1.1 The Phenomenon
Cold air damming (CAD) is a mesoscale meteorological phenomenon in which a shallow, cold, stable air mass becomes mechanically trapped against the eastern slope of a mountain barrier and resists displacement by an approaching synoptic-scale warm or moist air mass. The cold pool is not simply advected cold air — it is a dynamically maintained structure whose persistence depends on a continuous balance between the pressure gradient force trying to push it away, the terrain blocking it from draining westward, and its own negative buoyancy anchoring it against the slope.
The phenomenon was named and systematically described by Forbes et al. (1987), but Bailey et al. (2003) produced the first rigorous climatological algorithm for automated identification. Miller et al. (2014) — the CADEX paper — extended detection into the New Hampshire White Mountains with a modified approach. The PA system inherits architecture from both.
Adjust column temperatures to see how the cold, dense air column produces anomalously high surface pressure — the CAD mesohigh.
1.2 The Three-Layer Physical Mechanism
Layer 1 — Terrain Blocking & Hydrostatic Pressure Perturbation
When a cold, dense air mass impinges on the eastern Appalachian slope, it cannot easily cross the ridge crest. The terrain acts as a dam. The cold air pools on the eastern side, deepening until its hydrostatic pressure at the base of the barrier exceeds ambient pressure to the east. This creates a mesohigh — a local pressure maximum entirely caused by the cold column's weight.
Δp = (p₀ · g · Δz) / (Rᴅ · T̄)
// Warm col (288K, 1500m): Δp = 154.2 hPa pressure drop
// Cold col (275K, 1500m): Δp = 161.4 hPa pressure drop
// → Cold column surface pressure ~7 hPa HIGHER = CAD mesohigh
Layer 2 — Static Stability & Cold Pool Resistance
The trapped cold air is statically stable — potential temperature θ increases with height. Any parcel forced upward is negatively buoyant and resists displacement. This is why CAD events persist 12–72 hours even when synoptic flow above is southwesterly and warm.
// A statically stable layer: ∂θ/∂z > 0
// Cold pool: lower θ at surface than aloft → resists uplift
Layer 3 — Geostrophic Adjustment & the Low-Level Jet
Once the mesohigh forms, the pressure gradient force drives eastward flow. Coriolis deflects this rightward in the NH, producing the characteristic northeasterly low-level jet along the mountain front. This is not the cause of CAD — it's a consequence. Bailey detects the pressure structure; the wind is a diagnostic confirmation.
f at MDT (40.19°N) = 2 · 7.292×10⁻⁵ · sin(40.19°) = 9.44×10⁻⁵ s⁻¹
1.3 How Bailey (2003) Defines CAD
Bailey defines a CAD event as a period where all five criteria are simultaneously true for ≥ 6 consecutive hours:
- C1Mesoscale pressure ridge present along eastern slope → positive ∇²p across mountain-normal rib
- C2Cold pool with stable lower troposphere → negative ∇²θ across same rib
- C3Parent anticyclone identifiable within ~2000 km (closed 1024+ hPa isobar)
- C4850 hPa flow not strongly southwesterly (< 225°–315° at > 15 kts)
- C5Positive SLP gradient from mountain anchor to coast (Line D criterion)
1.4 How CADEX (Miller et al., 2014) Defines CAD
CADEX takes a broader view: any event where cold air is terrain-trapped and produces a measurable θᵥ anomaly, regardless of synoptic pattern. Requirements:
- C1Positive virtual potential temperature (θᵥ) difference between upslope and downslope anchor stations
- C2CADINX value exceeds minimum threshold
- C3Minimum duration of 3 hours (vs Bailey's 6)
CADEX drops the parent anticyclone requirement and the Line D criterion entirely. This captures in-situ events — cold air forming locally through radiative cooling or orographic drainage — that Bailey systematically misses.
1.5 Where the Definitions Diverge — PA Implications
| Criterion | Bailey (2003) | CADEX (2014) | PA Recommendation |
|---|---|---|---|
| Core variable | Dry θ (T, p) | Virtual θᵥ (T, p, Td) | Use θᵥ — Ridge-and-Valley moisture variability is large |
| Spatial operator | Laplacian ∇²(·) on 3-station rib | First difference, 2-station pair | Use Laplacian — single-diff misses mesohigh concavity |
| Pressure check | ∇²p required | Not present | Retain — MDT mesohigh is real and detectable |
| Parent anticyclone | Required | Not required | Require for CDEN/CDRY; relax for INST events |
| Persistence | 6 hours | 3 hours | 6 hr classical / 3 hr in-situ |
| Domain extent | TN → VA | NH White Mountains | Neither covers PA directly |
1.6 Key Vocabulary
Temperature a dry air parcel would have if brought adiabatically to 1000 hPa. Conserved under dry adiabatic processes. Units: Kelvin.
Temperature a dry parcel would need to match density of a moist parcel. Tᵥ = T(1 + 0.608q). Moist air is less dense than dry air at same T.
Second spatial derivative — measures curvature of a scalar field. Negative ∇²p at midpoint = local pressure maximum = CAD mesohigh.
Longer segment ÷ shorter segment in a 3-station rib. Ratio of 1.0 = perfectly symmetric. High ratios degrade the Laplacian approximation.
Bailey's mountain-to-coast SLP gradient check. SLP at mountain anchor must exceed SLP at coastal anchor. Uses SLP (not station pressure) only for this criterion.
Mesoscale pressure maximum produced by the weight of the cold column against terrain. Distinct from the synoptic anticyclone. What the Laplacian is detecting.
2.1 The Geometric Logic of a Three-Station Rib
Bailey's algorithm is not simply "three stations in a line." It is a discrete approximation of a second-order spatial derivative (the Laplacian) oriented perpendicular to the mountain barrier. Every geometric property — bearing, segment lengths, balance ratio, station elevations — directly affects the accuracy of that approximation.
Four requirements for a valid rib:
- G1Mountain-normal orientation: Appalachian ridge axis ~030°–210°. Mountain-normal = roughly 100°–120°. PIT→MRB→ACY (101.6°) and ERI→IPT→LGA (103.3°) both qualify.
- G2Sufficient total length: Must span the full CAD perturbation — upstream reference, mesohigh core, downstream reference. Target ~490–550 km for the PA/Appalachian system.
- G3Balance ratio near 1.0: Bailey accepted up to ~1.65. Above ~2.0 the Laplacian becomes unreliable without explicit correction. CRW→RIC→ORF at 3.20 is definitively disqualified.
- G4Correct terrain positioning: A west of barrier crest (unperturbed upstream); B on eastern slope where mesohigh centers; C well east in coastal plain (unperturbed downstream).
Bailey's original southern network (solid) + PA Mid-Atlantic extensions (dashed). Click any rib or station for details.
2.2 Bailey's Original Southern Network
| Route | Role | Total km | Bearing | Ratio | Laplacian? |
|---|---|---|---|---|---|
| TYS→GSP→CHS | Southern rib | 490.1 | 130.7° | 1.58 | ✓ Yes |
| TYS→GMU→CHS | S rib alt (pre-1962) | 487.4 | 130.7° | 1.65 | ✓ Yes |
| TRI→GSO→ILM | Central rib (best balanced) | 500.1 | 119.6° | 1.22 | ✓ Yes |
| CRW→LYH→ORF | Northern rib (PA parent) | 511.4 | 107.4° | 1.13 | ✓ Yes |
| GSP→GSO→RIC | Spine (along-barrier) | 525.7 | 55.1° | 1.15 | Spine only |
The spine at 55.1° is roughly perpendicular to the ribs (~120°). This orthogonality is intentional — ribs measure the cross-barrier gradient, the spine measures the along-barrier gradient. Together they give Bailey a 2D picture of the pressure field from surface stations alone.
2.3 Your Mid-Atlantic PA Extension
| Route | Bearing | Ratio | Role | Valid? | Issue |
|---|---|---|---|---|---|
| PIT→MRB→ACY | 101.6° | 1.29 | Primary PA rib | ✓ | Asymmetric correction needed |
| ERI→IPT→LGA | 103.3° | 1.10 | Northern PA rib | ✓ | Lake-effect screen needed at ERI |
| CRW→RIC→ORF | 107.4° | 3.20 | — | ✗ | Ratio too high — disqualified |
| RIC→BWI→ABE | 24.3° | 1.01 | Spine only | Spine | Nearly meridional — parallel to front |
Why CRW→RIC→ORF is Disqualified (ratio 3.20)
With segments 386.3 km and 120.9 km, the symmetric Laplacian assigns equal weight to a synoptic-scale gradient (386 km) and a mesoscale gradient (121 km). These are physically incommensurable — averaging them produces a meaningless second derivative. The ratio-3.20 rib cannot reliably detect the CAD mesohigh.
Why RIC→BWI→ABE is a Spine (bearing 24.3°)
Despite having the most perfect balance ratio (1.01) in the entire dataset, this route runs nearly north-south — parallel to the Appalachian front, not perpendicular to it. All three stations (RIC, BWI, ABE) sit on the eastern slope and are likely inside the cold pool simultaneously during CAD. Use it as the PA spine for the along-barrier gradient check.
3.1 Why the Variable Choice Matters
Bailey uses dry potential temperature (θ) — temperature and pressure only. CADEX uses virtual potential temperature (θᵥ), which adds a moisture correction. In a typical late-autumn PA CAD event: the cold pool at MDT might have T=4°C, Td=1°C (nearly saturated), while ACY has T=12°C, Td=2°C (warmer but drier). The moisture correction increases the density contrast between the cold-moist pool and the warm-dry air at ACY — making the signal stronger in θᵥ than in dry θ by ~0.27 K. In summer CAD events this difference can be large enough to reverse the sign of the density difference if dry θ is used. This is why the PA algorithm adopts θᵥ.
3.2 Station Pressure vs. SLP
Both algorithms require station pressure (actual pressure at station elevation), not SLP. The SLP reduction introduces errors of 1–3 hPa during CAD events with sharp surface inversions — large enough to contaminate the Laplacian signal.
MDT example: z = 93m, SLP = 1018.0 hPa
p_s = 1018.0 · exp(−93/8430) = 1018.0 × 0.98904 = 1006.8 hPa
// 11.2 hPa difference — critical to compute consistently across all rib stations
3.3 Potential Temperature (θ) — Full Derivation
From the first law of thermodynamics applied to a dry adiabatic process, entropy is conserved. Setting entropy equal at the parcel's actual state (T, p) and at the reference state (θ, p₀=1000 hPa):
Constants:
· T in Kelvin: T_K = T_C + 273.15
· p₀ = 1000 hPa (reference)
· Rᴅ = 287.05 J kg⁻¹ K⁻¹
· cₚ = 1004.0 J kg⁻¹ K⁻¹
· κ = Rᴅ/cₚ = 0.28541 (Poisson's ratio)
Adjust T, Td, and p_s at any station to see the full T → p_s → e_s → e → w → T_v → θᵥ chain computed in real time.
3.4 The Full θᵥ Derivation Chain
Step 1 — Saturation Vapor Pressure (August-Roche-Magnus)
MDT (T = 4.0°C): eₛ = 6.1078 · exp(69.078/241.29) = 6.1078 × 1.3315 = 8.131 hPa
Step 2 — Actual Vapor Pressure from Dew Point
MDT (Td = 1.0°C): e = 6.1078 · exp(17.2694/238.29) = 6.567 hPa
RH check: 6.567/8.131 × 100 = 80.8% ← consistent with saturated CAD air mass
Step 3 — Mixing Ratio
MDT: w = (0.622 × 6.567) / (1006.8 − 6.567) = 4.085/1000.23 = 4.084 g kg⁻¹
Step 4 — Virtual Temperature
MDT: Tᵥ = 277.15 × (1 + 0.608×0.004067) = 277.15 × 1.002473 = 277.84 K
Moisture correction: +0.69 K
Step 5 — Virtual Potential Temperature
MDT: θᵥ = 277.84 × (1000/1006.8)^0.28541 = 277.84 × 0.99807 = 277.30 K
3.5 Full Variable Summary Table
| Station | Role | T (°C) | Td (°C) | pₛ (hPa) | w (g kg⁻¹) | Tᵥ (K) | θ (K) | θᵥ (K) |
|---|---|---|---|---|---|---|---|---|
| PIT | Mountain | 7.0 | −1.0 | 977.6 | 3.634 | 280.77 | 281.97 | 282.59 |
| MRB | Cold pool | 2.0 | 0.5 | 999.9 | 3.966 | 275.81 | 275.16 | 275.82 |
| ACY | Coastal | 12.0 | 5.0 | 1017.5 | 5.379 | 286.08 | 283.74 | 284.67 |
3.6 Sensitivity Analysis
| Input | ASOS Accuracy | Effect on θᵥ | Algorithm Consequence |
|---|---|---|---|
| Temperature T | ±0.3°C | ±0.30 K | Dominant error source |
| Dew point Td | ±0.5°C | ±0.05–0.15 K | Secondary — matters most at ACY |
| Station pressure pₛ | ±0.3 hPa | ±0.08 K | Small at low elevation; larger at PIT |
Combined θᵥ uncertainty: ±0.35–0.45 K per station. Across the rib, Laplacian uncertainty is roughly ±0.7–1.0 K from sensor noise alone — directly informing the threshold values in Part IV.
4.1 What the Laplacian Measures
The Laplacian is the second spatial derivative — it measures the curvature of a scalar field. On a three-station rib, it detects whether the midpoint station is a local maximum (hill-shaped = ridge) or minimum (bowl-shaped = trough) relative to the two endpoints.
· ∇²p < 0 → pressure concave-down at B → local pressure maximum = CAD mesohigh ✓
· ∇²θᵥ > 0 (or CPI > 0) → θᵥ concave-up at B → local θᵥ minimum = cold pool ✓
Both must be satisfied simultaneously for Bailey's joint trigger.
4.2 Symmetric vs. Asymmetric Laplacian
The standard symmetric three-point Laplacian assumes equal segment lengths d:
⚠ Only valid when d₁ = d₂. Significant bias when balance ratio ≠ 1.0
For unequal segments d₁ (A→B) and d₂ (B→C), the asymmetric (generalized) discrete Laplacian is required:
// Reduces to symmetric form when d₁ = d₂ = d
Adjust station pressures and θᵥ values. Both the symmetric and asymmetric Laplacians are computed in real time, showing the bias introduced by using the wrong formula.
4.3 Worked Example: Pressure Laplacian on PIT→MRB→ACY
Using the Part III CAD scenario: pₛ(PIT)=977.6, pₛ(MRB)=999.9, pₛ(ACY)=1017.5 hPa. Segments d₁=226.7 km, d₂=292.7 km.
(p_C − p_B)/d₂ = (1017.5 − 999.9)/292.7 = +0.06012 hPa km⁻¹
(p_B − p_A)/d₁ = (999.9 − 977.6)/226.7 = +0.09837 hPa km⁻¹
Step 2 — Second difference:
0.06012 − 0.09837 = −0.03825 hPa km⁻¹ ← NEGATIVE = pressure increasing faster west→east on west segment
Step 3 — Asymmetric Laplacian:
∇²p = [2/519.4] × (−0.03825) = 0.003851 × (−0.03825)
∇²p = −0.0001473 hPa km⁻² = −1.473 hPa/(100km)²
MRB is 4.9 hPa above linear interpolation → CAD mesohigh confirmed
4.4 Potential Temperature Laplacian (CPI)
(θᵥ_C − θᵥ_B)/d₂ = (284.67−275.82)/292.7 = +0.03023 K km⁻¹
(θᵥ_B − θᵥ_A)/d₁ = (275.82−282.59)/226.7 = −0.02987 K km⁻¹
∇²θᵥ = [2/519.4] × (0.03023 − (−0.02987)) = 0.003851 × 0.06010
∇²θᵥ = +0.0002314 K km⁻² = +2.314 K/(100km)²
// POSITIVE = MRB is a θᵥ minimum (cold pool) → define CPI = −∇²θᵥ convention
CPI = +2.314 K/(100km)² ← cold pool confirmed
4.5 The Line D Criterion
SLP_PIT = 977.6 + 43.4 = 1021.0 hPa (elevation correction added back)
SLP_ACY = 1017.5 + 2.3 = 1019.8 hPa
ΔpₗᵢₙₑD = 1021.0 − 1019.8 = +1.2 hPa ✓ Positive gradient = CAD consistent
// Line D uses SLP only — the one place in Bailey's algorithm where SLP is appropriate,
// because it removes the elevation-driven difference and isolates the meteorological gradient
4.6 The Joint Trigger
∇²p < Tₚ AND CPI > T_θ AND ΔpₗᵢₙₑD > TₗᵢₙₑD
All three must be satisfied simultaneously for ≥ 6 consecutive hours
| Criterion | Value | Threshold | Met? |
|---|---|---|---|
| ∇²p (pressure Laplacian) | −1.473 hPa/(100km)² | < −0.5 | ✓ YES |
| CPI (cold pool index) | +2.314 K/(100km)² | > +1.0 | ✓ YES |
| Line D (SLP gradient) | +1.2 hPa | > 0 hPa | ✓ YES |
4.7 Symmetric vs. Asymmetric — Quantifying the Bias
For PIT→MRB→ACY (ratio 1.29): using the symmetric formula with d = average segment = 259.7 km gives ∇²p = −0.697 hPa/(100km)². The correct asymmetric result is −1.473 hPa/(100km)².
5.1 CADEX Architecture Overview
Where Bailey builds upward from a second-order spatial operator (the Laplacian), CADEX builds from a simpler first-order difference applied to a more physically complete variable (θᵥ). The CADINX is fundamentally a weighted potential temperature difference between the upslope and downslope stations, computed across a two-station pair rather than a three-station rib.
This reflects the different terrain of the White Mountains. In New Hampshire, the ridges are shorter, more irregular, and more densely spaced than in the southern Appalachians. A three-station rib spanning 500 km would cross several independent terrain features. Miller et al. chose shorter, more localized two-point transects that each capture one specific terrain-trapping geometry.
The consequence for PA: CADINX alone is insufficient. It cannot distinguish between a deep, mesohigh-anchored CAD pool and simple cold air advection on a flat pressure gradient. Bailey's Laplacian detects the mesohigh explicitly. The PA algorithm needs both.
5.2 The CADINX Formula (PA Adaptation)
During a PA CAD event, the cold pool occupies the eastern slope. The midslope station (MRB or IPT) is the coldest. The PA midpoint-depression formulation is:
· Negative = B is colder than endpoint mean = cold pool present
· More negative = deeper cold pool
· Equivalent to (−1/2) × symmetric Laplacian × d²
Part III scenario:
CADINX_PA = 275.82 − (282.59 + 284.67)/2 = 275.82 − 283.63 = −7.81 K
5.3 Intensity Classification
| Class | CADINX_PA threshold | Physical description | Typical PA scenario |
|---|---|---|---|
| Weak | −2 K > CADINX_PA ≥ −5 K | Shallow cold pool, marginal damming, easily eroded by daytime heating | Warm season, nocturnal valley cold pools |
| Moderate | −5 K > CADINX_PA ≥ −10 K | Well-established cold pool, classical damming present | Cold season, post-frontal high, MDT freezing rain |
| Strong | CADINX_PA < −10 K | Deep pool, persistent damming, surface icing likely | CDEN events with strong Canadian high |
5.4 Worked Example: CADINX on JST→MDT→PHL
JST: T=6.0°C, Td=0.0°C, pₛ=988.5 hPa → θᵥ = 280.1 K
MDT: T=3.0°C, Td=1.0°C, pₛ=1006.8 hPa → θᵥ = 275.9 K
PHL: T=11.0°C, Td=5.0°C, pₛ=1016.2 hPa → θᵥ = 283.1 K
CADINX_PA = 275.9 − (280.1 + 283.1)/2 = 275.9 − 281.6 = −5.7 K
Classification: MODERATE — well-established cold pool at MDT
Pressure Laplacian (d₁=157km, d₂=170km, ratio=1.08):
∇²p = [2/327] × [(1016.2−1006.8)/170 − (1006.8−988.5)/157]
= 0.006116 × (0.05529 − 0.11656)
= 0.006116 × (−0.06127) = −3.75 hPa/(100km)² ← strong mesohigh
5.5 What Each Algorithm Detects — Comparison Matrix
| Scenario | Bailey ∇²p + ∇²θ | CADINX_PA | Best Detector |
|---|---|---|---|
| Classical damming with clear mesohigh | ∇²p strongly − | Strongly − | Both fire; Bailey more specific |
| Shallow in-situ cold pool, flat pressure | Near zero | Weakly − | CADINX |
| Post-frontal cold advection, no trapping | Near zero | Weakly − | Neither — false positive risk |
| Warm-season damming, high moisture | May miss with dry θ | θᵥ captures it | CADINX with θᵥ |
| Strong damming with eroding pressure ridge | Weakens as ridge erodes | Still strongly − | CADINX more persistent |
| Valley cold pool (non-damming) | Near zero | Weakly − | Neither — requires screening |
6.1 Bailey's Six-Criteria System
Bailey requires all six criteria simultaneously satisfied for ≥ 6 consecutive hours. A single criterion failing at any timestep resets the event counter.
Criterion 1 — Pressure Laplacian Threshold
Must exceed 1 standard deviation below climatological mean
Typical σ ≈ 0.5–0.8 hPa/(100km)²
Part III scenario: Z_p ≈ −2.1 std deviations → very strong signal
Criterion 2 — Potential Temperature Laplacian Threshold
CPI must exceed 1 standard deviation above climatology
Part III scenario: Z_θ ≈ +2.5 std deviations → strong cold pool
Criterion 3 — Line D (SLP Gradient)
Part III scenario: SLP_PIT − SLP_ACY = 1021.0 − 1019.8 = +1.2 hPa ✓
Criterion 4 — Parent Anticyclone
A closed 1024+ hPa isobar must be identifiable within ~2000 km of the CAD region. The center must be positioned north or northeast of the CAD region. For automated implementation: mean SLP over the northern box (42°–50°N, 65°–85°W) > 1020 hPa.
Criterion 5 — 850 hPa Flow Direction
The 850 hPa wind at the nearest radiosonde site (BUF, PIT, or IAD for PA) must not be from the SW quadrant (225°–315°) with speed > 15 knots. Prevents flagging residual cold pools during active warm frontal passages.
Criterion 6 — Six-Hour Persistence
All five criteria above must be simultaneously satisfied for six consecutive hourly observations. A single-hour gap resets the event counter. This criterion excludes transient radiative cold pools, frontal passages, and data gaps. It is Bailey's most conservative filter.
6.2 CADEX's Two-Threshold System
CADEX is structurally simpler: CADINX > minimum threshold AND duration ≥ 3 hours. No parent anticyclone check. No 850 hPa wind check. No pressure Laplacian. The simplicity aids operational use but prevents mechanism classification.
6.3 Head-to-Head: March 15 PA CAD Event
Classic late-season PA CAD event, Ontario high at ~1026 hPa, 18Z conditions:
| Station | T (°C) | Td (°C) | SLP (hPa) | pₛ (hPa) | θᵥ (K) |
|---|---|---|---|---|---|
| PIT | 5.0 | −2.0 | 1026.0 | 982.4 | 280.8 |
| MRB | 0.0 | −1.0 | 1024.5 | 1004.9 | 272.8 |
| ACY | 9.0 | 4.0 | 1022.0 | 1019.7 | 281.7 |
| Algorithm | Key Metric | Value | Classification |
|---|---|---|---|
| Bailey | ∇²p = −1.88, CADINX_PA = −8.45 K, Line D = +4.0 hPa | All criteria met | MODERATE CDRY |
| CADEX | CADINX_PA = −8.45 K | Exceeds 5K threshold | MODERATE |
Both agree on intensity. But CADEX cannot distinguish this from flat-gradient cold advection producing the same θᵥ contrast. Bailey's ∇²p = −1.88 hPa/(100km)² confirms the mesohigh — only Bailey can make that distinction.
7.1 Bailey's Six-Type Taxonomy
Classification is applied after the detection algorithm confirms a CAD event is occurring. It is based on the parent anticyclone characteristics and synoptic flow pattern.
CDEN Classic Dense Cold Air Damming
Parent high: ≥ 1030 hPa, centered north or northeast (New England, Maritime Canada). Strong ∇²p (Z_p < −1.5) and strong CPI (Z_θ > +1.5). Northeasterly surface winds at MRB ≥ 10 kts. Duration ≥ 12 hours.
The deepest, most persistent CAD type. Cold pool typically 1500–3000 m deep. At MRB, surface temperatures may be 10–15°C below the 850 hPa temperature, indicating a strong inversion. Winter precipitation is typically freezing rain or ice pellets — overrunning warm moist air cannot penetrate the cold pool. Occurs 5–15 times per year in the Mid-Atlantic.
CDRY Classic Dry Cold Air Damming
Parent high: ≥ 1025 hPa, centered Ohio Valley or Great Lakes (west of Appalachians). Moderate ∇²p (−1.5 < Z_p < −1.0). Dew point depression at midslope station > 5°C.
Cold air spills eastward over the Appalachians rather than being fed from the north. Cold pool is shallower and drier than CDEN. Winter precipitation is more likely to be snow. More common in early and late winter (October, November, March).
HYBR Hybrid Cold Air Damming
Intermediate between CDEN and CDRY. Parent high moves from northwest to northeast during the event. θᵥ contrast moderate (CADINX_PA −3 to −7 K). Both Laplacians marginal. Most complex type — precipitation type (mixed ice, snow, freezing rain) is notoriously difficult to forecast. Events often begin as CDRY and evolve toward CDEN as the high moves northeast.
WKDR Weak Dry Cold Air Damming
Both Laplacians marginal (Z values −0.5 to −1.0). No well-defined parent anticyclone. Duration 6–12 hours. Often post-frontal. Cold pool is shallow (<500 m), mesohigh barely detectable. Surface temperatures at MDT only 2–4°C below 850 hPa temperature. Erodes quickly with daytime heating.
INST Instantaneous (In-Situ) Cold Air Damming
CADINX_PA criterion met, but ∇²p criterion not met (no detectable mesohigh). Duration ≥ 3 hours. No parent anticyclone required. Cold pool forms in place through radiative cooling, orographic drainage, or evaporative cooling. Common in Pennsylvania's river valleys (Susquehanna, Juniata, Cumberland Valley corridors) on calm, clear nights. This is what CADEX detects and Bailey misses.
UNKN Unknown / Unclassifiable
Meets detection criteria but cannot be unambiguously placed in Types 1–5. Typically assigned when parent anticyclone data is missing, Laplacian values are contradictory across the two ribs, or event duration is exactly at the persistence threshold.
7.2 CADEX's Three-Type Scheme
| CADEX Type | Bailey Equivalent | Key characteristic |
|---|---|---|
| Classic CAD | CDEN + CDRY | Identifiable parent anticyclone, sustained θᵥ gradient, ≥ 6 hours |
| Hybrid CAD | HYBR + WKDR | Moderate θᵥ gradient, transitioning pattern, 3–6 hours typical |
| In-Situ CAD | INST | No parent anticyclone, local terrain trapping only, ≥ 3 hours |
7.3 Where PA Events Most Commonly Fall
| Type | Frequency | Primary season | Meteorological impact |
|---|---|---|---|
| CDEN | 5–8% | Nov–Mar | Highest — freezing rain, ice storms |
| CDRY | 8–12% | Oct–Apr | High — snow, moderate icing |
| HYBR | 15–20% | Oct–Apr (shoulders) | Most uncertain — mixed precip types |
| WKDR | 20–25% | Year-round | Low — shallow pool, quick erosion |
| INST | 35–45% | Year-round, peak late summer–fall | Minor meteorologically; numerous |
| UNKN | 2–5% | Any | Data-limited; ambiguous |
8.1 Why Neither Algorithm Transfers Directly to PA
Click any station marker for details. Color zones show physiographic provinces relevant to CAD.
8.2 The PA-CADINX Algorithm: Complete Equation Set
For each rib (southern: PIT→MRB→ACY; northern: ERI→IPT→LGA) at each hour t:
eⱼ(t) = 6.1078 · exp[17.2694·Tᴅ,ⱼ / (Tᴅ,ⱼ + 237.29)]
0 otherwise
0 otherwise
Classical event: Σ[t−5 to t] F₂ⁱ = 6 (6-hr min)
8.3 Full Dual-Rib Worked Example
Warm-season analog scenario (Ontario high, 1026 hPa, June-type pattern, 06Z):
Adjust station observations on either rib and watch both CADINX_PA and ∇²p update in real time. The algorithm classifies each rib independently.
| Stn | T(°C) | Td(°C) | SLP |
| PIT | |||
| MRB | |||
| ACY |
| Stn | T(°C) | Td(°C) | SLP |
| ERI | |||
| IPT | |||
| LGA |
8.4 Threshold Calibration Strategy
| Variable | Likely PA threshold | Calibration source |
|---|---|---|
| ∇²p (PIT→MRB→ACY) | < −1.0 hPa/(100km)² | 90-yr MDT/CXY ASOS; ERA5 comparison |
| ∇²p (ERI→IPT→LGA) | < −0.8 hPa/(100km)² | 90-yr IPT ASOS (back to 1937) |
| CADINX_PA (both ribs) | < −3.0 K | Known event catalog; ROC optimization |
| Line D gradient | > +1.0 hPa SLP | Rarely violated during real events |
| Persistence (classical) | ≥ 6 hours | Fixed — from Bailey |
| Persistence (INST) | ≥ 3 hours | Fixed — from CADEX |
8.5 Final Comparison: Bailey vs. CADEX vs. PA-CADINX
| Property | Bailey (2003) | CADEX (2014) | PA-CADINX |
|---|---|---|---|
| Domain | TN–VA | NH White Mtns | PA Mid-Atlantic ✓ |
| Core thermal variable | Dry θ | Virtual θᵥ | Virtual θᵥ ✓ |
| Spatial operator | Laplacian (3-station) | First diff (2-station) | Laplacian (3-station) ✓ |
| Pressure check | Yes (∇²p + Line D) | No | Yes ✓ |
| Parent anticyclone | Required always | Not required | Required for classical; relaxed for INST ✓ |
| Persistence | 6 hours | 3 hours | 6 hr classical / 3 hr INST ✓ |
| Balance ratio correction | Not documented | N/A | Asymmetric Laplacian ✓ |
| In-situ detection | No (missed) | Yes (primary) | Yes — Stage 1 filter ✓ |
| Calibration dataset | 1950–1997 NC/VA | 2-yr NH record | 90-yr PA ASOS archive ✓ |
| Classification | 6 types | 3 types | 6 types (Bailey-compatible) ✓ |