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H04 C15500 Copper vs. H04 C16200 Copper

Both H04 C15500 copper and H04 C16200 copper are copper alloys. Both are furnished in the H04 (full hard) temper. They have a very high 99% of their average alloy composition in common. There are 30 material properties with values for both materials. Properties with values for just one material (2, in this case) are not shown.

For each property being compared, the top bar is H04 C15500 copper and the bottom bar is H04 C16200 copper.

Metric UnitsUS Customary Units

Mechanical Properties

Elastic (Young's, Tensile) Modulus, GPa 120
120
Elongation at Break, % 5.0
9.0
Fatigue Strength, MPa 170
210
Poisson's Ratio 0.34
0.34
Shear Modulus, GPa 43
43
Shear Strength, MPa 250
390
Tensile Strength: Ultimate (UTS), MPa 430
510
Tensile Strength: Yield (Proof), MPa 410
470

Thermal Properties

Latent Heat of Fusion, J/g 210
210
Maximum Temperature: Mechanical, °C 200
370
Melting Completion (Liquidus), °C 1080
1080
Melting Onset (Solidus), °C 1080
1030
Specific Heat Capacity, J/kg-K 390
380
Thermal Conductivity, W/m-K 350
360
Thermal Expansion, µm/m-K 17
17

Electrical Properties

Electrical Conductivity: Equal Volume, % IACS 90
90
Electrical Conductivity: Equal Weight (Specific), % IACS 91
90

Otherwise Unclassified Properties

Base Metal Price, % relative 33
30
Density, g/cm3 8.9
9.0
Embodied Carbon, kg CO2/kg material 2.7
2.6
Embodied Energy, MJ/kg 42
41
Embodied Water, L/kg 360
310

Common Calculations

Resilience: Ultimate (Unit Rupture Work), MJ/m3 21
45
Resilience: Unit (Modulus of Resilience), kJ/m3 730
970
Stiffness to Weight: Axial, points 7.2
7.2
Stiffness to Weight: Bending, points 18
18
Strength to Weight: Axial, points 13
16
Strength to Weight: Bending, points 14
16
Thermal Diffusivity, mm2/s 100
100
Thermal Shock Resistance, points 15
18

Alloy Composition


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Cadmium (Cd), % 0
0.7 to 1.2
Copper (Cu), % 99.75 to 99.853
98.6 to 99.3
Iron (Fe), % 0
0 to 0.2
Magnesium (Mg), % 0.080 to 0.13
0
Phosphorus (P), % 0.040 to 0.080
0
Silver (Ag), % 0.027 to 0.1
0
Residuals, % 0 to 0.2
0