BLT Equation
Understanding the BLT Equation
The BLT equation treats a cable network as a collection of transmission line segments connected at junctions. Each segment has a propagation matrix P (describing wave travel and attenuation). Each junction has a scattering matrix S (describing how waves reflect and transmit at connections). External sources (incident fields, lightning currents) couple energy into the segments.
The framework handles shielded cables (using transfer impedance), multi-wire bundles, and arbitrary network topologies. Solutions are computed in the frequency domain and transformed to time domain for transient analysis.
Where:
I = identity supermatrix
S = scattering supermatrix (junctions)
P = propagation supermatrix (segments)
V = junction voltage vector
Vs = source vector (field coupling)
BLT Application Domains
| Domain | Threat | Network | Output |
|---|---|---|---|
| HEMP | EMP E1/E2/E3 | Facility cables | Pin voltages |
| Lightning | Direct/indirect strike | Aircraft harness | Transient currents |
| Automotive | Radiated immunity | CAN/LIN buses | Error voltages |
| Nuclear | Seismic + EMP | Cable trays | Safety margins |
Frequently Asked Questions
What does BLT stand for?
Baum-Liu-Tesche, 1978. Developed for EMP coupling to cable networks. Extends transmission line theory to arbitrary network topologies.
How structured?
[I−S·P]·V = S·Vs. S=scattering (junctions), P=propagation (segments), Vs=external sources. Solves all junction voltages.
Applications?
HEMP hardening, lightning protection, automotive EMC, nuclear cable analysis. Any complex cable network with field coupling.