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Introduction to the Impedance and Impedance Curve of Headphones

Sha1rholder

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Understanding this article requires basic knowledge of complex numbers and high-school-level electricity knowledge.
Special thanks to Engineer Mr. Xu from XK-Audio for his patient guidance; and to amirm, the moderator of AudioScienceReview Forum, for authorizing the usage of his measurements, which made this article possible.

Essentially, headphone drivers are just electric components, and headphone systems are just complex circuits. To analyze the electroacoustic performance of headphone drivers, we can consider all the components from the last stage of amplifier to the headphone driver as an active local circuit. This article will unveil one of the most important parameters of headphones — the impedance.

BTW, here's non-profit advertisement. Have a glance at my GitHub repository Sha1rholder/Sound-Library: Your Acoustics Knowledge Base (github.com) which dedicates to helping audiophiles and those interested in high-quality audio learn the knowledge of sound : )

Impedance and Impedance Curve​

Impedance describes the opposition that an electronic component presents to the flow of current. It consists of resistance and reactance, where reactance is further divided into inductive reactance and capacitive reactance. Impedance can be described mathematically as follows:
1722020316621.png

1722020326762.png
Where Z is impedance, R is linear resistance, X is reactance, XL is inductive reactance, XC is capacitive reactance, and j is the imaginary unit −1. All these quantities are measured in ohms (Ω). Impedance is a complex number, with its real part being resistance and its imaginary part being reactance. The magnitude of impedance reflects the extent to which a component opposes the flow of current.

For dynamic and planar magnetic headphone drivers, the capacitive reactance is usually much smaller than the linear resistance and inductive reactance, i.e., X≈XL. Therefore, the impedance of headphones can be approximated as being composed only of resistance and inductive reactance, i.e.,
1722020385418.png
Inductive reactance is the opposition to current flow caused by inductance and is positively correlated with the rate of change of current. Therefore, the frequency of electric signal affects the inductive reactance, which in turn affects the impedance. The relationship between signal frequency and impedance is known as the impedance curve.
1722020404273.png
Guess which headphone's impedance curve it is! The answer will be revealed at the end of the article.

Impedance of Planar Magnetic Headphones​

Planar magnetic headphones use conductive traces printed on a diaphragm and drive the diaphragm using electromagnetic induction. A planar magnetic headphone driver consists of magnets and a diaphragm with conductive traces. The magnets produce a magnetic field, and the conductive traces carry the signal current, which creates a force that drives the diaphragm, causing it to vibrate and produce sound. The following images show two typical planar magnetic driver structures.
1722020439840.png

1722020446791.png
In the second image, the conductive traces and magnetic field lines are perpendicular to each other, and the current flowing in the direction shown generates a downward force. Because the vibrating part of planar magnetic headphones is very light, the conversion of electric energy to mechanical energy is minimal, resulting in very low inductive reactance. Therefore, the impedance of most planar magnetic headphones is almost equal to their linear resistance. Since linear resistance is not affected by the signal current frequency (as it's called "linear"), the impedance curves of most planar magnetic headphones are flat.
1722020459774.png

1722020468021.png
The impedance curve of HIFIMAN Susvara is flat.
1722020480249.png

1722020486436.png
However, not all planar have perfectly flat impedance curves, as seen with the DCA Expanse.

Impedance of Dynamic Headphones​

Dynamic headphones bind a voice coil to a diaphragm and use electromagnetic induction to drive the voice coil, which in turn drives the diaphragm. A dynamic driver consists of a magnet, a voice coil, and a diaphragm. The magnet produces a magnetic field, and the voice coil carries the signal current, generating a force that drives the diaphragm, causing it to vibrate and produce sound. The following images show a typical structure of dynamic driver.
1722020500946.png

1722020515002.png
As shown in the images, the voice coil acts the same like all coils which exhibit self-inductance. Additionally, the vibration of dynamic drivers cuts through the magnetic induction line more than planars, resulting in significant inductive reactance. Since inductive reactance is affected by signal frequency, the impedance curves of dynamic headphones are not flat.
1722020530685.png
As shown, the impedance of the Beyerdynamic dt880 (600 Ω) fluctuates significantly with frequency.
1722020541899.png
You may notice that early premium dynamic headphones generally had higher impedance, such as the hd600 and dt880. This is because early headphone amplifiers had high output impedance, making it quite inefficient to drive low-impedance headphones due to the voltage division principle of series circuits. Therefore, some headphones increased their resistance by reducing the wire diameter, to subsequently increase impedance. Additionally, the materials and craftsmanship of early dynamic diaphragms, voice coils, and magnets were not as advanced as today, so increasing the number of voice coil results in the enhancement of the response to magnetic, and significantly increased resistance and self-induction effects.

Resonance and Self-Induction in Dynamic Headphones​

You may have noticed a great peak in dt880's impedance curve at low frequencies. This is because dynamic drivers tend to resonate near certain frequencies, causing a large amount of electromagnetic and mechanical energy to convert back and forth. This phenomenon is known as resonance, and the frequency at which it occurs is the resonant frequency, aka f0, which is of great interest to audiophiles and acoustic engineers.
1722020559149.png
Severe resonance can cause both frequency response defects and nonlinear distortion. Therefore, in headphone design, resonance is often suppressed by increasing damping, enhancing diaphragm stiffness, and enlarging the diaphragm area. Increasing resistance can also "dilute" the effect of resonant inductive reactance.

According to Engineer Mr. Xu from XK-Audio, the first generation of Avalon headphones, similar to the dt880, experienced a significant increase in impedance at certain low frequencies due to resonance, negatively affecting sound quality. The second generation of Avalon learned from the first generation's experience, increased resistance, and used an ultra-large diaphragm (d = 70 mm) to make the impedance curve flatter, resulting in a high-impedance dynamic headphone.
1722020572100.png
Returning to the impedance curve of dt880, you may also notice an upward trend in impedance at high frequencies. This is because (higher frequency + more turns in the voice coil) -> (more pronounced the self-induction effect of the voice coil) -> (greater inductive reactance) -> (more pronounced high-frequency rise in the impedance curve).

dt880 Impedance Treble Peak

These two effects will also cause the voltage sensitivity calculated from impedance and power sensitivity to be lower than the actual situation. Therefore, when evaluating the "difficulty" of driving dynamic headphones, voltage sensitivity is more meaningful than power sensitivity. The calculation method and derivation process can be found in ths article The Algebraic Relationship Between Sensitivity and Impedance

AR5000 Impedance

The impedance curves of some modern dynamic headphones can be flatter, such as the Aune AR5000.

AR5000

Does Output Impedance Affect Frequency Response Curves?​

In most cases, no. The frequency response distortion caused by the high output impedance of tube amplifiers is negligible!
The following section can be skipped by general readers. There is an old Chinese saying: "To know what is so, and to know why it is so." This section is for true audiophiles.
Here comes math

Algebraic Relationship​

The output section of an amplifier and the headphone driver form a series circuit, causing the voltage distribution across the headphone unit to vary at different frequencies. If the impedance curve, linear resistance, and frequency response curve of the headphone and the tube amp are known, we can accurately calculate the frequency response of the headphone on this tube amp.

If at a certain frequency, the linear resistance of the headphone is R, the reactance is X; the linear resistance part of output impedance the tube amp is r, and the reactance is x, then while under the same total equivalent voltage, the decibel sound pressure level, aka dBSPL, driven by the tube amp will be:

1722020640952.png
If the linear resistance of a certain headphone is R, and the linear resistance part of the output impedance of a certain tube amp is r; at 1 kHz, the reactance of the headphone is X1, and the reactance part of the output impedance of the tube amp is x1; at frequency f, the reactance of the headphone is X2, and the reactance part of the output impedance of the tube amp is x2. Then, when the tube amp and a regular low-output-impedance headphone amp drive the same headphone to same dBSPL at 1 kHz, the dBSPL driven by the tube amp at frequency f will be:
1722020654958.png

1722020909203.png

Frequency Response Simulation​

Based on the above principles, we can use code to simulate the effect of output impedance of tube amps on headphone frequency response.

In this program, I used the frequency response and impedance curve of the Beyerdynamic dt1990 measured by amirm from ASR Forum and reduced the overall linear resistance by 230 Ω to create a hypothetical "low-impedance dt1990" to amplify the effect of output impedance on headphone frequency response. I also assumed a tube amp with an output impedance of Z=300+0.01∗frequency+100/frequency (very few tube amps have such high output impedance nowadays).

We then get the following output, where the blue line is the original frequency response of our hypothetical "low-impedance dt1990", and the red line is the frequency response of the "low-impedance dt1990" driven by a high-output-impedance tube amp.

Extreme Tube Amp FR


What? You mean, where's the red line?

Partially Enlarged Frequency Response

There's Poison in the Food

Answer Revealed​

Thanks for reading this far, you are true audiophiles! Let's reveal the answer to the question at the beginning:

masked impedance
Guess which headphone's impedance curve this is!
r70x ASR

It's ATH-R70x with super cool super high super varied impedance curve!
 
A lot of integrated amps incl AVR with headphone output sockets can have output resistances up to 400 ohm and there are quite a few headphones around that can have a substantially changed frequency response.

Below the measured frequency response of the DT1990 driven from 0.2, 10, 32 and 120 ohm output R.

1722023093022.png
 
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I can hear difference with HD 560S when using low output impedance Topping amplifier and higher output impedance iD4 interface. Since I liked iD4 tonality better, I used EQ to make it similar on Topping.

 
A lot of integrated amps incl AVR with headphone output sockets can have output resistances up to 400 ohm and there are quite a few headphones around that can have a substantially changed frequency response.

Below the measured frequency response of the DT1990 driven from 0.2, 10, 32 and 120 ohm output R.

View attachment 383194
that was really beyond my knowledge. Thanks for letting me know.

Most tube amps beloved by Chinese audiophiles has relatively lower output impedance. I guess that's what made me think it is so.
 
I can hear difference with HD 560S when using low output impedance Topping amplifier and higher output impedance iD4 interface. Since I liked iD4 tonality better, I used EQ to make it similar on Topping.
HD560S on 0.2, 10, 32 and 120 ohm
1722055449342.png
 
that was really beyond my knowledge. Thanks for letting me know.

Most tube amps beloved by Chinese audiophiles has relatively lower output impedance. I guess that's what made me think it is so.
The drawings of both the dynamic drivers and planar ones are technically incorrect b.t.w.
 
The drawings of both the dynamic drivers and planar ones are technically incorrect b.t.w.
Can you point out where these diagrams are incorrect? Additionally, the diagram of the planar magnetic driver was manually drawn by me based on the simulation of the planar magnetic driver from XK-Audio, so I think there shouldn't be errors.
 
the planar has the windings between the magnets just like the upper part shows, also note the magnet direction which depends on the current direction.
1722076668742.jpeg

Your drawing combined both methods so either draw the upper or the bottom one. Also there is a round planar driver.

The airgap for the dynamic driver is on the right side and the middle of the inductor should be in the airgap. (below picture is drawn by me)
dynamic-driver.png
1722076920241.png
 
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j is the imaginary unit −1

j is the square root of -1

It's more relevant in this context to think of it as a vector of magnitude 1 with phase +90 degrees.

Therefore, some headphones increased their resistance by reducing the wire diameter, to subsequently increase impedance.

Reduce wire diameter in order to coil it more times (or to reduce the distance between the wire and the magnet but honestly it's mostly coiling it more times)

The resistance part of speaker drivers do not contribute to magnetics, consequently increasing resistance without increasing the magnetic effects (i.e. making the magnetics unchanged) only reduces efficiency. The sane amount of current will be needed for same output, but more voltage will be needed.
 
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the planar has the windings between the magnets just like the upper part shows, also note the magnet direction which depends on the current direction.View attachment 383271
Your drawing combined both methods so either draw the upper or the bottom one. Also there is a round planar driver.

The airgap for the dynamic driver is on the right side and the middle of the inductor should be in the airgap. (below picture is drawn by me)
dynamic-driver.png
View attachment 383272
Actually there are many choices for the arrangement of magnets, the placement of magnetic poles, and the shape of magnets in planar magnetic headphones. What I have drawn is just one of the options and not the type of magnets used by Audeze.
 
Actually there are many choices for the arrangement of magnets, the placement of magnetic poles, and the shape of magnets in planar magnetic headphones. What I have drawn is just one of the options and not the type of magnets used by Audeze.
Do with the info what you want.
 
Actually there are many choices for the arrangement of magnets, the placement of magnetic poles, and the shape of magnets in planar magnetic headphones. What I have drawn is just one of the options and not the type of magnets used by Audeze.

Allow me to draw your attention to your 2nd graphic since possibly you're looking at magnets and overlooking a detail. That rendering inaccurately dis-placed the conductive traces off center of the opposing magnets when the conductive traces are functionally located by having an interface with the magnets. (I don't think your 1st planar drawing reveals anything precise about conductive traces.) Below is your blue and red 2nd schematic placement of conductive traces followed by a rendering (similar to solderdude's) for planar headphone magnets with their placement of conductive traces (represented by a blue dash).
IMG_0749.jpeg

IMG_3392.jpeg
 
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Allow me to draw your attention to your 2nd graphic since possibly you're looking at magnets and overlooking a detail. That rendering inaccurately dis-placed the conductive traces off center of the opposing magnets when the conductive traces are functionally located by having an interface with the magnets. (I don't think your 1st planar drawing reveals anything precise about conductive traces.) Below is your blue and red 2nd schematic placement of conductive traces followed by a rendering (similar to solderdude's) for planar headphone magnets with their placement of conductive traces (represented by a blue dash).
View attachment 383373
View attachment 383372
Actually, in the drawing I made, the wire should not be placed directly below the magnet but rather between the two magnets. You can try drawing the magnetic field lines or conducting a finite element simulation, and you will find that the position of the wire is arranged in the location where the magnetic field is strongest.
 
Do with the info what you want.
Consider what the "S" in ASR stands for. If you lack respect for facts and blindly trust your own experience, you won't be able to learn anything.
 
Actually, in the drawing I made, the wire should not be placed directly below the magnet but rather between the two magnets. You can try drawing the magnetic field lines or conducting a finite element simulation, and you will find that the position of the wire is arranged in the location where the magnetic field is strongest.
It is not just the strength of the magnetic field, but also the directions of the magnetic flux lines. The Lorentz force (or Biot–Savart law) is the cross product of the current vector and magnetic field vector. Therefore, for the magnetic force on the diaphragm to act straightly in the up and down direction, the magnetic flux lines need to be horizontal at the wires as shown in the picture (since current flows in the direction into and out of the picture). It is not clear if the arrangement of magnets you showed will do that. Better to display the flux lines as @solderdude did in his post.
 
Actually, in the drawing I made, the wire should not be placed directly below the magnet but rather between the two magnets. You can try drawing the magnetic field lines or conducting a finite element simulation, and you will find that the position of the wire is arranged in the location where the magnetic field is strongest.
Thanks for the correct orientation like shown below.
IMG_0760.jpeg
 
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It is not just the strength of the magnetic field, but also the directions of the magnetic flux lines. The Lorentz force (or Biot–Savart law) is the cross product of the current vector and magnetic field vector. Therefore, for the magnetic force on the diaphragm to act straightly in the up and down direction, the magnetic flux lines need to be horizontal at the wires as shown in the picture (since current flows in the direction into and out of the picture). It is not clear if the arrangement of magnets you showed will do that. Better to display the flux lines as @solderdude did in his post.

Thank you for your suggestion. I will draw the magnetic field lines to improve this diagram. In China, drawing magnetic field lines based on magnets is a mandatory part of the junior high school curriculum, so I mistakenly assumed that everyone would be able to understand it.
 
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