Radio Hill Gazette

SARC 50th Anniversary: Celebrating 50 Years of Amateur Radio, Service, and Friendship

SARC 50th Anniversary: Celebrating 50 Years of Amateur Radio, Service, and Friendship

SARC celebrates 50 years of amateur radio, public service, and friendship.

The SARC 50th Anniversary marks a proud moment for the Schaumburg Amateur Radio Club. For five decades, SARC has brought people together through radio, learning, service, and friendship.[1]

Since the mid-1970s, SARC members have shared a simple goal: keep amateur radio active, useful, and welcoming. As a result, the club has grown into a strong local group with deep roots in Schaumburg and the surrounding area.[2]

A Milestone Worth Celebrating

A 50th anniversary does not happen by accident. Instead, it happens because members show up, teach others, try new things, and serve the community.

Over the years, SARC has helped people discover amateur radio. Also, the club has supported licensed operators who want to learn more, build more, and get on the air more often.[3]

Today, SARC continues that work through:

  • Weekly nets
  • Monthly meetings
  • License classes
  • Test sessions
  • Mentoring
  • Repeaters
  • Building projects
  • Outdoor operating
  • Public-service events
  • Emergency-readiness activities

Therefore, the SARC 50th Anniversary celebrates more than the past. It also celebrates the people who keep the club active today.

50 Years of Service to the Community

Amateur radio has always blended fun with purpose. SARC proves that point through steady public service.[4]

SARC members support local events and community activities. In addition, they give their time, skills, and equipment when clear communication matters.

The club’s public-service work has included support for events such as the Schaumburg Triathlon, the MS Walk, Septemberfest, and other area activities. Because of this work, SARC shows the value of amateur radio beyond the shack.[5]

Field Day: A Perfect Time to Celebrate

Field Day gives SARC a strong public stage. It welcomes visitors, introduces new people to ham radio, and lets members show what radio can do.[6]

This year, the SARC 50th Anniversary can add even more meaning to Field Day. For example, the club can use the milestone to welcome guests, thank members, and invite the public to learn more.

A few simple ideas can make the celebration stand out:

  • Share an anniversary cake after dinner
  • Display photos from past club events
  • Invite visitors to the Get On The Air station
  • Recognize longtime members
  • Promote SARC classes and test sessions
  • Share the club’s public-service story

Meanwhile, members can use the event to talk with guests about what makes SARC special.

Ways to Mark the SARC 50th Anniversary

A great anniversary celebration does not need to be complicated. However, it should feel visible, warm, and meaningful.

SARC can celebrate in several ways:

  • Request a Village of Schaumburg proclamation to honor the club’s 50 years.[7]
  • Operate a special event station to share the milestone on the air.[8]
  • Publish a Radio Hill Gazette anniversary edition with photos, stories, and memories.[9]
  • Create SARC 50th Anniversary shirts, hats, or badges for members and events.
  • Host a club history presentation with fun stories from longtime operators.
  • Scan and save historic photos, newsletters, and records for future members.[10]
  • Plan a fall SARC in the Park or build event to keep the celebration going.[11]

Together, these ideas can turn one milestone into a full year of connection.

Preserving the Story for the Next 50 Years

Every club has stories. However, those stories can fade when no one saves them.

Therefore, the SARC 50th Anniversary gives the club a great reason to protect its history. Members can gather old newsletters, photos, minutes, callbooks, Field Day records, and personal memories.

Then, SARC can scan and store those items in a club-controlled archive. As a result, future members will be able to see where the club started, how it grew, and who helped build it.[12]

This project can also support future website articles, meeting programs, and Radio Hill Gazette features.

A Celebration for Every Member

This anniversary belongs to everyone in SARC. It belongs to the founding members who helped start the club. It belongs to the longtime operators who kept it going. Also, it belongs to new members who will carry it forward.

Every member can take part. For example, members can:

  • Share a favorite SARC memory
  • Add old photos
  • Invite a friend to a meeting
  • Help at Field Day
  • Mentor a newer ham
  • Wear anniversary gear
  • Support public-service events

Most of all, members can keep doing what SARC has always done best: get on the air, help others, and make radio fun.

Looking Ahead

The SARC 50th Anniversary gives the club a chance to look back with pride. Yet it also points forward.

Amateur radio keeps changing. New tools, new modes, and new operators continue to shape the hobby. Still, the heart of SARC remains the same: people helping people connect.[13]

So, let’s celebrate 50 years of SARC with energy, gratitude, and purpose.

Then, let’s build the next 50 years together.

References

  1. “ARRL Clubs — Schaumburg Amateur Radio Club.” ARRL, The National Association for Amateur Radio. Accessed June 20, 2026. https://www.arrl.org/Groups/view/schaumburg-amateur-radio-club
  2. “Membership.” Schaumburg Amateur Radio Club. Accessed June 20, 2026. https://www.n9rjv.org/info/membership/
  3. “Activities.” Schaumburg Amateur Radio Club. Accessed June 20, 2026. https://www.n9rjv.org/activities/
  4. “47 CFR § 97.1 — Basis and purpose.” Electronic Code of Federal Regulations, Office of the Federal Register and National Archives and Records Administration. Accessed June 20, 2026. https://www.ecfr.gov/current/title-47/chapter-I/subchapter-D/part-97/subpart-A/section-97.1
  5. “Public Service.” Schaumburg Amateur Radio Club. Accessed June 20, 2026. https://www.n9rjv.org/activities/public-service/
  6. “Field Day.” ARRL, The National Association for Amateur Radio. Accessed June 20, 2026. https://www.arrl.org/field-day; “Field Day 2026.” Schaumburg Amateur Radio Club. Accessed June 20, 2026. https://www.n9rjv.org/field-day-2026/
  7. “Village Recognition.” Village of Schaumburg, Illinois. Accessed June 20, 2026. https://www.villageofschaumburg.com/i-want-to/request/village-recognition
  8. “Special Event Call Signs.” ARRL, The National Association for Amateur Radio. Accessed June 20, 2026. https://www.arrl.org/special-event-call-signs
  9. “Radio Hill Gazette.” Schaumburg Amateur Radio Club. Accessed June 20, 2026. https://www.n9rjv.org/category/news/rhg/
  10. “Digitization of Federal Records.” National Archives and Records Administration. Accessed June 20, 2026. https://www.archives.gov/records-mgmt/policy/digitization
  11. “Activities.” Schaumburg Amateur Radio Club. Accessed June 20, 2026. https://www.n9rjv.org/activities/
  12. “What are shared drives?” Google Workspace Learning Center. Accessed June 20, 2026. https://support.google.com/a/users/answer/7212025; “Digitization of Federal Records.” National Archives and Records Administration. Accessed June 20, 2026. https://www.archives.gov/records-mgmt/policy/digitization
  13. “47 CFR § 97.1 — Basis and purpose.” Electronic Code of Federal Regulations, Office of the Federal Register and National Archives and Records Administration. Accessed June 20, 2026. https://www.ecfr.gov/current/title-47/chapter-I/subchapter-D/part-97/subpart-A/section-97.1

Upgrade to a Extra Class License with our Class

The Schaumburg Amateur Radio Club offers a free upgrade class for those already holding a General or technician level license looking to upgrade to a LEVEL 3: Extra Class License Class beginning September 12, 2026.

This class is intended for those already holding their General-level license and who are looking to upgrade their privileges and bands that they can operate on to Extra class. This upgrade opens up all of the bands, including SSB (voice modes) for the operator.

This course is offered at no charge. The class is held from 09:30 a.m. to 11:30 p.m. on Saturdays from September 12 through December 14.

The class uses the American Radio Relay League Extra Class License Manual Fifth Edition as a study guide and students are encouraged to get their own copy.

Product Details
Spiral Bound: 416 pages
Publisher: The American Radio Relay League, Inc.
Copyright: Thirteenth Edition, First Printing (2024)
Language: English
ISBN: 978-1-62595-193-9

Register at: https://www.schaumburglibrary.org/Extra Class License

Location

RF Ground Conductor Comparison

40m – 70cm Ham Station RF

Executive summary

For the two candidates you specified, the 1.5 × 0.25 inch copper bar is the better RF ground conductor for a ham station bond or entry-panel ground path from 7 MHz through 430 MHz. Under a conservative model that treats your H02 bar as 100% IACS copper and treats “standard plumbing copper” as the common C12200 phosphorus-deoxidized plumbing tube at 85% IACS, the bar has about 1.9× lower calculated RF AC resistance per unit length than a representative 1/2-inch nominal plumbing tube across the entire 40 m–70 cm range. Its DC resistance is also far lower because it contains much more copper cross-section. The bar’s advantage comes mostly from geometry and alloy choice: it is wide and flat, so it presents more usable surface for RF current, and it is not penalized by the phosphorus used in plumbing copper.[1][4][17]

The subtle but important nuance is that the real electrical jump is not from C110 to C101. Official copper-alloy sources show that C10100 OFE is indeed purer than C11000 ETP, but the conductivity difference is small in practice: C10100 is specified at 101% IACS in the annealed condition, while C11000 has a minimum annealed conductivity of 100% IACS and a typical physical-property listing of about 101% IACS. By contrast, C12200 plumbing copper is about 85% IACS, so going from electrical copper to plumbing copper is the much bigger electrical downgrade. In other words, your flat bar beats plumbing tube mainly because it is flat and because plumbing alloy is worse, not because OFE is magically far better than ordinary electrical-grade copper.[1][3][4][5]

There is also a practical RF-grounding caveat: at HF/VHF/UHF, the few tens of milliohms of conductor resistance are usually less important than path impedance from length, bends, and routing. Motorola R56 explicitly says grounding conductors should be short, straight, smooth, and with as few bends as possible, and it explicitly prefers solid copper strap because it has lower inductance than large round wire conductors. So the bar is the better choice, but the biggest improvement still comes from topology: single-point bonding, short runs, gentle bends, and good connections.[15]

My bottom-line recommendation is therefore:

  • If you are choosing between these two exact candidates for station RF grounding, use the 1.5 × 0.25 inch copper bar.
  • If you are buying new material and cost matters, a flat C110 copper strap or bar is usually the best value compromise; true OFE/C101 is electrically excellent but usually unnecessary for a ham-station ground bond.

Scope and assumptions

This report treats “RF ground” as the station bonding/ground conductor used to connect radio equipment, an entry panel, or a house/external ground bar together, rather than as an antenna radial field or a tuned RF counterpoise. That distinction matters because for station bonding, conductor geometry and routing often control performance more than raw material purity. Motorola R56’s guidance for communication sites is a good fit for that use case: it calls for conductors that are short, straight, smooth, and it specifically prefers copper strap where reduced impedance is desired.[15]

Because the plumbing conductor was not fully specified, I used a representative and realistic assumption: 1/2-inch nominal copper water tube per ASTM B88, UNS C12200, with the standard plumbing outside diameter of 0.625 inch. For DC calculations, I show both Type L and Type M wall thicknesses from the Copper Tube Handbook. For RF AC calculations, Type L and Type M come out essentially the same because the first-order RF resistance depends mainly on outside diameter, not wall thickness, when current is confined to the outside skin. If your “approx. 1/2 inch diameter” copper is actually a solid 0.500 inch round rod instead of plumbing tube, it performs a bit worse at RF than the 0.625 inch OD tube assumption; that would only strengthen the case for the bar.[10][11][12]

All calculations below are at 20 °C, using the classical good-conductor skin-effect approximation with μr ≈ 1 for copper. For the bar, I used 100% IACS as the calculation basis because your exact commercial 101-H02 ASTM B187 product listing states 100% IACS; official C10100 datasheets list 101% IACS in the soft condition, and CDA notes that cold work can pull conductivity down by about 1 to 5 percentage points from annealed values. Using 101% instead of 100% would change the bar’s calculated RF resistance by only about 0.5%, which does not affect the recommendation.[1][6][17]

For the AC model, I used the classical skin-depth and surface-resistance relations for metals, then applied them to each conductor’s effective outside perimeter. NIST technical notes describe the standard metal skin-depth and surface-resistance relationships and note that surface resistance rises with frequency while skin depth falls. I ignored proximity effect and nearby-metal crowding in the base tables, so the tabulated RF resistances are best treated as first-order, lower-bound conductor values. In practice, mounting a conductor near other metal can increase its effective impedance.[13][14]

Material identity, standards, and conductivity

“RF ground” as the station bonding/ground conductor used to connect radio equipment

Your bar description — 99.99% OFE/OFHC copper, ASTM B187, H02 temper — lines up most closely with UNS C10100 OFE, not generic C10200 OF copper. Official alloy data show C10100 as 99.99% minimum Cu with 101% IACS conductivity in the soft condition; C10200 is the lower-purity oxygen-free grade at 99.95% minimum Cu and 100% IACS in the soft condition. Copper.org also notes that “OFHC” is historical trade language; formally, the common oxygen-free grades are OFE/C10100 and OF/C10200. So if the stock is truly 99.99%, that is a C10100/OFE-type product rather than ordinary C10200.[1][2][8]

Official sources also show why the C101 vs C110 discussion is often oversimplified. Copper.org’s C11000 alloy page gives 99.90% minimum Cu and says the alloy has a minimum annealed conductivity of 100% IACS; the same page’s physical-properties section lists 101% IACS as an actual property value. That means it is true that C10100 is purer than C11000, but it is not true that C10100 enjoys a dramatic conductivity lead over C11000 in ordinary room-temperature service. The difference is modest, and cold work can erase part of it. By contrast, plumbing alloy C12200 is listed at 85% IACS, which is a genuinely large step down.[3][4][5]

The plumbing side is much less ambiguous. Mueller Streamline, a primary U.S. tube manufacturer, states that its plumbing copper tube is made from UNS C12200 and manufactured to ASTM B88 for Type K, L, and M water tube. Copper.org’s C12200 alloy page lists 85% IACS, and the CDA engineering guide explicitly remarks that phosphorus-deoxidized copper can have about 99.9% copper content yet only 85% IACS, because phosphorus strongly depresses conductivity. That is the key reason ordinary plumbing copper is a poorer electrical conductor than electrical grades.[4][5][11]

The standards picture is therefore straightforward. ASTM B187/B187M is the governing specification family for copper bus bar, rod, and shapes for electrical applications; ASTM’s own scope summary says it covers copper conductor bars, rods, and shapes for electrical bus and general applications. Your specific commercial 101-H02 bar is sold as ASTM B187, and CDA’s ASTM B601 temper examples identify H02 as 1/2 hard. Typical plumbing copper is instead bought to ASTM B88 as C12200 water tube.[6][9][10][17]

The conductivity and alloy comparison that matters for your decision is summarized below. The values in the right-hand columns are the ones that matter most for electrical grounding work at room temperature.

Alloy Common name Cu purity / key chemistry Conductivity at 20 °C Resistivity basis
C10100 OFE 99.99% min Cu, O max 0.0005% 101% IACS in soft condition about 1.707 µΩ·cm
C10200 OF / OFHC-type 99.95% min Cu, O max 0.001% 100% IACS in soft condition 1.7241 µΩ·cm
C11000 ETP electrical copper 99.90% min Cu+Ag, oxygen-bearing minimum 100% IACS annealed; typical page value 101% IACS 1.7241 µΩ·cm nominal IACS basis
C12200 DHP plumbing copper phosphorus-deoxidized 85% IACS about 2.028 µΩ·cm

The temperature/temper story is also important but secondary. CDA’s copper property guide states that cold-worked tempers may run 1 to 5 percentage points below the annealed conductivity value, and gives annealed high-conductivity copper at 100–101.5% IACS versus 97% IACS for fully cold-worked material. The same guide gives the temperature coefficient of resistance for 100% IACS annealed copper as 0.00393/°C at 20 °C, so a copper ground conductor at 50 °C will have about 11.8% higher resistance than the same conductor at 20 °C. In practice, that means alloy choice matters more than H02 vs annealed, and routing matters more than either for RF grounding.[6][7]

RF calculations and comparison

For a good conductor at RF, current is confined to a very thin layer near the surface. Using the classical skin-effect approximation, skin depth is

δ = √(ρ / (π f μ)),

and surface resistance is

Rs = ρ / δ = √(π f μ ρ).

For an isolated long conductor whose outside dimensions are all much larger than δ, the first-order AC resistance per unit length is well approximated by R′ ≈ Rs / Peff, where Peff is the conductor perimeter that actually carries current. For the wide bar, I used the full outside perimeter 2(w+t); for the plumbing tube, I used the outer circumference πD. This is the correct comparison for a practical station bond where current is on the external conductor surface.[13][14]

The geometry is where the bar starts to pull ahead. The 1.5 × 0.25 in bar has a total outside perimeter of 3.5 in, while a representative 1/2-in nominal plumbing tube with 0.625 in OD has an outside circumference of only 1.963 in. So even if both were the same conductivity, the bar would already offer about 78% more RF-carrying perimeter. After you include alloy conductivity — 100% IACS for the H02 C101 bar basis versus 85% IACS for C12200 tube — the plumbing tube’s calculated RF resistance comes out about 1.93× higher than the bar’s across the whole 7–430 MHz span.[4][12][17]

The DC picture is even more one-sided. The bar’s metal cross-sectional area is 0.375 in². A representative 1/2-in Type L tube has only about 0.0735 in² of copper metal, and Type M only about 0.0525 in². That gives the bar a DC resistance of about 0.071 mΩ/m, compared with 0.428 mΩ/m for Type L and 0.599 mΩ/m for Type M. DC resistance matters most for fault/equalization currents and lightning-energy distribution; RF resistance matters more for RF current on the bond itself. In both regimes, the bar wins.[12]

The table below gives the geometry and DC resistance basis. The RF tables that follow use the Type L/M outside diameter of 0.625 in for the plumbing conductor, because that is what controls first-order RF resistance. Sources for dimensions and conductivity are cited in the note beneath the table; the arithmetic itself is mine.

Candidate Assumed form Key dimensions Effective outside perimeter Copper metal area DC resistance
OFE bar Solid rectangular bar 1.5 in × 0.25 in 3.500 in 0.3750 in² 0.0713 mΩ/m
Plumbing copper Type L Round tube 0.625 in OD, 0.545 in ID 1.963 in 0.0735 in² 0.4277 mΩ/m
Plumbing copper Type M Round tube 0.625 in OD, 0.569 in ID 1.963 in 0.0525 in² 0.5987 mΩ/m
Round 0.500 in solid reference Solid round 0.500 in OD 1.571 in 0.1963 in² 0.1601 mΩ/m

Now the RF results. The copper skin depth is only a few tens of micrometers at HF and only a few micrometers by 430 MHz, so both conductors are very much in the skin-effect regime. At 7 MHz, the calculated skin depth is about 25.0 µm for the bar’s 100% IACS copper basis and 27.1 µm for C12200; by 430 MHz it falls to about 3.19 µm and 3.46 µm, respectively. These depths are tiny compared with either conductor’s macroscopic dimensions, which is why outside perimeter is the controlling geometric term.

Frequency Skin depth in bar copper Skin depth in plumbing copper AC resistance of bar AC resistance of plumbing tube Plumbing/bar ratio
7 MHz 24.98 µm 27.09 µm 7.764 mΩ/m 15.012 mΩ/m 1.93×
14 MHz 17.66 µm 19.16 µm 10.981 mΩ/m 21.230 mΩ/m 1.93×
28 MHz 12.49 µm 13.55 µm 15.529 mΩ/m 30.024 mΩ/m 1.93×
50 MHz 9.35 µm 10.14 µm 20.751 mΩ/m 40.122 mΩ/m 1.93×
144 MHz 5.51 µm 5.97 µm 35.216 mΩ/m 68.089 mΩ/m 1.93×
430 MHz 3.19 µm 3.46 µm 60.855 mΩ/m 117.660 mΩ/m 1.93×

A practical way to read that table is by multiplying by your actual run length. For a 10-foot bond run, the bar’s conductor resistance is about 23.7 mΩ at 7 MHz and 0.185 Ω at 430 MHz; the plumbing tube would be about 45.8 mΩ at 7 MHz and 0.359 Ω at 430 MHz. Those are not huge absolute numbers, which is why it is so important not to over-focus on copper purity alone. The routing and inductive behavior of the bond usually matter more, and that is exactly why wide, flat conductors are preferred in communication-site grounding practice.[15]

One subtle caveat is worth stating explicitly. The bar’s RF-resistance advantage assumes it is installed so its outside surfaces are actually participating in the current flow. If you bolt the bar tightly, face-to-face, against a large conductive sheet or wall plate, one broad face may contribute less to current carrying than in the isolated-conductor model, so the pure “surface resistance” advantage shrinks. Even then, the bar generally remains preferable because it still gives a better low-inductance path and better bonding geometry. That is an inference from the field distribution and the installation geometry, not a direct catalog specification.

Mechanical and installation factors

Ground Conductor Comparison 40m – 70cm Ham Station RF

Mechanically, the copper bar is better suited to a ground bus / station bond role. A rigid flat bar is easy to drill, easy to bolt with two-hole lugs, easy to standoff from a wall or entry panel, and easy to use as a real bus bar that multiple chassis and surge protectors can land on. R56 repeatedly shows this style of layout: an external ground bus bar at the cable entry point, bonded by solid copper strap to the grounding electrode system, with a corresponding interior master bus bar. That is much harder to do cleanly with a piece of round plumbing tube unless you start improvising pipe clamps, flattened ends, or custom saddles.[15]

flowchart LR
    A[Antenna feedlines] --> B[Outside entry ground bar]
    B --> C[Coax surge protectors / cable bonds]
    C --> D[Short wide copper strap or bar]
    D --> E[Ground ring or rods]
    B --> F[Through-wall bond]
    F --> G[Inside master ground bar]
    G --> H[Transceiver]
    G --> I[Tuner / amp / PSU]
Show code
flowchart LR
    A[Antenna feedlines] --> B[Outside entry ground bar]
    B --> C[Coax surge protectors / cable bonds]
    C --> D[Short wide copper strap or bar]
    D --> E[Ground ring or rods]
    B --> F[Through-wall bond]
    F --> G[Inside master ground bar]
    G --> H[Transceiver]
    G --> I[Tuner / amp / PSU]

That topology is not just neat; it matches communication-site practice. R56 says the external ground bar should be at the cable-entry point, should connect directly to the grounding electrode system, and may be connected with solid copper strap because even relatively small strap has significantly less inductance than large wire conductors. It also says the RF transmission-line entry point and ground bar should be installed as low to the ground as practical.[15]

On corrosion and surface condition, both candidate materials are fundamentally good copper alloys with excellent corrosion resistance in ordinary indoor/outdoor service, and C12200’s plumbing heritage is obviously built around that. Aurubis lists excellent corrosion resistance for oxygen-free coppers, and Copper.org lists corrosion resistance among the characteristic reasons C11000 and C12200 are widely used. The bigger real-world hazard is not the bulk alloy but joint quality and dissimilar-metal interfaces. R56 requires removal of paint, enamel, lacquer, and other nonconductive coatings at bonding surfaces, and it warns to use correct methods where dissimilar metals are involved.[3][4][15][16]

On joining methods, the broad engineering lesson is simple: grounding joints should be mechanical/compression/exothermic, not casual solder-only assemblies. R56 prefers exothermic welds, listed irreversible compression connectors, and listed compression two-hole lugs for grounding and bus connections. That strongly favors the flat bar in practice because it naturally accepts bolted lugs and bus-bar hardware. Plumbing copper, by contrast, is optimized for soldered, brazed, or press plumbing joints; Copper.org rates C12200 soldering and brazing as excellent, which is great for plumbing, but it does not make round tube the preferable ham-shack ground bus material.[4][15]

On flexibility, the story splits by temper. Straight stick plumbing tube is often sold in hard temper, while soft Type L coil is sold precisely because it is flexible and easy to snake through a building. That is useful in plumbing but not ideal for RF bonding, because extra curves and bends raise impedance; R56 explicitly warns against sharp bends and says grounding conductors should be run short, straight, and smoothly. Your H02 bar is stiffer than soft copper, which is actually an advantage for maintaining a disciplined routing geometry.[15]

Finally, on surface finish, NIST notes that copper surface roughness has relatively small effect at low frequency and becomes noticeably worse above about 1 GHz. Since your highest band here is 430 MHz, ordinary mill finish or light tarnish on the conductor body is usually not the main issue. The important surface-related problem at amateur frequencies is usually contact resistance at joints, not the conductor’s broad-side finish. Clean, bright metal and high-pressure bolted/compression joints matter more than polishing the entire conductor.[14]

Cost and availability tradeoffs

This is the one category where plumbing copper wins decisively. Current retail/distributor pages show that 1/4 × 1-1/2 in C101 oxygen-free H02 bar is a specialty metal product sold in cut lengths, with a representative price of $35 for 1 ft and $382.54 for 12 ft from an OnlineMetals/Southern Copper listing. By contrast, commodity plumbing copper is stocked at home centers: a representative 1/2 in × 10 ft Type L pipe was about $40.71 or $4.07/ft, a 1/2 in × 10 ft soft Type L coil about $39.62 or $3.96/ft, and Type M around $29.96 or $3.00/ft. So on a small-buy basis, the OFE bar is roughly 8× to 12× more expensive per foot than plumbing copper.[17][18][19]

Availability follows the same pattern. Plumbing copper is a commodity: you can often buy it the same day at a plumbing or home-improvement store. The OFE bar is a specialty electrical/metals item: it is available, but usually by mail order or metals distributor rather than from a local shelf. For many ham projects, that availability difference matters more than the raw metal cost.

There is also an important “best value” observation. If your real goal is simply the best practical station grounding conductor, flat electrical-grade copper is the sweet spot. A representative 1/4 × 1-1/2 in C110-H02 bar is also stocked to ASTM B187, but with electrical conductivity listed at 100% IACS and small-quantity pricing of about $47.33 for 1 ft and $343.12 for 12 ft in one current listing. Official copper-alloy data show that C110’s electrical performance is extremely close to C101 in room-temperature service. So if you want the geometry advantage of a bar/strap without paying a premium for oxygen-free copper, C110 flat copper is usually the logical choice.[3][20]

Recommendation and practical installation tips

For the specific comparison you asked for, the recommendation is clear: the 1.5 × 0.25 inch copper bar will work better than standard 1/2-inch-class plumbing copper as an RF ground conductor for a 40 m through 70 cm ham station. It has lower DC resistance, roughly half the calculated RF AC resistance of representative plumbing tube, lower-inductance geometry in actual grounding practice, and far better mechanical suitability as a real bus or bond conductor.

The most important caveat is that the bar’s biggest advantage is not that it is OFE. If you replaced the bar with a flat C110 electrical copper bar or strap of the same size, you would keep almost all of the practical grounding benefit, because the difference between C101 and C110 is small, while the difference between flat bar and plumbing C12200 tube is large. So if you already own the OFE bar, use it. If you are buying from scratch, flat copper bar or strap is the right form factor, and C110 is usually the better value buy unless you have a special reason to insist on oxygen-free stock.

If you only have plumbing copper on hand, it is still perfectly possible to make an acceptable station bond with it — especially for a very short run — but it becomes the second-best option as the run gets longer, the bands get higher, and the routing gets bendier. The penalty is not that it will “fail” as a ground conductor; it is that its alloy and geometry are both less favorable, so it gives you less performance margin.

Practical installation tips follow directly from the standards and the calculations:

  • Use a single-point ground / entry bar arrangement, with the feedline entry bonded immediately to an external ground bar and then to the grounding-electrode system.
  • Keep the conductor as short, straight, and smooth as possible. Avoid loops, sharp 90° kinks, and decorative routing. R56 calls for the fewest bends possible and gives an 8-inch minimum bend radius guidance.
  • Prefer a wide flat bar or strap over round conductors for the main bond path. R56 specifically says solid copper strap gives lower inductive impedance than large wire conductors.
  • Use bolted compression lugs, irreversible compression connectors, or exothermic welds for the grounding path. Do not rely on casual solder-only joints for the primary bond.
  • Clean joint surfaces to bright metal. Remove paint, enamel, lacquer, and other nonconductive coatings before bonding.
  • If copper meets galvanized steel, aluminum, or other dissimilar metals, use proper bimetallic hardware/practice and protect the finished joint from corrosion.
  • If the bar is mounted near other metal, consider standoffs so the conductor remains a real strap/bar rather than becoming a face-clamped plate with reduced useful surface. This is an engineering best practice inferred from the current-distribution model.

Open questions and limitations

The main open-ended element in your prompt is the plumbing conductor itself. “Standard plumbing copper” could mean Type L or Type M, hard straight pipe or soft coil, and possibly even a scrap round rod rather than actual water tube. I treated the most likely case — 1/2-inch nominal ASTM B88 C12200 tube with 0.625 inch OD — and showed why the conclusion is robust even if your exact specimen varies. If your actual round copper is larger in OD than that, its RF result improves somewhat; if it is smaller, it gets worse.

The RF resistance values are also first-order conductor-only calculations. They deliberately do not include proximity effect, nearby metal surfaces, or the complete loop/return inductance of your station grounding network. In practice, those topology issues often dominate, which is why the installation guidance in the recommendation section is every bit as important as the material choice itself.

References

  1. C10100 Alloy. Copper Development Association / Copper.org. Accessed June 14, 2026. https://alloys.copper.org/alloy/C10100.
  2. C10200 Alloy. Copper Development Association / Copper.org. Accessed June 14, 2026. https://alloys.copper.org/alloy/C10200.
  3. C11000 Alloy. Copper Development Association / Copper.org. Accessed June 14, 2026. https://alloys.copper.org/alloy/C11000.
  4. C12200 Alloy. Copper Development Association / Copper.org. Accessed June 14, 2026. https://alloys.copper.org/alloy/C12200.
  5. Industrial: Design Guide — Conductivity of Alloy Classes. Copper Development Association / Copper.org. Accessed June 14, 2026. https://copper.org/applications/industrial/DesignGuide/selection/conductalloy02.php.
  6. A Guide to Working With Copper and Copper Alloys. Copper Development Association. Accessed June 14, 2026. https://www.copper.org/publications/pub_list/pdf/a1360.pdf.
  7. Introduction to Copper: Fact Sheets. Copper Development Association / Copper.org. Accessed June 14, 2026. https://www.copper.org/publications/newsletters/innovations/2001/08/intro_fac.html.
  8. Introduction to Copper: Types of Copper. Copper Development Association / Copper.org. Accessed June 14, 2026. https://www.copper.org/publications/newsletters/innovations/2001/08/intro_toc.html.
  9. Standard Specification for Copper, Bus Bar, Rod, and Shapes and General Purpose Rod, Bar, and Shapes (ASTM B187/B187M-20). ASTM International. Accessed June 14, 2026. https://store.astm.org/b0187_b0187m-20.html.
  10. B88 Standard Specification for Seamless Copper Water Tube. ASTM International. Accessed June 14, 2026. https://www.astm.org/b0088-20.html.
  11. Plumbing Copper Tube. Mueller Streamline. Accessed June 14, 2026. https://muellerstreamline.com/products/copper-tube/plumbing-copper-tube/.
  12. Copper Tube Handbook. Copper Development Association. Accessed June 14, 2026. https://www.copper.org/publications/pub_list/pdf/copper_tube_handbook.pdf.
  13. NBS/NIST Technical Note 1532: Relative Permeability Measurements for Metal-Detector Research. National Institute of Standards and Technology. Accessed June 14, 2026. https://nvlpubs.nist.gov/nistpubs/Legacy/TN/nbstechnicalnote1532.pdf.
  14. NIST Technical Note 1520: Dielectric and Conductor-Loss Characterization and Measurements on Electronic Packaging Materials. National Institute of Standards and Technology. Accessed June 14, 2026. https://nvlpubs.nist.gov/nistpubs/Legacy/TN/nbstechnicalnote1520.pdf.
  15. Standards and Guidelines for Communication Sites (R56), 68P81089E50-B. Motorola, Inc.; PDF copy hosted by the U.S. Bureau of Land Management. Accessed June 14, 2026. https://www.blm.gov/sites/blm.gov/files/Lands_ROW_Motorola_R56_2005_manual.pdf.
  16. C10100 / Cu-OFE Data Sheet. Aurubis. Accessed June 14, 2026. https://www.aurubis.com/en/dam/jcr%3A6969eb67-ba93-4da2-b140-0a0019af908e/c10100-cu-ofe-us.pdf.
  17. 0.25 in. × 1.5 in. Oxygen Free Copper Rectangle Bar 101-H02. OnlineMetals.com / Southern Copper. Accessed June 14, 2026. https://www.onlinemetals.com/en/buy/copper/0-25-x-1-5-oxygen-free-copper-rectangle-bar-101-h02/pid/mp-00005335.
  18. 1/2 in. × 10 ft. Type L Soft Copper Coil Tubing. The Home Depot. Accessed June 14, 2026. https://www.homedepot.com/p/Everbilt-1-2-in-x-10-ft-Type-L-Soft-Copper-Coil-Tubing-1-2-L-10RE/203654558.
  19. Copper Pipe Listings: 1/2 in. × 10 ft Type M Hard Temper Straight Pipe and 1/2 in. × 10 ft Type L Pipe. The Home Depot. Accessed June 14, 2026. https://www.homedepot.com/b/Plumbing-Pipe-Fittings-Pipe-Copper-Pipe/N-5yc1vZ1z18i44.
  20. 0.25 in. × 1.5 in. Copper Rectangle Bar 110-H02. OnlineMetals.com. Accessed June 14, 2026. https://www.onlinemetals.com/en/buy/copper/0-25-x-1-5-copper-rectangle-bar-110-h02/pid/4286.

Midwest (East-North) Ground-System Performance

Maidenhead EN Ham Radio Performance

Executive summary

We define “EN” as the eastern-northern portion of the Midwest, this report treats it as an operationally defined Great Lakes / eastern-northern Midwest subregion.
For early June 2026, the official space-weather picture is usable but variable rather than quiet-stable. NOAA SWPC’s June 4 forecast expected low-to-moderate solar activity, with chances for R1–R2 radio blackouts from active regions, and active to G1 geomagnetic conditions with a minor chance of stronger disturbance. SWPC defines R1 as weak/minor HF degradation on the sunlit side. The smoothed June 2026 solar-cycle forecast also remained elevated, with a predicted sunspot number near 101.3 and F10.7 near 126.3, which is still favorable for daytime F-region support on 20–10 meters compared with solar-minimum years.

For the Midwest EN region, that translates into a practical HF pattern of stronger daytime potential on 20/17/15 meters, intermittent but still meaningful opportunities on 12/10 meters, and less stable 40/80-meter daytime performance whenever D-layer absorption is elevated. After sunset, the D layer weakens, so 40 and 80 meters typically become the more reliable regional/interregional bands, while 20 meters often stays usable later into the evening in summer. This seasonal/diurnal pattern is an inference from NOAA’s D-region absorption product, ionospheric reflection physics, and current Cycle 25 flux levels.

On 2 m / 70 cm / 23 cm, ordinary range remains mostly line-of-sight plus scatter, but the Great Lakes and adjacent flat terrain can produce useful tropospheric enhancement when high pressure, subsidence inversions, nocturnal cooling, and lake/land temperature contrasts align. A long-running engineering summary of William Hepburn’s tropo maps notes that ducting is more common in the Midwest, Great Lakes, and Northeast in fall, though early-summer overnight lake-path enhancements still occur under stable air. NOAA and NWS sources also show why: the Great Lakes cool nearby summer air, generate lake-breeze circulations, and help support shallow stable layers along lake paths.

The soil side of the problem is at least as important as the sky side for verticals and ground-mounted antennas. USDA/NASS data for the week ending May 31, 2026 showed that parts of the eastern-northern Midwest were drying quickly even without widespread formal drought: Illinois topsoil in the “very short + short” categories was 33%, Michigan 28%, Minnesota 35%, and Wisconsin 34%, while Ohio was still only 1% and Indiana 15%. CPC’s June outlook simultaneously favored subnormal precipitation across the Great Lakes and adjacent areas, and CPC’s hazards outlook flagged rapid-onset drought possible for parts of the Upper/Middle Mississippi Valley, Ohio Valley, and Great Lakes region.

That matters because soil moisture is a major control on ground conductivity and permittivity. ITU-R states that moisture content is the major factor in ground electrical properties, and gives a striking order-of-magnitude example: loam that is normally around 10⁻² S/m can dry to about 10⁻⁴ S/m, roughly the conductivity of granite. USDA/NRCS similarly notes that wetter soils conduct better, and soil-science literature models bulk soil conductivity as a function of both volumetric water content and the conductivity of the soil solution. In other words, seasonal drying can create a several-fold to ~100× conductivity penalty depending on texture, salts, and moisture history.

For operators, the most actionable finding is this: do not expect a ground rod to replace radials. ARRL explicitly states that a ground rod is useful for safety/lightning functions, but its RF resistance is high; a quarter-wave vertical needs a low-RF-resistance return path, which is what radial wires supply. In N6LF’s classic QEX measurements, 64 radials on the ground improved signal by about +5.8 dB relative to a sparse 4-radial baseline, while 4 elevated radials at about 48 inches produced about +5.9 dB, essentially matching the 64-radial on-ground case on 40 meters. Conversely, he described a 4-radial on-ground system as an emergency measure.

The practical implication for the Midwest EN region during dry spells is straightforward: if your vertical suddenly “still tunes, but gets out worse,” suspect ground loss before blaming the rig. The most effective mitigations are to add radials, especially in the first fraction of a wavelength from the base; consider resonant elevated radials if you cannot lay many ground radials; use an antenna analyzer to track the feedpoint resistance/reactance shift rather than relying only on shack SWR; and, for safety/lightning, test the grounding electrode separately with a ground-resistance tester using methods aligned with IEEE 81, recognizing that this does not measure RF radial performance.

Scope and assumptions

For this report, “Midwest EN” is treated as the eastern-northern Midwest / Great Lakes arc, with emphasis on Wisconsin, Michigan, Illinois, Indiana, Ohio, and adjacent upper-Midwest contexts such as Minnesota when regional soil-moisture or propagation patterns matter. That is a practical definition, not a formal one. The overlap with the Maidenhead EN field is worth noting because PSKReporter and VHF/UHF operators often think in grid fields, but I have not assumed your “EN” means only the grid field.

A second assumption is methodological: for “current” propagation, I prioritize official SWPC/CPC/USDA products and current measurement networks over anecdotal on-air reports. PSKReporter and WSPRnet are therefore treated as observational networks, not as deterministic forecasts; NOAA SWPC and CPC products are treated as the official baseline for space weather and drought/soil-moisture outlooks.

Propagation across the Midwest EN region

HF behavior

Cross-section diagram of the ionosphere over the Midwest showing F-region ionization supporting 20–10 m bands, thick D-layer absorption affecting lower HF, and the sunset transition where 40/80 m signals recover. Labels include solar EUV, R1–R2 blackouts, and geomagnetic Kp.
The official June 4 SWPC forecast called for low-to-moderate solar activity, with chances for M-class flares and R1–R2 radio blackouts, while geomagnetic conditions were expected to be elevated to G1 with a minor chance of stronger disturbance. SWPC’s definitions matter here: R1 already implies weak/minor HF degradation on the sunlit side, and Kp-driven geomagnetic disturbance affects users of radio signals reflected by or passing through the ionosphere.

For Midwest EN operators, the practical pattern is therefore a two-track HF day. On the one hand, the still-elevated Cycle 25 background supports daytime 20/17/15 m very well and keeps 12/10 m genuinely worth checking, especially around local late morning through mid-afternoon. On the other hand, any R1–R2 intervals and elevated D-region absorption will most obviously punish 40/30/20 m sunlit paths at the lower end of HF, with the strongest daytime degradation usually on the lower HF bands. This is an inference from SWPC’s D-RAP absorption model and ionosonde reflection physics combined with the current smoothed sunspot/F10.7 forecast.

The seasonal pattern in early summer is classic midlatitude behavior. Longer daylight and stronger solar illumination raise daytime ionization, which helps the upper HF bands, but they also raise D-layer absorption, which is why 40 and 80 meters can feel “dead” by day and then recover sharply after sunset. In winter, the balance shifts: daytime absorption is lower, so 80 and even 160 meters improve materially, while summer still favors the upper bands more often. The spring and fall transition seasons often bring the best all-around balance between low daytime absorption and still-healthy F-region support. The seasonal summary here is a first-principles inference from the official D-layer and ionospheric references rather than a single Midwest-specific climatology product.

A useful mental model for the region is:

HF propagation drivers in the Midwest EN region (early June 2026)

Solar flux & EUV
→ F-region ionization
Flares & proton events
→ R1–R2 blackouts
D-region absorption
→ 40/30/20 m daytime fading
Geomagnetic disturbance
→ Erratic path quality
Sunset + overnight cooling
→ D-layer decay → 40/80 m recovery
Result
Strong 20–10 m daytime openings
Variable lower-HF sunlit paths

This diagram summarizes SWPC’s official HF-degradation and ionospheric mechanisms and the diurnal transition most relevant to Midwest operators.

VHF and UHF behavior

Tropospheric Ducting over the Great Lakes – VHF/UHF Enhancement Mechanism
For 2 m, 70 cm, and 23 cm, most ordinary Midwest EN operating remains local or regional LOS/scatter, but VHF/UHF enhancement becomes dramatically better when the lower troposphere forms refractive ducts or strong super-refraction layers. NTIA’s classic ducting review explains that atmospheric stratification can strongly alter service and interference fields, while the NAB summary of Hepburn’s maps explains the practical recipe: warm, dry air overriding cooler, moister air produces the vertical refractive gradients that favor VHF/UHF bending and ducting.

For the Great Lakes slice of the Midwest EN region, lake physics help. NOAA-reviewed Great Lakes climatology notes that the lakes moderate temperatures, cool nearby summers, and warm nearby winters, and NWS defines the lake breeze as a thermally produced circulation from the lake toward shore caused by differential heating. Alongshore and cross-lake paths therefore get exactly the kind of shallow stable layers and inversion boundaries that can support overnight or morning tropo enhancement, especially when a synoptic high settles in and winds stay light.

The important seasonal nuance is that the Midwest/Great Lakes are not at peak tropo season in early June. The Hepburn/NAB climatological note says the fall is more favorable for the Midwest, Great Lakes, and Northeast. So the rigorous way to say it is: local VHF/UHF ducting risk is present in early summer but not climatologically maximal; expect the best odds on overnight to early-morning lake paths and during stable high-pressure episodes, with a stronger regional tendency later in summer into fall.

Observation sources and recent maps

The most useful official HF nowcasting product is NOAA SWPC’s D-Region Absorption Predictions, which SWPC explicitly describes as guidance for understanding HF radio degradation and blackouts. SWPC’s broader product suite also includes Planetary K-index, GloTEC, and WAM-IPE links, which are the right official context layers when you want to decide whether a bad day is caused mainly by absorption, geomagnetic disturbance, or background electron-content structure.

For actual on-air observation, PSKReporter is the fastest practical lens into what the bands are really doing. PSKReporter says its purpose is to automatically gather digimode reception records and make them available in near real time. Its public MQTT mirror also makes clear that spots can be filtered by band, mode, callsign, grid square, or field, which is why it is especially useful for a Midwest EN operator trying to separate “the band is shut” from “my station is underperforming.”

WSPRnet fills a slightly different niche. Its own site presents a Map, Activity, and Database, and publishes frequency coverage from LF through microwave, including 144 MHz, 432 MHz, and 1296 MHz. Because WSPR transmissions are structured for weak-signal propagation reporting, WSPRnet is excellent for night-to-night A/B comparisons of antenna changes, radial additions, drying-soil effects, and sunset/sunrise behavior, especially if you hold power, band, and schedule constant.

For planned-path work rather than nowcasting, VOACAP Online remains a standard planning tool, while real-time ionosonde-based tools such as KC2G’s MUF map are useful secondary references. These are not substitutes for local observation, but they are good for answering, “Should 15 m exist at all right now?” before you diagnose your station.

For VHF/UHF, the two practical maps are different in purpose. Hepburn’s tropo forecast is a forecast of refractive potential; VHF DX View is a real-time observation layer based on APRS-IS paths and highlights unusually long 144 MHz behaviors. Used together, they let you distinguish “forecast improvement” from actual enhancement already in progress.

Soil moisture, drought, and what that means for conductivity

Rapid Surface Drying in the Eastern-Northern Midwest – May 31, 2026 USDA/NASS Topsoil Moisture
The current broad drought picture is mixed, not uniformly severe. The U.S. Drought Monitor notes that drought categories run from D0 through D4, while CPC’s June 2026 Midwest discussion said that, outside Kentucky and adjacent southeastern Missouri, there was very little drought elsewhere in the Midwest, limited mainly to north-central Minnesota and some western fringes. At the same time, CPC’s June outlook favored subnormal precipitation across the Great Lakes and adjacent areas, and the weekly hazards outlook flagged rapid-onset drought possible for parts of the Upper/Middle Mississippi Valley, Ohio Valley, and Great Lakes region.

That broad-scale picture can hide rapid surface drying, which is what RF ground systems care about first. USDA/NASS weekly topsoil data for the week ending May 31, 2026 showed that some eastern-northern Midwest states had already dried markedly at the surface despite not being in major regional drought.

State May 17 very short + short May 24 very short + short May 31 very short + short Practical read
Illinois 17% 16% 33% Clear late-May drying
Indiana 16% 11% 15% Near-steady to slightly dry
Michigan 16% 14% 28% Noticeable drying
Minnesota 39% 32% 35% Persistently drier than neighbors
Ohio 12% 1% 1% Surface stayed moist
Wisconsin 14% 17% 34% Clear late-May drying

*Derived from USDA/NASS “Topsoil Moisture Condition – Selected States” for the weeks ending May 17, May 24, and May 31, 2026. The table uses “very short + short” as a practical dryness indicator for RF-ground behavior.

The reason this matters electrically is direct and large. FCC’s ground-wave references say U.S. ground conductivities typically span roughly 0.1 to 30 mS/m. ITU-R P.527/P.527-5 says moisture is the major factor controlling soil permittivity and conductivity and gives a useful order-of-magnitude example: loam may normally be around 10⁻² S/m, but when dried can fall to about 10⁻⁴ S/m. USDA/NRCS says the same thing in plainer language: wetter soil conducts better.

An illustrative engineering view looks like this:

Illustrative soil conductivity vs. relative wetness

Very dry Dry Moderate Moist Wet

10 9 8 7 6 5 4 3 2 1 0

Bulk conductivity, mS/m

(Order-of-magnitude synthesis from ITU, FCC, USDA/NRCS, and soil-EC literature)

This is not a site calibration; it is an order-of-magnitude synthesis from ITU, FCC, USDA/NRCS, and soil-EC literature showing the direction and approximate scale of change that can occur as moisture rises. Texture, salts, organic matter, and compaction can move a real site far above or below these points.

Grounding, radials, and the physics behind performance changes

Ground-Loss Comparison: 4 Radials vs. Dense Radial System – Impact on Antenna Performance
ARRL’s grounding guidance is unusually clear on the central distinction: safety ground, lightning ground, and RF ground are not the same thing. A quarter-wave vertical needs an RF return path with low RF resistance; a ground rod helps only a little at RF and remains a high-RF-resistance connection compared with a proper radial system. ARRL’s verticals primer adds the other half of the picture: the vertical is effectively a dipole with half its structure “mirrored” in the counterpoise or ground system, and poor ground conductivity makes the classic joke true that a bad vertical “radiates equally poorly in all directions.”

In circuit terms, the important quantity is radiation efficiency:

η ≈ R_rad / (R_rad + R_loss)

ARRL’s modeling tutorial states this explicitly, and for short verticals the implication is severe: if the antenna’s radiation resistance is already low, then a few extra ohms of ground loss become a large fraction of the total input resistance. That is why short, loaded, or low-band verticals are much more sensitive to soil and radial quality than a better-behaved half-wave structure.

The near field around the base is where the damage happens. N6LF notes that most ground loss is concentrated within about half a wavelength of the base of the vertical. That does not mean every radial must be half a wavelength long; it means the first portion of the return-current region is the most valuable place to reduce loss. It is also why adding more modest-length radials near the base is often more productive than trying to install just a few very long wires.

Drying soil affects both loss and tuning. ITU says moisture changes both conductivity and permittivity. In N6LF’s elevated-radial analysis, the radial length needed for resonance at 3.65 MHz changed with soil characteristics, and a low dipole at 8 ft could resonate anywhere from roughly 64.5 to 66.4 ft depending on soil. In his 2009 measurements, he also noted that small changes in the system could vary with soil moisture and that observed measurements were run after periods of rain and after later drainage/drying. So a drying site can do three things at once: raise ground loss, shift resonance, and change feed impedance.

The most useful experimental ham evidence in the source set comes from N6LF’s QEX work on 40 m. With 33-foot radials on the ground, going from 4 to 8 to 16 to 32 radials improved field strength by roughly +2.26 dB, +3.76 dB, and +4.16 dB relative to the 4-radial baseline; he explicitly described the 4-radial case as “really flaky” and suitable only as an emergency measure. Separately, his Part 3 measurements found 64 radials on the ground at about +5.8 dB over the 4-radial ground baseline, while 4 elevated radials at 48 inches produced about +5.9 dB, which is effectively the same result for practical purposes.

That experimental result is the cleanest answer to the buried-vs-elevated question: many on-ground radials work, and a small number of properly resonant elevated radials can work just as well, especially where space is limited. But there is a catch. N6LF’s later elevated-radial analysis showed that with only a few radials, making them “too long” relative to the optimum can create a deep gain notch, even on the order of several dB, and can move the takeoff angle upward. In other words, sparse elevated radials must be treated as resonant antenna elements, not just “some wires that look about right.”

ARRL and secondary ARRL-hosted references in the source set also support several practical corollaries: surface or shallow-buried radials are preferred for ground-mounted verticals; poor soil requires more elevated-radial height for the same performance; and ground rods do not replace radials for RF return current.

Practical station guidance for Midwest EN operators

Practical Antenna Maintenance for Midwest EN Operators During Dry ConditionsPractical Antenna Maintenance for Midwest EN Operators During Dry Conditions

Radial and counterpoise choices

If you have room for a real ground system, the most robust HF choice in the Midwest EN region is still a ground-mounted vertical with many on-ground or shallow-buried radials. For 40–10 m, N6LF found that 32 radials of about 33 ft worked very well whether on the ground or elevated, which is a strong practical benchmark for multiband field and home installations. If you cannot lay that many wires, use 16–32 rather than stopping at 4–8 if at all possible.

If you cannot lay many ground radials, then do not half-commit to a poor earth return. Instead, switch strategies: use 4 resonant elevated radials at a genuine height above ground, or use a complete antenna structure such as a vertical dipole or other design that does not depend on earth-return RF current. ARRL explicitly notes that a “complete” antenna such as a dipole or ground plane does not require an RF ground in the same way, provided common-mode current is controlled with a choke.

Configuration Evidence-backed behavior When to use Main risk / caveat
4 on-ground radials Emergency-level baseline; N6LF called this “really flaky” Portable, temporary, proof-of-concept High ground loss; strong seasonal sensitivity
8 on-ground radials About +2.26 dB over 4-radial baseline on 40 m Entry-level improvement Still meaningfully lossy
16 on-ground radials About +3.76 dB over 4-radial baseline Good practical minimum for many sites Dry soil still hurts
32 on-ground radials About +4.16 dB over 4-radial baseline; worked very well 40–10 m in N6LF work Strong home or semi-permanent installation Labor and yard management
64 on-ground radials About +5.8 dB over 4-radial baseline High-performance installation More wire for diminishing returns
4 elevated resonant radials About +5.9 dB over 4-radial ground baseline, roughly matching 64 on-ground in N6LF’s 40 m test Small lots, roof/deck edges, constrained sites Must be resonant, symmetric, and properly elevated
Ground rod only Helps little at RF; ARRL says RF resistance remains high Safety/lightning system only Not a substitute for RF counterpoise

*Table values are synthesized from ARRL grounding guidance and N6LF’s QEX measurements.

What to expect as the soil dries

How Soil Moisture Dramatically Affects Ground Conductivity (Engineering Approximation)

Soil / moisture condition Representative conductivity band Likely antenna symptoms Best operator response
Wet to moist ~3 to 10+ mS/m Lowest ground loss; tuning close to spring baseline Record analyzer baseline; this is your reference state
Moderately dry ~1 to 3 mS/m Slight upward/downward resonance drift, more tuner work, weaker low-band reports Add radials near base, verify choke, compare WSPR/PSK reports to wet baseline
Dry ~0.3 to 1 mS/m Noticeable efficiency loss on 80/40 m verticals, feedpoint resistance/reactance shift, “it tunes but is deaf/weak” complaints Add 16–32 radials if possible, or convert to elevated resonant radials
Very dry / drought-stressed surface ~0.1 to 0.3 mS/m or worse Ground loss dominates short/loaded verticals; strongest seasonal performance drop Temporary irrigation near base if practical, aggressive radial upgrade, consider vertical dipole or complete counterpoise design

These conductivity bands are engineering approximations, not measured site values. They are based on the FCC/ITU/USDA ranges and on the fact that ITU’s loam example spans about 0.1 mS/m to 10 mS/m as soil dries or wets. The strongest practical impact will usually show first on low-band verticals and shorter loaded antennas because their loss budget is least forgiving.

Tuning and measurement

Use an antenna analyzer first and an SWR meter second. The analyzer tells you where resonance moved, whether feedpoint R and X changed, and whether the antenna became “easy to match but inefficient.” A shack SWR reading alone cannot tell you that; even ARRL licensing material reminds operators that a perfect 1:1 SWR does not guarantee an effective antenna.

For a rigorous Midwest EN seasonal workflow, build a wet-spring baseline and then compare it to late-summer dry-state measurements. Record at minimum: resonant frequency, (R), (X), SWR bandwidth, band/mode, transmit power, radial count, and soil condition. Then correlate those station measurements with PSKReporter or WSPRnet observations using the same band, power, mode, and time-of-day windows. A consistent drop in spots or in median path quality during dry periods, with the rig and schedule held constant, is strong circumstantial evidence that the ground system is the culprit.

If you want to test your safety/lightning grounding electrode, use a real ground-resistance tester rather than RF instruments. IEEE 81 is the governing measurement standard for ground resistance and potential gradients in earth. Clamp-on and fall-of-potential tools are the right electrical-domain instruments for this job. But be strict about the interpretation: that result tells you about the grounding electrode system, not the RF quality of your radial field. RF performance still has to be evaluated by feedpoint measurements and on-air field results.

Seasonal maintenance and dry-condition mitigation

For the EN Midwest climate, the highest-value maintenance is seasonal rather than one-time. After the wet spring, measure and log the antenna. Then repeat after prolonged dry periods, because that is when conductivity and permittivity shifts show up most strongly in real use. If the resonant point moves only a little but outgoing reports fall materially, the likely culprit is higher loss, not a catastrophic mismatch.

When dry conditions arrive, prioritize mitigation in this order:

  1. Add or densify radials, especially close to the base where most ground loss occurs.
  2. If space is limited, shift to properly resonant elevated radials instead of tolerating a sparse ground field.
  3. Verify that the feed line is not becoming part of the antenna by adding or improving a common-mode choke where appropriate.
  4. For temporary relief, wetting the soil near the base can help because soil conductivity rises with moisture and most loss is concentrated near the antenna base region.
  5. If the site is chronically poor, consider a complete counterpoise-based design such as a vertical dipole or other structure less dependent on earth conductivity.

Open questions and limitations

I did not establish a formal, authoritative geographic boundary for “Midwest EN,” because none of the reviewed official sources define one. I therefore used the user-specified interpretation and noted the alternate Maidenhead-grid meaning of “EN.”

I also did not quantify a separate, Midwest-specific 6-meter Sporadic-E climatology in this pass, because the strongest high-confidence recent sources I gathered were better on HF space weather, tropospheric VHF/UHF, and ground-system engineering than on real-time 6 m Es for this specific region. The VHF/UHF discussion above therefore emphasizes the tropospheric mechanisms that were well supported by the current source set.

Finally, the conductivity-versus-moisture plot and the recommended conductivity classes are engineering approximations, not a site survey. If you need a design-grade number for a specific property, the right next step is a local soil/ground-conductivity measurement or modeled estimate, plus a station-specific before/after validation with analyzer readings and on-air weak-signal reporting networks.


HF Dipole Quick‑Check

Field Measurements & Troubleshooting Flow

This quick-reference guide helps troubleshoot HF dipoles using real-world measurements, feed-line comparisons, and a practical field workflow.

Shop‑Ready Measurement Examples (20m Half‑Wave Dipole)

Example

Feedline Rig‑Side R (Ω) Rig‑Side X (Ω) Rig‑Side SWR Notes

A

Well
Tuned

20–30 ft LMR‑400 ≈ 48–55 ≈ ±0–10 ≈ 1.05–1.30 Feedpoint ≈ 50 + j0 Ω
B
Lossier
Line
30 ft RG‑8X Similar resonance Similar May appear “better” Expect 0.5–1.0 dB more loss vs LMR‑400. Lossy coax can hide true SWR.

Page Troubleshooting Flow

  • Calibrate analyzer using open / short / load.
  • Measure directly at the feedpoint first.
  • Record R, X, and SWR at the operating frequency.
  • Measure again at the rig with the installed feedline.
  • Clamp a current probe at the feedpoint and shack entry.
  • If common‑mode current is present, add a choke and re‑test.
  • Inspect connectors, weatherproofing, and strain relief.
  • Trim or length‑adjust elements to center resonance if needed.

HF Dipole Recommended Choke

Use a 9–12 turn FT‑240‑43 ferrite choke or equivalent at the feedpoint and/or shack entry to reduce common‑mode current on the coax shield.

Pass / Fail Thresholds

  • Feedpoint SWR > 2:1 → trim or length‑adjust the dipole elements.
  • Rig‑side SWR > 1.8:1 with low‑loss coax → verify feedpoint mismatch.
  • Clamp current > ~0.2 A RMS at shack entry → add or relocate choke(s).
  • Lossy coax can make SWR readings appear better than reality.
Target values near band center: R ≈ 50 Ω and X ≈ 0 Ω.

HF Dipole Field Tips

  • Document coax type and total feedline length.
  • Keep the feedpoint centered and mechanically balanced.
  • Weatherproof all outdoor connections.
  • Use low‑loss coax whenever possible for accurate readings.
  • Recheck measurements after each change.