# The importance of Electrostatic Discharge Rates

The control of electrostatic discharge is an important aspect when manufacturing, assembling and repairing devices that employ electronics. Electrostatic discharges can damage an electronic component at any stage of its production or application if not controlled. The primary method of control is to ground (or bring to the same potential) all conductors that come in contact or near proximity to the electronic device(s). These conductors include humans, tools, ESD mats, other electronic devices, boards, connectors, packaging, etc.

There are other components to a good ESD Control programme including removal of unnecessary insulators, shielding, ionisation, environmental controls, training, education and top-down compliance. This post will talk about controlling discharges to a grounded ESD mat on a workstation. Watch out: it’s about to get technical!

**Introduction**

Of specific interest in controlling an electrostatic discharge is the time rate of the discharge. A discharge will occur much quicker in/on a conductor with a surface resistance of 10^{2} ohms than in a conductor with a surface resistance of 10^{9} ohms. How fast or slow should the controlled discharge be? Understanding the importance of discharge times will help you choose the right ESD control materials in building, maintaining or auditing your own ESD Safe workbench(es).

The upper and lower boundaries of an ESD safe discharge rate are determined by the application and materials used. To limit the discussion, the potential energy sourced from the Human Body Model (HBM), [refer to EN 61340-5-1], is applied to an ESD sensitive work area or ESD mat.

**Body and Movement**

You should be familiar with the timing of the human body’s movements relative to handling or working near ESD sensitive devices to have a handle on the upper limit of the controlled discharge. To reduce the likelihood of an operator discharging onto an ESD sensitive device, they should drain any charges before bringing an ESD sensitive device in contact with themselves or another conductor, whether floating or grounded.

Table 1 – Movement times (averaged) from typical operations:

Table 1 shows averaged times (in milliseconds) for the handling of tools or devices at a work bench with a corresponding standard deviation in milliseconds. The shortest time of 153ms, or worst case, is the time that we will design our ESD sensitive workbench tabletop with. You want to be sure that your device is fully discharged well before the 153ms landing time. A good rule of thumb would be to engineer a x2 safety factor. Therefore, your device should be fully discharged before reaching 76.5ms (76.5ms x 2 = 153ms). The time constraint of 76.5ms for body movement defines the upper boundary of the controlled discharge rate (not including the standard deviation of 11ms).

**Energy Considerations**

Table 2 – Typical Discharge times [t = R x C x ln(V/V_{0})] for an RC circuit where C = 200pF and V_{0} = 249 Volts:

Table 2 shows calculated discharge rates for the human body model (HBM) onto an ESD grounded mat with surface-to-ground (R_{G}) resistances from 10^{2} to 10^{11} ohms. The more conductive the ESD mat on the workbench is, the faster the discharge, but there is another consideration too.

How fast is too fast? When does the discharge energy at any given time reach a critical level that can damage a semiconductor? The answer depends on several variables relative to the semiconductor’s construction such as line spacing, composition, density, packaging, etc., all leading to an ESD component classification [refer to ESD STM5.1-2007 and the manufactures’ device specifications].

For simplicity’s sake assume the worst case, class 0, which has a 0 to 249 Volt tolerance. Applying the HBM, a conservative worst case capacitance would be 200pF, twice that of the HBM and resistance of 10 kilohms. Therefore, the maximum power (P) level based on Ohm’s Law is P = V^{2}/R (J/s) and the worst case HBM is ((249)^{2}/10K) = 6.2 Watts or Joules per second (Js^{-1}).

The maximum energy (E) stored in a worst case HBM capacitance (C) of 200 pF and at a maximum voltage (V) of 249 Volts, (using E = 1/2 CV^{2}), yields 6.2mJ.

The next concern is to relate energy to time. The time constant (t) is the measure of the length in time, in a natural response system, for the discharge current to die down to a negligible value (assume 1% of the original signal). For an RC circuit, the time constant (t) is equivalent to the multiple of the equivalent resistance and capacitance. In this case, the time constant (t) of our RC circuit is (10 kilohms) x (200pF) or t = 2ms. Discharging this energy upon touching a conductor at zero volts yields a current, (using I = P/V), of (6.2Js^{-1})/(249V) or 24.8mA. To avoid damaging a class 0 ESD sensitive device, the discharge current must be below 24.8mA. Engineering in a “2x” safety factor, the maximum discharge current would be 12.4mA. To maintain a discharge current below 12.4mA, we need to look at our grounding equipment on the ESD sensitive workbench.

Table 3 – Discharge currents from a 6.2 mJ lossless energy source (with C = 200pF & V = 249V) dependent on the discharge time.

The rate at which 6.2mJ of energy discharges is very important. Too fast a discharge will lead to an ESD Event, which can electromagnetically be measured using a simple loop antenna attached to a high impedance input of a high-speed storage scope. The faster the discharge the greater the discharge current becomes as well as the emf (electromotive force) on the loop antenna from the EMI (ElectroMagnetic Interference). Table 3 depicts the discharge current for 6.2mJ at varying discharge times. We are assuming lossless conditions during the discharge for the worst case. For our example, to keep the discharge current below 12.4mA, the discharge rate [from Table 3] must be no quicker than 2.01ms. This energy-based-time constraint forms the lower boundary of the controlled discharge rate.

**Choosing your Matting**

The upper (76.5ms) and lower (2.01ms) boundary of our controlled discharge rate are now defined and can be used to help in choosing the correct ESD mat for an ESD sensitive workstation. ESD mat materials come in many variations. In general, mats are either made from vinyl or rubber material and can be homogeneous or multi-layered. Rubber mats, in general, have good chemical and heat resistance but vinyl tends to be more cost effective. The electrical properties of an ESD mat are important to know in controlling the electrostatic discharge.

An ESD mat will be either electrically conductive or dissipative. Both terms mean that the mat will conduct a charge when grounded. The difference in the terms is defined by the materials resistance, which affects the speed of the discharge. A conductive material has a surface resistivity of less than 1 x 10^{5} ohms/sq and a dissipative material is greater than 1 x 10^{5} ohms/sq but less than 1 x 10^{12} ohms/sq. Anything with a surface resistivity greater than 1 x 10^{12} ohms/sq is considered insulative and will essentially not conduct charges.

Back to our example: If the maximum discharge current of our ESD sensitive device is 12.4mA, then the discharge time based on energy must be slower than 2.01ms and based on body movement must be faster than 76.5ms. Using the discharge times from Table 2 and assuming that the mat has a negligible capacitance relative to the HBM, then the mat resistance must be greater than 2.2 x 10^{3} ohms or 2.2 x 10^{4} ohms/sq and less than 8.3 x 10^{7} ohms or 8.3 x 10^{8} ohms/sq. In other words, a very conductive mat for some applications may be too quick to discharge and yield more dangerous ESD events whether properly grounded or not.

Graph 1 shows the natural response of a 249 Volt discharge in an RC circuit using a capacitance of 200 pF (HBM) into resistances (mat) of 10^{4}, 10^{5}, and 10^{6} ohms. The natural response of the10^{4} ohms curve is below 1% of its’ initial voltage in less than 10ms where the 10^{6} ohms curve takes less than 1ms to discharge to less than 1% (V < 2.49V) of its initial value (V_{0 }= 249V).

**The role of Wrist Straps**

Another defence, and the most common method, to reduce the risk of creating an ESD event is wearing a grounded wrist strap at the workstation. The wrist strap connects the skin (a large conductor) to a common potential (usually power ground). Properly worn, the wrist strap should fit snugly, making proper contact with the skin, to reduce contact resistance.

The wrist strap, since it is connected to ground, will quickly discharge any charge the body either generates through tribocharging or becomes exposed to through induction. Any time the body directly touches a charged conductor, a discharge will occur because the body is at a different potential (0 Volts). Controlling this discharge is important if the conductor is an ESD sensitive device and in minimising induced charges through EMI onto nearby ungrounded ESD sensitive devices.

The electrical properties of the skin of an operator can have a wide range in both resistance and capacitance depending on several variables. An operator’s hand touching a charged device will initiate a discharge at the rate of the time constant of the skin before including the RL properties of the wrist strap. To reduce the potential of an unsafe discharge from a device to a very conductive operator, adding resistance to the operator at the interface from skin to device may be necessary. Some solutions are static dissipative gloves or finger cots, which if worn properly, may add from 1 to 10 megohms to the RC circuit of the skin. This, in turn, slows down the discharge rate to well over 2ms.

**Conclusion**

The upper and lower boundaries of a safe discharge rate are determined by the application and materials used. The movements of the operator define our upper boundary and the max energy, as defined by the ESD sensitive component classification, dictates our lower boundary. We want to design an ESD sensitive workbench to control the discharge rate (via the circuit’s time constant) of our grounded or conductive materials within these limits.

For the HBM and a class 0 device, the materials chosen for a safe ESD workbench should have electrical properties to support discharge rates between 2ms and 76.5ms. These discharge rates, using worst case assumptions, equate to an ESD mat surface with a Resistance-To-Ground (R_{G}) between 2.2 x 10^{3} ohms and 8.3 x 10^{7} ohms. This controlled discharge rate window will vary depending on the class of semiconductor components used (class 0 to class 3B per ESD STM5.1-2007) and the properties of production resources used (human vs. automated).

Please note that the numbers calculated were based on assumptions used to simplify the explanation of the material. Real-world applications are much more complex and require a more detailed analysis, which was beyond the scope of this blog post.

Posted on 2017-03-30, in Articles, ESD Information, Resources, Working Surface Mats and Accessories. Bookmark the permalink. Leave a comment.

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