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The overlap between a printed resistor and its conductor termination is an electrical transition region. Increasing the visible overlap may improve registration margin, but it also changes where current transfers between materials. To evaluate that region, keep the resistor body, process sequence and sensing boundary controlled. A useful overlap study identifies which contribution changes and whether the same result survives ordinary dimensional variation.
Key design decisions
- Define nominal and minimum actual overlap from both printed layers and their relative registration.
- Measure several resistor lengths so body resistance can be separated from combined terminal contributions.
- Evaluate both low-excitation resistance and the relevant powered condition before accepting an overlap change.
Define the overlap in the processed geometry
The artwork may show one layer extending beneath another, but the electrical structure depends on the actual conductor and resistor edges after processing. Record which material is printed first, which stages are fired or cured, and which boundary defines the nominal resistor length. Changing that length definition between studies can make an overlap effect appear larger or smaller than it is.
Measure overlap at several locations across the terminal width. A skewed edge can provide generous overlap on one side and little overlap on the other. A single centerline dimension misses that condition. Include the actual lateral alignment and terminal width, particularly where the conductor is narrower than the resistor or where current enters from one side.
Use a body-plus-ends model as a diagnostic
A first diagnostic model writes total measured resistance as the body contribution plus two end contributions. For rectangular bodies of fixed width, body resistance changes approximately linearly with length. The intercept of a length series then represents the combined length-independent contribution under the chosen sensing boundary.
This decomposition is useful even though a real transition is distributed rather than a point contact. It becomes unreliable if short structures have overlapping end regions or if printing thickness changes with resistor length. Examine the residuals and actual geometry. Do not label an intercept as pure interface resistance when it also includes conductor spreading, attachment resistance or a mismatch in the chosen length origin.
Rtotal(L) ≈ (Rs/W)L + Rend1 + Rend2
- Rs is the effective sheet resistance of the uniform body region.
- W and L are the processed body width and defined body length.
- Rend1 and Rend2 include transition contributions inside the measurement boundary.
Widths and processes are comparable, end contributions are approximately length-independent, and the end regions do not strongly interact.
Change overlap independently from the resistor length
Use a matrix of overlap lengths and several body lengths. Keep conductor composition, resistor composition, width and processing sequence fixed within each comparison. Position repeated structures across the same substrate so location effects can be distinguished from the nominal design change. Record the measured dimensions instead of fitting against artwork dimensions alone.
A minimal two-length comparison can reveal a trend, but it cannot show whether the relationship is actually linear. Additional lengths provide a check on the model and help identify short structures for which the end regions are no longer independent. Repeats at each geometry are also necessary: without them, a single unusual print can be mistaken for a systematic overlap effect.
Interpret slope and intercept separately
Suppose a hypothetical fixed-width series gives 120, 220 and 320 ohms at defined lengths of one, two and three millimeters. The fitted slope is 100 ohms per millimeter and the intercept is 20 ohms. If a revised overlap gives 110, 210 and 310 ohms, the unchanged slope and ten-ohm intercept suggest that the length-independent contribution has changed.
If the revised series instead gives 110, 200 and 290 ohms, the slope falls to 90 ohms per millimeter while the intercept remains 20 ohms. Investigate the resistor body process and dimensions first, retaining the terminal-region comparison as a control. An unchanged fitted intercept alone does not prove an unchanged contact interface. These numbers are calculation examples, not measured material performance. Their purpose is to show why total resistance from one geometry cannot uniquely separate contact improvement from a change in the resistor body.
Choose evidence that distinguishes competing explanations
The same lower total resistance can have several causes. Use paired electrical and dimensional observations to distinguish them, and retain the original specimens until the explanation is settled. A resistance target met by compensating errors can become unstable when one process contribution shifts.
| Observed result | Possible explanation | Next discriminating check |
|---|---|---|
| Intercept changes while slope remains similar | A terminal-region contribution has changed | Inspect overlap and conductor spreading at the same sense boundary |
| Slope changes across every overlap | Body sheet resistance or width has changed | Measure body dimensions and a separate sheet-resistance reference |
| Only the shortest resistors deviate | End regions interact or length definition is unsuitable | Add intermediate lengths and inspect the transition extent |
| Results scatter with lateral registration | Current transfer is sensitive to asymmetric overlap | Map minimum overlap across the full terminal width |
| Low-current values agree but powered values differ | Localized terminal heating or nonlinear contact is relevant | Compare voltage distribution and temperature at controlled power |
Keep the voltage-sensing boundary constant
Four-wire measurement separates force-lead voltage drop from the measured voltage, but the sense locations determine whether conductor and overlap regions are included. Use fixed coordinates and ensure the force contacts do not mechanically disturb the terminal. For a low-value structure, even a small shift along a resistive conductor can alter the measured result.
A resistor-length series can separate a body-related slope from end and contact contributions when the assumed linear model is valid. Validate that decomposition using the actual processed thick-film geometry and material pair. Do not transfer thin-film material values or aging behavior to the printed construction merely because the same fitted relationship is used.
Include process order and local power in the study
Overlap geometry cannot be evaluated independently of material compatibility and process order. A conductor printed over a resistor may create a different transition from a resistor printed over a conductor. Repeated thermal cycles and subsequent protective layers can also alter the final structure. Preserve those stages in the experimental record rather than reporting only a nominal peak process temperature.
At the relevant current, examine whether appreciable voltage drop is concentrated near an end. Local electrical loss can create a hot region even when the total resistor power seems moderate. Compare both terminals because asymmetric feed geometry or attachment can produce unequal behavior. Any destructive examination should follow the electrical and thermal measurements, so the original transition remains available for diagnosis.
Translate the study into drawing and inspection controls
Specify overlap as a functional region with a minimum processed condition, registration allowance and inspectable edge definition. Include permitted defects or exclusions only when they are tied to the agreed evaluation. Avoid adding a very tight overlap tolerance merely because the artwork system can display it; the tolerance should reflect the electrical sensitivity and the demonstrated measurement method.
The final design review should connect overlap, body length and termination sensing to the same drawing revision. If trimming compensates the initial resistance, retain untrimmed study results as well. Otherwise, the adjustment can hide an end contribution that later changes with load or processing. A stable finished value is best supported by an understood transition and a controlled body, each within the project's operating conditions.
Provide the conductor-resistor transition details
Include both layers and the process sequence so overlap can be evaluated as an electrical interface.
- Layer drawings with resistor length definition, terminal width and nominal overlap.
- Measured registration and processed edge dimensions from available samples.
- Conductor and resistor material identification with printing and thermal sequence.
- Resistance-versus-length data and exact Kelvin sense positions.
- Operating current, mounting conditions and any observed terminal heating or drift.
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