
82CD878: Crystal Diamond Metallic Blue Iris A A A 4MM 16" String
These 4mm machine-cut crystal diamond beads come on a 16-inch strand with a metallic blue iris finish that earns the name — the surface shifts with the light in a way that flat color simply can't. If you're working with a cool-toned or jewel-toned palette, this is the bead that pulls everything together.
The finish is fully opaque with a metal-like surface that reads like plated metal, layered with a blue iris shift — think deep cobalt with a living, iridescent overlay rather than a flat coat.
Specifications
- Size: 04mm
- Color: Blues (mixed)
- Material: Glass Crystal
- Quantity: 16" Strand
What to make with them
The diamond cut and compact 4mm size make these ideal for structured bead-weaving patterns like right-angle weave or cubic RAW, where facets catch light at every angle. They also work beautifully strung as a standalone bracelet or layered in multi-strand necklaces where the metallic surface holds its own without competing with neighboring elements.
Original: $5.85
-65%$5.85
$2.05Product Information
Product Information
Shipping & Returns
Shipping & Returns
Description
These 4mm machine-cut crystal diamond beads come on a 16-inch strand with a metallic blue iris finish that earns the name — the surface shifts with the light in a way that flat color simply can't. If you're working with a cool-toned or jewel-toned palette, this is the bead that pulls everything together.
The finish is fully opaque with a metal-like surface that reads like plated metal, layered with a blue iris shift — think deep cobalt with a living, iridescent overlay rather than a flat coat.
Specifications
- Size: 04mm
- Color: Blues (mixed)
- Material: Glass Crystal
- Quantity: 16" Strand
What to make with them
The diamond cut and compact 4mm size make these ideal for structured bead-weaving patterns like right-angle weave or cubic RAW, where facets catch light at every angle. They also work beautifully strung as a standalone bracelet or layered in multi-strand necklaces where the metallic surface holds its own without competing with neighboring elements.











