{"product_id":"seymour-duncan-78-model-chevalet-noir-366980","title":"'78 MODEL CHEVALET NOIR","description":"\u003ch3\u003eA Pickup Born from the Golden Age of Custom Shop Mods\u003c\/h3\u003e\u003cp\u003eIn the late 1970s, Seymour Duncan established itself as the reference for custom pickups. In 1978, the demand was clear: rewind a P.A.F to make it more sensitive to natural and artificial harmonics while preserving the vintage spirit. The \"'78 Model\" follows this approach with a winding faithful to the specifications of the era and a decidedly musical personality.\u003c\/p\u003e\u003ch3\u003eWho It's For and Its Usage\u003c\/h3\u003e\u003cp\u003eThe Seymour Duncan \"'78 Model\" in the \u003cstrong\u003ebridge\u003c\/strong\u003e position is aimed at guitarists seeking a vintage-voiced sound but with the energy needed to go from \u003cstrong\u003enervous crunch\u003c\/strong\u003e to \u003cstrong\u003ebiting lead\u003c\/strong\u003e. It excels on rock\/hard rock riffs, articulate solos, and techniques where harmonics need to \"pop\" effortlessly, while maintaining expressive pick dynamics.\u003c\/p\u003e\u003ch3\u003eAlnico II + Double Coil: Warmth, Attack, and Harmonics\u003c\/h3\u003e\u003cp\u003eIts \u003cstrong\u003eAlnico II\u003c\/strong\u003e magnet provides a pleasant natural compression and warm tone, while the \u003cstrong\u003edouble coil\u003c\/strong\u003e (humbucker) ensures a consistent output level for dense and defined saturation. Thanks to its \u003cstrong\u003e4-conductor\u003c\/strong\u003e configuration, you can utilize modern wiring options (split, series\/parallel) to expand the tonal palette, from a snappier single-coil-like sound to classic humbucker thickness.\u003c\/p\u003e\n\n\u003ch2\u003eTechnical specifications\u003c\/h2\u003e\n\u003cstyle\u003e@media(max-width:632px){table[data-wb-spec]{display:grid;grid-template-columns:minmax(0,1fr) minmax(0,1fr)}table[data-wb-spec] colgroup{display:none}table[data-wb-spec] tbody,table[data-wb-spec] tr{display:contents}table[data-wb-spec] td{display:block;overflow-wrap:anywhere;grid-row:var(--wb-l);background-color:var(--wb-lb)}table[data-wb-spec] td[data-r]{grid-row:var(--wb-r);background-color:var(--wb-rb)}table[data-wb-spec] td[colspan=\"2\"]{grid-column:1\/-1}table[data-wb-spec] td:empty{display:none}}\u003c\/style\u003e\n\u003ctable data-wb-spec style=\"width:100%;table-layout:fixed\"\u003e\n\u003ccolgroup\u003e\u003ccol style=\"width:25%\"\u003e\u003ccol 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style=\"text-align:left\"\u003e\u003cstrong\u003eColor\u003c\/strong\u003e\u003c\/td\u003e\u003ctd data-r style=\"text-align:left;font-weight:var(--font-body-weight-bolder)\"\u003eBlack\u003c\/td\u003e\u003c\/tr\u003e\n\u003c\/table\u003e\n\u003ctable data-wb-spec style=\"width:100%;table-layout:fixed\"\u003e\n\u003ccolgroup\u003e\u003ccol style=\"width:25%\"\u003e\u003ccol style=\"width:25%\"\u003e\u003ccol style=\"width:25%\"\u003e\u003ccol style=\"width:25%\"\u003e\u003c\/colgroup\u003e\n  \u003ctr style=\"background-color:transparent;--wb-l:1;--wb-r:4;--wb-lb:var(--wb-neutral-50);--wb-rb:transparent\"\u003e\u003ctd style=\"text-align:left\"\u003e\u003cstrong\u003eBrand\u003c\/strong\u003e\u003c\/td\u003e\u003ctd style=\"text-align:left;font-weight:var(--font-body-weight-bolder)\"\u003eSeymour Duncan\u003c\/td\u003e\u003ctd data-r style=\"text-align:left\"\u003e\u003cstrong\u003eNeck resistance\u003c\/strong\u003e\u003c\/td\u003e\u003ctd data-r style=\"text-align:left;font-weight:var(--font-body-weight-bolder)\"\u003e7.85 kOhms\u003c\/td\u003e\u003c\/tr\u003e\n  \u003ctr style=\"background-color:var(--wb-neutral-50);--wb-l:2;--wb-r:5;--wb-lb:transparent;--wb-rb:var(--wb-neutral-50)\"\u003e\u003ctd style=\"text-align:left\"\u003e\u003cstrong\u003eModel\u003c\/strong\u003e\u003c\/td\u003e\u003ctd style=\"text-align:left;font-weight:var(--font-body-weight-bolder)\"\u003e\u0026quot;\u0026#039;78 Model\u0026quot;\u003c\/td\u003e\u003ctd data-r style=\"text-align:left\"\u003e\u003cstrong\u003eBridge resistance\u003c\/strong\u003e\u003c\/td\u003e\u003ctd data-r style=\"text-align:left;font-weight:var(--font-body-weight-bolder)\"\u003e8.82 kOhms\u003c\/td\u003e\u003c\/tr\u003e\n  \u003ctr style=\"background-color:transparent;--wb-l:3;--wb-r:6;--wb-lb:var(--wb-neutral-50);--wb-rb:transparent\"\u003e\u003ctd style=\"text-align:left\"\u003e\u003cstrong\u003eConstruction\u003c\/strong\u003e\u003c\/td\u003e\u003ctd style=\"text-align:left;font-weight:var(--font-body-weight-bolder)\"\u003e4-conductor wiring for coil splitting\u003c\/td\u003e\u003ctd data-r colspan=\"2\"\u003e\u003c\/td\u003e\u003c\/tr\u003e\n\u003c\/table\u003e","brand":"Seymour Duncan","offers":[{"title":"Default Title","offer_id":54334642323731,"sku":"366980","price":175.0,"currency_code":"EUR","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0984\/0872\/6803\/files\/14fccd219ab04b89a168657a745c248c85239cb8_ESD_78_B_B.png?v=1789070569","url":"https:\/\/woodbrass.shop\/products\/seymour-duncan-78-model-chevalet-noir-366980","provider":"Woodbrass.com","version":"1.0","type":"link"}