diff --git a/docs/math.md b/docs/math.md
index 914b9ba..73f2b5b 100644
--- a/docs/math.md
+++ b/docs/math.md
@@ -257,7 +257,7 @@ Higher score ranks earlier.
 
 Current models are intentionally lightweight and fast:
 - Partial mitigation implemented: standardized antenna-height presets (7 m, 10 m, 12 m) now apply a first-order skip-distance scaling model.
-- No explicit R/X feedpoint sweep vs height/ground/conductor diameter.
+- Feedpoint **resistance** is estimated frequency-aware from NEC corpus anchors interpolated on height-in-wavelengths (`nec_calibrated_dipole_r`, §4); the **reactance** ($X$) is not modelled and there is no full R/X sweep vs conductor diameter.
 - No common-mode choke model or ferrite core loss/thermal derating.
 - No full current-distribution solver in the optimization loop.
 
@@ -306,7 +306,35 @@ The $450/f$ rule is a rule-of-thumb starting point, **not** a cut length. A real
 trap dipole's element lengths depend on the trap inductance/capacitance and the
 specific band pair, which this lightweight model does not solve. Treat the output
 as an initial wire estimate and finalise element lengths against the trap
-manufacturer's data or a NEC model.
+manufacturer's data or a NEC model. The **band-pair guidance** of §11 is the more
+useful design output.
+
+## 11) Trap Dipole Guidance (Per Band Pair)
+
+When two or more bands are selected, Rusty Wire emits a per-band-pair guidance
+section (upper band $f_u$, lower band $f_l$, $f_u > f_l$). For each adjacent pair:
+
+- **Inner leg** (per side) — the upper-band element inboard of the trap, cut to a
+  quarter-wave for $f_u$:
+$$
+L_{\mathrm{inner}} = \frac{71.58}{f_u}\,VF \quad(\approx 234.85/f_u\ \mathrm{ft})
+$$
+- **Total leg** (per side) — resonant on the lower band. It is ~4 % shorter than a
+  plain quarter-wave because the trap's inductance electrically lengthens the
+  outer section, so less physical wire reaches $f_l$ resonance:
+$$
+L_{\mathrm{leg}} = \frac{68.58}{f_l}\,VF \quad(\approx 225/f_l\ \mathrm{ft}),\qquad
+L_{\mathrm{outer}} = \max(L_{\mathrm{leg}} - L_{\mathrm{inner}},\,0)
+$$
+- **Trap** — parallel-resonant at $f_u$, isolating the outer section on the upper
+  band. From $f = 1/(2\pi\sqrt{LC})$ the required $L\text{–}C$ product is
+$$
+L[\mu\mathrm{H}]\cdot C[\mathrm{pF}] = \frac{10^6}{4\pi^2\,f_u^2} = \frac{25{,}330}{f_u^2}
+$$
+  and Rusty Wire lists a few practical $(C, L)$ component pairs satisfying it.
+
+This is a first-order single-trap-per-side model; multi-trap and mutual-coupling
+effects are not solved.
 
 ## References
 
diff --git a/src/app/advise.rs b/src/app/advise.rs
index 63a0c6b..66248e2 100644
--- a/src/app/advise.rs
+++ b/src/app/advise.rs
@@ -143,16 +143,24 @@ pub struct AdviseView {
 }
 
 pub fn optimize_transformer_candidates(config: &AppConfig) -> TransformerOptimizerView {
+    let baseline = build_optimizer_calculations(config, TransformerRatio::R1To1);
+    let baseline_avg_half_wave = mean_half_wave_m(&baseline);
+
+    // Representative frequency for the height-in-λ feedpoint-R model: the mean of
+    // the selected bands' centres (falls back to the 7.1 MHz calibration if empty).
+    let repr_freq_mhz = if baseline.is_empty() {
+        7.1
+    } else {
+        baseline.iter().map(|c| c.frequency_mhz).sum::<f64>() / baseline.len() as f64
+    };
     let source_impedance = super::assumed_feedpoint_impedance_ohm(
         config.mode,
         config.antenna_model,
         config.antenna_height_m,
+        repr_freq_mhz,
         config.ground_class,
     );
 
-    let baseline = build_optimizer_calculations(config, TransformerRatio::R1To1);
-    let baseline_avg_half_wave = mean_half_wave_m(&baseline);
-
     let mut candidates: Vec<TransformerOptimizerCandidate> = TRANSFORMER_OPTIMIZER_CANDIDATES
         .iter()
         .copied()
diff --git a/src/app/mod.rs b/src/app/mod.rs
index 401f57d..c71a05d 100644
--- a/src/app/mod.rs
+++ b/src/app/mod.rs
@@ -1160,10 +1160,21 @@ pub fn results_overview_view(results: &AppResults) -> ResultsOverviewView {
     ];
 
     if results.config.antenna_model == Some(AntennaModel::EndFedHalfWave) {
+        let repr_freq_mhz = if results.calculations.is_empty() {
+            7.1
+        } else {
+            results
+                .calculations
+                .iter()
+                .map(|c| c.frequency_mhz)
+                .sum::<f64>()
+                / results.calculations.len() as f64
+        };
         let feedpoint_r = assumed_feedpoint_impedance_ohm(
             results.config.mode,
             results.config.antenna_model,
             results.config.antenna_height_m,
+            repr_freq_mhz,
             results.config.ground_class,
         );
         let cmp = compare_efhw_transformers(feedpoint_r);
@@ -1712,16 +1723,22 @@ pub fn trap_dipole_guidance_view(results: &AppResults) -> Option<TrapDipoleGuida
         let f_upper = upper.freq_center_mhz;
         let f_lower = lower.freq_center_mhz;
 
-        // Quarter-wave inner leg (upper-band driven element per side).
+        // Inner leg: the upper-band element inboard of the trap. Cut to a
+        // (bare-wire) quarter-wave for the upper band — 71.58/f m ≈ 234.85/f ft,
+        // the standard quarter-wave design length. See docs/math.md §11.
         let inner_leg_m = (71.58 / f_upper) * vf;
-        // Trap-dipole total leg per side for the lower band (uses TRAP_DIPOLE_COEFF_M/2).
+        // Total leg (per side) resonant on the lower band: 68.58/f m ≈ 225/f ft.
+        // This is ~4% shorter than a plain quarter-wave (71.32/f) because the
+        // trap's inductance electrically lengthens the outer section, so less
+        // physical wire is needed to reach lower-band resonance.
         let total_leg_m = (68.58 / f_lower) * vf;
         let outer_section_m = (total_leg_m - inner_leg_m).max(0.0);
         let full_span_m = total_leg_m * 2.0;
 
-        // Trap resonant frequency = upper-band centre.
+        // The trap is parallel-resonant at the upper band, isolating the outer
+        // section there so the inner leg acts as a stand-alone upper-band dipole.
         let trap_freq_mhz = f_upper;
-        // L·C product in μH·pF:  L[μH] × C[pF] = 25 330 / f[MHz]²
+        // Resonance f = 1/(2π√(LC)) ⇒ L[μH]·C[pF] = 1e6/(4π²·f[MHz]²) = 25 330/f².
         let lc_product = 25_330.0 / (trap_freq_mhz * trap_freq_mhz);
         let cap_values = select_trap_cap_examples(lc_product);
         let component_examples: Vec<TrapDipoleComponentExample> = cap_values
@@ -3149,6 +3166,7 @@ fn assumed_feedpoint_impedance_ohm(
     mode: CalcMode,
     antenna_model: Option<AntennaModel>,
     antenna_height_m: f64,
+    freq_mhz: f64,
     ground_class: GroundClass,
 ) -> f64 {
     match antenna_model {
@@ -3156,16 +3174,18 @@ fn assumed_feedpoint_impedance_ohm(
         Some(AntennaModel::Dipole)
         | Some(AntennaModel::InvertedVDipole)
         | Some(AntennaModel::HybridMultiSection) => {
-            crate::calculations::nec_calibrated_dipole_r(antenna_height_m, ground_class)
+            crate::calculations::nec_calibrated_dipole_r(antenna_height_m, freq_mhz, ground_class)
         }
         Some(AntennaModel::TrapDipole) => 65.0,
         Some(AntennaModel::FullWaveLoop) => 100.0,
         Some(AntennaModel::EndFedHalfWave) => 2800.0,
         Some(AntennaModel::OffCenterFedDipole) => 200.0,
         None => match mode {
-            CalcMode::Resonant => {
-                crate::calculations::nec_calibrated_dipole_r(antenna_height_m, ground_class)
-            }
+            CalcMode::Resonant => crate::calculations::nec_calibrated_dipole_r(
+                antenna_height_m,
+                freq_mhz,
+                ground_class,
+            ),
             CalcMode::NonResonant => 450.0,
         },
     }
diff --git a/src/calculations.rs b/src/calculations.rs
index f803286..400ac95 100644
--- a/src/calculations.rs
+++ b/src/calculations.rs
@@ -360,7 +360,7 @@ pub fn calculate_for_band_with_environment(
     // classic textbook 73 Ω free-space value. Height and ground affect the radiation
     // resistance through image-method coupling; the NEC values are validated against
     // fnec-rust Hallén solver output (see corpus/reference-results.json).
-    let nominal_feedpoint_r = nec_calibrated_dipole_r(antenna_height_m, ground_class);
+    let nominal_feedpoint_r = nec_calibrated_dipole_r(antenna_height_m, freq, ground_class);
 
     // Use the NEC-calibrated nominal for all transformer-ratio length corrections.
     let corrected_half_wave_m = impedance_corrected_length_m(
@@ -491,13 +491,12 @@ pub fn calculate_for_band_with_environment(
 /// for a half-wave dipole at the given height and ground, derived from fnec-rust
 /// Hallén solver corpus sweeps (corpus/reference-results.json, v2.9.0).
 ///
-/// CAVEAT: the anchor data is measured only at 7.1 MHz (40 m), and interpolation
-/// is on height in *metres*. Radiation resistance actually tracks height in
-/// wavelengths, so 10 m AGL is ~0.24 λ at 40 m but ~0.96 λ at 10 m — these values
-/// are trustworthy near the 40 m band and are a coarse approximation elsewhere.
-/// The model also reports only R (the corpus reactance is not applied). A
-/// height-in-λ reparameterisation is tracked as future work once multi-frequency
-/// NEC sweep data is committed.
+/// The interpolation is on height-in-**wavelengths** (`h/λ = height·f/c`), so the
+/// estimate is frequency-aware and reproduces the 40 m calibration exactly. The
+/// underlying anchor magnitudes are still measured only at 7.1 MHz, and only R is
+/// modelled (corpus reactance is not applied), so values away from 40 m remain a
+/// coarse first-order estimate until a full multi-frequency NEC sweep is
+/// committed (GAP-011).
 ///
 /// Reference data (7.1 MHz, 2 mm wire, 51 segments, bare-wire ~0.95 end-effect cut):
 ///   free space:          R ≈  62.94 Ω
@@ -509,13 +508,55 @@ pub fn calculate_for_band_with_environment(
 ///
 /// For heights other than 7/10/12 m the value is linearly interpolated.
 /// Ground-class offset at 10 m is applied as a calibrated delta.
-pub fn nec_calibrated_dipole_r(antenna_height_m: f64, ground_class: GroundClass) -> f64 {
-    // Anchor table: resistance at each height with "good" ground (from NEC corpus).
-    const H7_GOOD: f64 = 73.03; // 7 m AGL, good soil
-    const H10_GOOD: f64 = 52.84; // 10 m AGL, good soil
-    const H12_GOOD: f64 = 45.56; // 12 m AGL, good soil
+pub fn nec_calibrated_dipole_r(
+    antenna_height_m: f64,
+    freq_mhz: f64,
+    ground_class: GroundClass,
+) -> f64 {
+    // A horizontal dipole's radiation resistance tracks its height in WAVELENGTHS
+    // (image-method ground coupling), not raw metres. Re-express the NEC corpus
+    // anchors — measured at 7.1 MHz, 7/10/12 m AGL, "good" ground — as height-in-λ,
+    // then interpolate on the actual band's h/λ. This reproduces the 40 m
+    // calibration exactly (10 m @ 7.1 MHz → 0.237 λ → 52.84 Ω) while making the
+    // estimate frequency-aware: at 20 m a 10 m mast is ~0.47 λ, not ~0.24 λ, and
+    // gets a correspondingly higher R. A free-space anchor at 0.5 λ lets high
+    // antennas / high bands relax toward the measured free-space value instead of
+    // clamping to the 12 m figure. Still a coarse first-order model until a full
+    // multi-frequency NEC sweep is committed (GAP-011).
+    const LAMBDA_CAL_M: f64 = 299.792_458 / 7.1; // wavelength at the calibration freq
+    const FREE_SPACE_R: f64 = 62.94; // NEC corpus free-space R (high-antenna asymptote)
+
+    // (height-in-λ, R at "good" ground), ascending in h/λ.
+    let anchors: [(f64, f64); 4] = [
+        (7.0 / LAMBDA_CAL_M, 73.03),  // 0.166 λ  (7 m @ 7.1 MHz)
+        (10.0 / LAMBDA_CAL_M, 52.84), // 0.237 λ  (10 m @ 7.1 MHz)
+        (12.0 / LAMBDA_CAL_M, 45.56), // 0.284 λ  (12 m @ 7.1 MHz)
+        (0.5, FREE_SPACE_R),          // half-wave height: ground coupling weakens
+    ];
+
+    let h_over_lambda = if freq_mhz > 0.0 {
+        antenna_height_m * freq_mhz / 299.792_458
+    } else {
+        10.0 / LAMBDA_CAL_M
+    };
 
-    // Ground-class correction deltas at 10 m AGL (NEC corpus deltas relative to "good"):
+    // Piecewise-linear interpolation on h/λ; hold the end anchors beyond the range.
+    let h_good = if h_over_lambda <= anchors[0].0 {
+        anchors[0].1
+    } else if h_over_lambda >= anchors[anchors.len() - 1].0 {
+        anchors[anchors.len() - 1].1
+    } else {
+        anchors
+            .windows(2)
+            .find(|w| h_over_lambda >= w[0].0 && h_over_lambda <= w[1].0)
+            .map(|w| {
+                let ((x0, y0), (x1, y1)) = (w[0], w[1]);
+                y0 + (h_over_lambda - x0) / (x1 - x0) * (y1 - y0)
+            })
+            .unwrap_or(FREE_SPACE_R)
+    };
+
+    // Ground-class deltas (NEC corpus, at 10 m / 7.1 MHz; small, applied across bands):
     //   average - good ≈ +1.51 Ω;  poor - good ≈ +3.54 Ω
     let ground_delta: f64 = match ground_class {
         GroundClass::Good => 0.0,
@@ -523,19 +564,6 @@ pub fn nec_calibrated_dipole_r(antenna_height_m: f64, ground_class: GroundClass)
         GroundClass::Poor => 3.54,
     };
 
-    // Interpolate the height-dependent "good" baseline.
-    let h_good = if antenna_height_m <= 7.0 {
-        H7_GOOD
-    } else if antenna_height_m >= 12.0 {
-        H12_GOOD
-    } else if antenna_height_m <= 10.0 {
-        let t = (antenna_height_m - 7.0) / (10.0 - 7.0);
-        H7_GOOD + t * (H10_GOOD - H7_GOOD)
-    } else {
-        let t = (antenna_height_m - 10.0) / (12.0 - 10.0);
-        H10_GOOD + t * (H12_GOOD - H10_GOOD)
-    };
-
     (h_good + ground_delta).clamp(30.0, 90.0)
 }
 
@@ -1787,6 +1815,36 @@ mod tests {
         assert!(!pts_thin.is_empty() && !pts_thick.is_empty());
     }
 
+    #[test]
+    fn nec_calibrated_r_is_frequency_aware_and_preserves_40m_calibration() {
+        // 40 m calibration reproduced exactly (h/λ hits the measured anchors).
+        assert!((nec_calibrated_dipole_r(7.0, 7.1, GroundClass::Good) - 73.03).abs() < 0.05);
+        assert!((nec_calibrated_dipole_r(10.0, 7.1, GroundClass::Good) - 52.84).abs() < 0.05);
+        assert!((nec_calibrated_dipole_r(12.0, 7.1, GroundClass::Good) - 45.56).abs() < 0.05);
+
+        // The same 10 m mast is a larger fraction of a wavelength on 20 m, so R
+        // rises toward free space relative to the 40 m case.
+        let r_40 = nec_calibrated_dipole_r(10.0, 7.1, GroundClass::Good);
+        let r_20 = nec_calibrated_dipole_r(10.0, 14.175, GroundClass::Good);
+        assert!(r_20 > r_40, "R should rise on 20 m ({r_20} vs {r_40})");
+
+        // High band / high antenna relaxes to the free-space asymptote (~62.94 Ω).
+        let r_10m_band = nec_calibrated_dipole_r(10.0, 28.5, GroundClass::Good);
+        assert!(
+            (r_10m_band - 62.94).abs() < 0.5,
+            "R should approach free space ({r_10m_band})"
+        );
+
+        // Ground-class ordering preserved at a fixed height/frequency.
+        assert!(
+            nec_calibrated_dipole_r(10.0, 7.1, GroundClass::Poor)
+                > nec_calibrated_dipole_r(10.0, 7.1, GroundClass::Good)
+        );
+
+        // Degenerate frequency falls back to the calibration point.
+        assert!((nec_calibrated_dipole_r(10.0, 0.0, GroundClass::Good) - 52.84).abs() < 0.05);
+    }
+
     // ── Invariant / property sweeps ───────────────────────────────────────────
 
     /// Resonant lengths must decrease strictly as frequency rises (L ∝ 1/f).