operates at half the sampling rate of standard real-signal sampling,

- In many hardware implementations operating at lower clock rates save power.

- For a given f_{s} sampling rate, we can capture wider-band analog signals.

- Quadrature sequences make FFT processing more efficient due to covering a wider frequency range than

when an FFT’s input is a real-valued sequence.

- Because quadrature sequences are effectively oversampled by a factor of two, signal squaring operations

are possible without the need for upsampling.

- Knowing the phase of signals enables coherent processing.

- Quadrature-sampling makes it easier to measure the instantaneous magnitude and phase of a signal during

demodulation.

Returning to the Figure 14 block diagram reminds us of an important characteristic of quadrature signals. We can send an analog quadrature signal to a remote location. To do so we use two coax cables on which the two real i(t) and q(t) signals travel. (To transmit a discrete time-domain quadrature sequence, we'd need two multi-conductor ribbon cables as indicated by Figure 19.)

**Figure 19.** Reiteration of how quadrature signals comprise two real parts.

To appreciate the physical meaning of our discussion here, let's remember that a continuous quadrature signal x_{c}(t) = i(t) + jq(t) is not just a mathematical abstraction. We can generate x_{c}(t) in our laboratory and transmit it to the lab down the hall. All we need is two sinusoidal signal generators, set to the same frequency fo. (However, somehow we have to synchronize those two hardware generators so that their relative phase shift is fixed at 90^{o}.) Next we connect coax cables to the generators' output connectors and run those two cables, labeled 'i(t)' for our cosine signal and 'q(t)' for our sine wave signal, down the hall to their destination.

Now for a two-question pop quiz. In the other lab, what would we see on the screen of an oscilloscope if the continuous i(t) and q(t) signals were connected to the horizontal and vertical input channels, respectively, of the scope? (Remembering, of course, to set the scope's Horizontal Sweep control to the 'External' position.)

**Figure 20.** Displaying a quadrature signal using an oscilloscope.

Next, what would be seen on the scope's display if the cables were mislabeled and the two signals were inadvertently swapped?

The answer to the first question is that we’d see a bright 'spot' rotating counterclockwise in a circle on the scope's display. If the cables were swapped, we'd see another circle, but this time it would be orbiting in a clockwise direction. This would be a neat little demonstration if we set the signal generators' fo frequencies to, say, 1 Hz.

This oscilloscope example helps us answer the important question, "When we work with quadrature signals, how is the j-operator implemented in hardware?” The answer is we can’t go to Radio Shack and buy a j-operator and solder it to a circuit board. The j-operator is implemented by how we treat the two signals relative to each other. We have to treat them orthogonally such that the in-phase i(t) signal represents an East-West value, and the quadrature phase q(t) signal represents an orthogonal North-South value. (By orthogonal, I mean that the North-South direction is oriented exactly 90^{o} relative to the East-West direction.) So in our oscilloscope example the j-operator is implemented merely by how the connections are made to the scope. The in-phase i(t) signal controls horizontal deflection and the quadrature phase q(t) signal controls vertical deflection. The result is a two-dimensional quadrature signal represented by the instantaneous position of the dot on the scope's display.

A person in the lab down the hall who's receiving, say, the discrete sequences i(n) and q(n) has the ability to control the orientation of the final complex spectra by adding or subtracting the jq(n) sequence as shown in Figure 21.

**Figure 21.** Using the sign of q(n) to control spectral orientation.

The top path in Figure 21 is equivalent to multiplying the original x_{bp}(t) by e^{-j2πfct}, and the bottom path is equivalent to multiplying the x_{bp}(t) by e^{j2πfct}. Therefore, had the quadrature portion of our quadrature-oscillator at the top of Figure 14 been negative, sin(2πf_{c}t), the resultant complex spectra would be flipped (about 0 Hz) from those spectra shown in Figure 21.

While we’re thinking about flipping complex spectra, let’s remind ourselves that there are two simple ways to reverse (invert) an x(n) = i(n) + jq(n) sequence’s spectral magnitude. As shown in Figure 21, we can perform conjugation to obtain an x'(n) = i(n) jq(n) with an inverted magnitude spectrum. The second method is to swap x(n)’s individual i(n) and q(n) sample values to create a new sequence y(n) = q(n) + ji(n) whose spectral magnitude is inverted from x(n)’s spectral magnitude. (Note, while x'(n)’s and y(n)’s spectral magnitudes are equal, their spectral phases are not equal.)

__Conclusions__

This ends our little quadrature signals tutorial. We learned that using the complex plane to visualize the mathematical descriptions of complex numbers enabled us to see how quadrature and real signals are related. We saw how three-dimensional frequency-domain depictions help us understand how quadrature signals are generated, translated in frequency, combined, and separated. Finally we reviewed an example of quadrature-sampling and two schemes for inverting the spectrum of a quadrature sequence.

**References**

[1] D. Struik, A Concise History of Mathematics, Dover Publications, NY, 1967.

[2] D. Bergamini, Mathematics, Life Science Library, Time Inc., New York, 1963.

[3] N. Boutin, "Complex Signals," RF Design, December 1989.

Answer to trivia question just following Eq. (5) is: The scarecrow in The Wizard of Oz.

**Have you heard this little story?**

While in Berlin, Leonhard Euler was often involved in philosophical debates, especially with Voltaire. Unfortunately, Euler's philosophical ability was limited and he often blundered to the amusement of all involved. However, when he returned to Russia, he got his revenge. Catherine the Great had invited to her court the famous French philosopher Diderot, who to the chagrin of the czarina, attempted to convert her subjects to atheism. She asked Euler to quiet him. One day in the court, the French philosopher, who had no mathematical knowledge, was informed that someone had a mathematical proof of the existence of God. He asked to hear it. Euler then stepped forward and stated: "Sir, , hence God exists; reply!" Diderot had no idea what Euler was talking about. However, he did understand the chorus of laughter that followed and soon after returned to France.

Although it's a cute story, serious math historians don't believe it. They know that Diderot did have some mathematical knowledge and they just can’t imagine Euler clowning around in that way.

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Dave Comer

You silver-tongued devil. Hope all is well with you.

[-Rick-]

If I may, I want to ask you a question about representing complex signal as real signals.

For example in QAM modulation, you have complex data, say, Z(t)=I(t)+jQ(t). To transmit this complex we modulate it and take the real component.

I.e.: we transmit the signal R(t) = Real{Z(t).e^(jft)}. Where 'f' is the carrier frequency. Then in the receiver side we mix this signal with sine and cosing, HPF it and extract I(t) and Q(t). This is fine.

Now, is there a way to do this in baseband? Can we send the baseband signal Z(t) without modulating it? That is f=0. Because when f=0, only real part of Z(t) is sent and no information about Q(t) is sent. So there is no way we can reconstruct Q(t) at receiver side.

For example in ADSL, when we perform DFT, we mirror our N complex data points and conjugate them before doing the DFT. This results in a real 2N signal, which is baseband, and can be transmitted without any carrier modulation.

But if we have complex a complex baseband signal, am I correct to think that there is no way to represent this complex signal as a real signal? Is there any way we can transmit this signal without sending I(t) and Q(t) separately in two wires as in your example?

Thank you very much for great contributions.

Thanks

Thanks

The top of Figure 15 is the spectrum of the input analog bandpass signal. Negative-freq spectral energy is shown by a dashed curve.

The center of Figure 15 is the spectrum of the output of the bottom mixer in our Figure 14 block diagram. Notice at the bottom right of Figure 9 that a real-valued sine wave is equivalent to a positive-freq exponential and a negative-freq exponential. BUT, notice that the positive-freq exponential part of a real sine wave is 180 degrees out of phase relative to the negative-freq exponential part.

So when you multiply a real-valued bandpass signal by a sine wave, half the bandpass signal's spectral energy is translated up in frequency and half the bandpass signal's spectral energy is translated down in frequency.

To quote Ardeth Bay in the 1999 movie The Mummy, "Know this!" The up-translated spectral energy is 180 degrees out of phase relative to the down-translated spectral energy. That super-important characteristic is shown in the center of Figure 15 where spectral energy below the horizontal axis is 180 degrees out of phase with spectral energy above the horizontal axis.

I presume you understand the bottom part of Figure 15. I hope what I've written makes sense. If not, let me know, OK?

Dear Mr. Lyons, this is a very good article. I have learned a lot from it, and it wasn't that much difficult.

However, it seems to me that your Figure 6 is not correct: comparing with the symbols shown in the previous figure (Figure 5), it should be a positive frequency, thus it should be a counter-clockwise spinning helix (or corkscrew), but it is a clockwise helix. It doesn't matter if we go along the increasing or decreasing direction of the time axis, because the helix would be the same, anyway, but the projection (the circle in perspective) at the bottom plane looks inverted when we look at it from the wrong side.

Well, I hope you can find some use for this comment. I sincerely enjoyed very much reading your fine article.

Mauricio

Retired professor of Chemistry

Hello mgconsta. Thank you for your kind words.

The spiral in my Figure 6(b) is rotating in the counter-clockwise direction. Notice that the spiral is coming up out of the page as time passes. That is, the positive-time axis is pointing upward at the reader.

Richard,

Excellent article. I'm confused about one thing. The bottom plot of figure 17 shows the entire spectra drawn on the real axis and nothing in the imaginary axis, however, the spectra is clearly complex. Does this mean that the complex spectra cannot be represented by a spectral decomposition of real and imaginary axes?

Thanks,

Frank

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