A plain-language guide to grounding and bonding strap inductance: why impedance rather than DC resistance governs a bond's effectiveness at RF, and why a wide flat strap beats a round-wire pigtail of the same length.
Measure a grounding strap or bonding jumper with a multimeter and it will read a fraction of an ohm — by DC resistance alone, it looks like an excellent connection. But EMC problems rarely live at DC. At any real frequency, what matters is impedance, not resistance, and a straight conductor's impedance is dominated by its self-inductance: Z = 2π·f·L. Because that grows directly with frequency, a strap that's essentially a short circuit at 60Hz can present tens of ohms at 100MHz — enough to completely defeat the purpose of the bond.
Even a straight length of wire or strap, with no coil or loop in sight, has self-inductance — the classical Grover/Terman result for a straight conductor's external inductance depends on its length and its cross-sectional geometry: a flat strap follows L(nH) = 0.2·l·[ln(2l/(w+t)) + 0.2235·(w+t)/l + 0.5] and a round wire follows L(nH) = 0.2·l·[ln(4l/d) − 1] (all dimensions in mm). Both share the same dominant behavior — inductance scales roughly with length and only logarithmically with cross-section — which is the key insight for grounding practice: length matters far more than how thick the conductor is.
For the same length, a wide flat strap has meaningfully lower inductance than a round wire — because the logarithmic term depends on the conductor's width-plus-thickness rather than just its diameter, a strap with the same cross-sectional area as a wire, but spread wide and thin instead of round, presents noticeably less impedance. This is the physical basis for one of the most repeated pieces of EMC grounding advice: replace a wire "pigtail" with a flat strap wherever possible, and keep it as short as the installation allows.
← All guides · Open the Grounding / Bond Strap Inductance Calculator