Why the last 5mm before an ESD protection diode defeats it

The clamping voltage in a TVS datasheet is measured at the TVS's own terminals. If the voltage reaching the IC pin is higher, the cause is not the trace from the connector to the TVS but the inductance of the stub branching off the signal line to the TVS and of the TVS's ground via, the last few mm before the current reaches ground.

Last updated: 2026-10-09 ESDTVSIEC 61000-4-2PCB layoutProtection circuit

IEC 61000-4-2 8kV contact discharge: the standard fixes only the first ns

IEC 61000-4-2 has contact discharge, where an ESD gun discharges directly onto a metal part, and air discharge through the air. Contact discharge is what mostly matters for board design, and the standard defines its current waveform by the initial peak current and the rise time.

An 8kV contact discharge (level 4) has an initial peak current Ip ≈ 30A and a rise time tr = 0.7 to 1ns. The current then continues for tens of ns, but what decides whether the TVS clamping voltage is exceeded and how much the path inductance to ground raises the voltage is the first 1ns or less. What matters is not distance on the board but the speed of this current.

di/dt is Ip ÷ tr = 30A ÷ (0.7 to 1ns) ≈ 30 to 43A/ns, the number the next section multiplies by inductance. It is orders of magnitude faster than an 8/20µs surge (IEC 61000-4-5), and 1mm of inductance can no longer be ignored.

IEC 61000-4-2 8kV contact discharge current, with the voltage at the TVS terminal and the IC pinTop right: the current from the ESD gun (schematic, Ip ≈ 30A, tr = 0.7 to 1ns). Bottom left: the TVS terminal voltage, a stepped waveform at about 20V clamp. Bottom right: the IC pin voltage past the stub and ground via, with a sharp L·di/dt spike on the same step reaching nearly 200V briefly. The IC's absolute maximum (about 4V) is the horizontal dashed line. IEC 61000-4-2 8kV contact discharge current, with the voltage at the TVS terminal and the IC pin Rise tr = 0.7 to 1ns, di/dt ≈ 30 to 43A/ns Current waveform (schematic) 30A Ip ≈ 30A tr = 0.7 to 1ns Time (ns, scale approximate) TVS terminal voltage 0V 20V 100V 200V Time (ns, scale approximate) 0 IC absolute max ≈ 4V Clamp only; settles to a step IC pin (past stub + ground path) 0V 20V 100V 200V Time (ns, scale approximate) 0 IC absolute max ≈ 4V Stub and ground path L·di/dt adds, briefly near 200V With the same clamp, a stub and ground path change the IC voltage by an order of magnitude or more.
Figure 1: top right, the 8kV contact discharge current (schematic). Bottom, the voltage at the TVS terminal (clamp only) and at the IC pin past the stub and ground via. The latter has an L·di/dt spike on top of the clamp.

The branch stub and ground via add to the clamping voltage

The datasheet clamping voltage VC is measured across the TVS itself and does not necessarily reach the IC pin as is. The inductance of the trace from the connector to the TVS does not raise the IC voltage. To the ESD current it is a series impedance on the source side, and it even slows the current's rise before it reaches the IC. How long that section is should be set by signal matching.

What raises the IC pin voltage is the inductance of the path where the current falls to ground. That means (a) the stub branching from the signal line to the TVS, plus the TVS's own ground side (pad, via, plane), and (b) with the IC between the connector and the TVS, the trace from the IC's branch point to the TVS. Most of the ESD current (30A class) takes this path, so the inductance L develops V = L × di/dt, which adds to the TVS terminal voltage and becomes the IC pin voltage. A guide is about 1nH/mm, and one via falls in this range. Check a via's value with the via inductance calculator.

Voltage added by the stub and ground path (L ≈ 1nH/mm, Ip = 30A, tr = 0.7 to 1ns, V = L × Ip/tr)
Stub + ground path lengthInductance guideAdded voltage (tr = 1ns)Added voltage (tr = 0.7ns)
One ground via tight to the pad (about 0.5nH)0.5nH15V21V
Stub + via, 2mm equivalent2nH60V86V
Stub + via, 5mm equivalent5nH150V214V
Stub + via, 10mm equivalent10nH300V429V

Just 5mm of equivalent inductance in the stub and ground path pushes a fast unit (0.7ns) above 200V. Even with a clamping voltage near 20V, what reaches the IC pin is clamping voltage plus added voltage: 170 to 230V at 5mm equivalent and 320 to 450V at 10mm. Even with the TVS working, this greatly exceeds the IC's absolute maximum rating (usually a few V). The "5mm" in the title is this path just before the current reaches ground.

This is an idealized estimate, and the numbers shift with current distribution and how the IC's ground is taken, but it does show that "a low clamping voltage makes stub and ground path length irrelevant" does not hold.

Where ESD current falls to ground (stub + ground via), the IC pin voltage jumpsESD current from the connector heads to the TVS at the branch point and falls through the stub and ground via to the plane. The trace from connector to branch does not raise the IC voltage. Stub and via inductance put the IC pin (branch point) above the TVS terminal. An animation of two states in turn. 1. Normal: no pulseTVS is reverse-biased; no current flows 2. ESD pulse passing: the stub and ground via spike the IC pinThe connector-side trace has no effect. The rise is where current falls to ground Connector Trace (source side) Hardly raises the IC voltage IC To IC Branch point (= IC pin) Branch stub TVS Ground via Ground plane This matters: stub + ground via (L ≈ 1nH/mm) TVS terminal voltage IC pin (branch) voltage This is L·di/dtHigher by the stub + ground via
Figure 2: the ESD pulse enters at the connector and heads for the TVS at the branch point. The trace from connector to branch (faint section) does not raise the IC voltage. The voltage jumps in the branch stub and ground via, so the IC pin is this much above the TVS terminal.

Correct placement: the signal passes through the TVS pad

  • Place connector, then TVS, then the protected part. With the TVS nearer than the IC, the ESD current falls to ground before it reaches the IC's branch point. In the reverse order (connector, IC, TVS), a large current flows in the trace from the IC's branch point to the TVS, and its inductance raises the IC voltage.
  • Route the signal through the pad instead of using a branch stub. A T-shaped stub makes the whole stub length the inductance in the table. If the signal passes between the two pads, the stub disappears and only the ground-side path remains.
  • Take the TVS ground to the plane by the shortest path. This is the top priority. Almost all the ESD current takes the path from the anode (ground side) to the plane. Put the ground via tight to the pad, and if possible directly under it (via in pad). If the ground side is long, shortening the signal-side stub does not reduce the added voltage.
Bad layout (stub, far ground via) and good layout (signal through the TVS pad)Board plan views. Left: the TVS sits on a stub off the signal path with its ground via away from the pad, and the signal runs from connector to IC past it. Right: the signal enters the TVS pad first, then goes to the IC by a short trace, with the ground via tight to the pad. Bad layout (stub, far ground via) and good layout (signal through the TVS pad) Bad: TVS on a stub Connector IC Stub TVS Ground via also far Ground plane Signal passes straight from connector to IC Stub and ground via both far: large total inductance Good: signal through the TVS pad Connector TVS IC Ground via Ground plane Routed connector, TVS, IC Ground via tight to the pad, shortest to the plane
Figure 3: in the bad layout (left) the TVS hangs off a stub and the ground via is away from the pad. In the good layout (right) the signal passes through the TVS pad and the ground via is tight to it.

Clamping voltage versus the IC's absolute maximum and its built-in ESD structure

The absolute maximum rating of most ICs is VDD ± 0.3 to 0.5V or a few V. The added voltage of 150 to 214V at 5mm equivalent is tens of times that or more. Many cases of an IC failing even though the TVS clamps, or becoming unstable later, are caused by this added voltage exceeding the rating.

The IC's built-in protection diodes are not designed to take system-level ESD alone. IC ESD robustness is based on component-level tests such as HBM and CDM, whose test currents are much smaller. The HBM (ANSI/ESDA/JEDEC JS-001) equivalent circuit discharges 100pF through 1.5kΩ, and even at 2kV the peak current is 2000V ÷ 1500Ω ≈ 1.33A with a 2 to 10ns rise. An 8kV contact discharge has a 30A peak and a rise under 1ns: more than 20 times the peak current and several times faster. The TVS's job comes before lowering the clamping voltage: it is to shunt the large current to ground outside the IC.

TVS dynamic resistance and reading TLP data

A TVS clamping voltage is not constant with current. In the I-V characteristic from a TLP (Transmission Line Pulse) test, voltage rises in proportion to current once the breakdown voltage VBR is exceeded. The slope is the dynamic resistance Rdyn, and the clamping voltage is VC = VBR + Rdyn × I.

A TLP test (ANSI/ESDA STM5.5.1) sends short ns-scale pulses of increasing size and records voltage and current. At a speed close to ESD, it shows the true clamping voltage and dynamic resistance that 8/20µs surge tests and DC characteristics do not. If the datasheet gives "clamping voltage at IPP" for several currents, you can back out Rdyn from the slope.

Even a TVS with a dynamic resistance of 0.3 to 1Ω adds Rdyn × I = 9 to 30V at 30A, which adds to the stub and ground path voltage in the table before it reaches the IC pin. Choose a TVS by its clamping voltage at high current (a small Rdyn) as well as a low VBR.

TVS I-V characteristic and dynamic resistance measured by TLPCurrent-voltage graph from TLP testing. Past the breakdown voltage VBR, voltage rises in proportion to current along the dynamic-resistance slope. The smaller the dynamic resistance, the lower the clamping voltage at high current. TVS I-V characteristic and dynamic resistance measured by TLP VC = VBR + Rdyn × I 0A 10A 20A 30A 40A 0V 10V 20V 30V 40V Low Rdyn (0.3Ω) High Rdyn (1.0Ω) I = 30A (IEC 8kV) 15V 36V VBR (breakdown) Slope = dynamic resistance Rdyn At the same VBR, a smaller Rdyn clamps lower at high current.
Figure 4: I-V characteristic measured by TLP. Past breakdown, voltage rises along the dynamic-resistance slope, so a TVS with lower dynamic resistance clamps lower at high current even at the same breakdown voltage.

A series resistor on the IC side shares the current

Even the shortest TVS placement does not bring the added voltage to zero. So a series resistor Rs (10 to 33Ω as a guide) is often placed between the TVS and the IC pin to limit the residual current flowing into the IC.

With the TVS-terminal node voltage Vnode (clamping voltage plus the stub and ground path addition) and the IC's built-in protection diode forward voltage Vf ≈ 0.8V, the current into the IC is about IIC = (Vnode − Vf) ÷ Rs. For Vnode = 20V, it falls to 1.9A with Rs = 10Ω, 0.9A with 22Ω, 0.6A with 33Ω and 0.2A with 100Ω. A larger Rs degrades the signal more (slower edges), so set it within what the signal allows.

This resistor does not replace the TVS: it limits what the TVS could not take to a current the IC's built-in structure survives. On a high-speed signal, Rs disturbs the line impedance, so confirm its value and position by measurement or similar.

TVS and series resistor Rs share the current reaching the ICCircuit where the TVS shunts most of the current to ground and the rest is limited by series resistor Rs on its way to the IC's built-in protection diode. An animation of two states in turn. 1. Normal: no ESD pulseTVS and the IC's built-in diode are both reverse-biased 2. ESD pulse passing: the TVS takes most, Rs limits the restI_IC = (Vnode − Vf) ÷ Rs Connector TVS Rs (10 to 33Ω guide) IC Built-in protection diode Most current goes to ground here Rest limited by Rs I_IC ≈ (Vnode − Vf) ÷ RsVnode = 20V, Rs = 33Ω → I_IC ≈ 0.6A
Figure 5: the TVS shunts most of the current to ground, and the rest is limited by series resistor Rs on its way to the IC's built-in protection diode.

Capacitance and signal speed: what TVS capacitance USB and HDMI allow

Seen from the signal line, a TVS is also a shunt capacitance to ground, which cuts bandwidth, worsens return loss and closes the eye. General guides are 1pF or less for USB 2.0 HS (480Mbps) and 0.3pF or less for the high-speed lanes of USB 3.x and HDMI. For low-speed signals such as UART, I2C and power lines, tens to hundreds of pF is no problem.

When a shunt capacitance C sits in the middle of a line terminated by 50Ω at both ends, the capacitor sees the two 50Ω in parallel, 25Ω. The −3dB corner is f = 1 ÷ (2π × 25Ω × C): about 6.4GHz for C = 1pF and about 21GHz for 0.3pF. A USB 2.0 HS edge is around 500ps (bandwidth 0.35 ÷ 500ps ≈ 700MHz), so even 1pF is not likely to cut the bandwidth.

High-speed lanes are still strict about capacitance because return-loss limits are set from frequencies far below the −3dB corner, the parasitic capacitance of the TVS package, pad and via adds on, and the eye margin at several Gbps is only tens of mV and a few ps.

For a high-speed lane TVS, in addition to clamping voltage and surge current, check the datasheet capacitance against the signal speed.

What catches people on real boards

A board that reboots when hit with an ESD gun, or does not change after adding a TVS, is common in designs where someone looked only at the clamping voltage and judged "within spec, so fine." Measure the branch stub length and ground via position, estimate the added voltage from the table, and if it is 5mm equivalent or more, suspect the layout. The typical case is a TVS hanging off a stub while the signal runs past the stub's root. If robustness suddenly drops in a new revision, check the Gerbers for changes such as a ground via moving away or a longer stub.

Protection that is weak only on a high-speed port comes from putting a general-purpose TVS of a few pF to a dozen pF on a USB 3.x or HDMI lane and closing the eye; switch to a low-capacitance part. Without a TLP system, measure the real length of branch point, TVS pad, ground via and plane in the Gerbers, estimate with the table, and if the margin is thin, revisit the layout before the part.

Frequently asked questions

If I use a TVS with a lower clamping voltage, are a longer stub and ground path acceptable?
The added voltage is set by the stub and ground path inductance and di/dt, and adds regardless of the TVS clamping voltage. Even with a 10V clamping TVS, a 5mm-equivalent stub and ground path delivers 160 to 220V to the IC. Improving the TVS and improving placement (especially the ground side) are separate axes, so you need both.
Is it safe to put the TVS as close to the connector as possible?
What raises the IC voltage is not the trace from the connector to the TVS but the TVS's own ground path and the branch stub from the signal line. Even right at the connector, a distant ground via or long stub limits the benefit. Keep the ground side shortest, route the signal through the TVS pad, and keep the order connector, TVS, IC.
On a 4-layer board I can only place one via from the TVS ground to the plane. Is that a problem?
One via (about 0.5nH) equals 0.5mm of trace and is not a big problem alone. The problem is a long path from the via to the solid ground (a distant inner-layer plane, or a detour around other traces). Check the effective distance to the plane rather than the number of vias.
Should I avoid a TVS with no TLP data?
If the datasheet gives clamping voltages at several currents (for example VC at IPP = 1A and 8A), you can estimate the dynamic resistance from the slope. With only one point, use TLP data from a similar product or ask the manufacturer.
How does a series resistor affect signal quality?
Matched to the transmission line's characteristic impedance, it can also act as source termination. If it is too large, its RC with the trace and driver output capacitance slows the edges. On high-speed lanes, see whether it can double as the ESD resistor within the damping-resistor design (see At what length does a trace become a transmission line?).

Standards and references

  • IEC 61000-4-2, Electromagnetic compatibility (EMC) – Part 4-2: Testing and measurement techniques – Electrostatic discharge immunity test — Test levels and current waveform (peak current, rise time) for contact and air discharge
  • ANSI/ESDA/JEDEC JS-001, Human Body Model (HBM) – Component Level — Equivalent circuit (100pF, 1.5kΩ) and test current of the component-level ESD test
  • ANSI/ESDA STM5.5.1, Transmission Line Pulse (TLP) – Electrostatic Discharge Sensitivity Testing — How to measure I-V characteristics and dynamic resistance by TLP
  • Manufacturers' TVS and ESD protection diode datasheets and application notes — Clamping voltage, dynamic resistance, capacitance, and recommended PCB placement

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