30
630
672
2,174
MPa
315.4
ksi
30
630
672
2,174
MPa
315.4
ksi
The Hardness Conversion Calculator converts between the three most widely used hardness scales — Brinell (HB), Rockwell C (HRC), and Vickers (HV) — and provides an approximate ultimate tensile strength (UTS) for steel. Hardness scales measure a material's resistance to permanent indentation but use different indenter geometries and loads, so the relationship between scales is empirical rather than exact: $$HV \approx 0.0544 \cdot HRC^2 + 12.09 \cdot HRC + 260$$ $$HB \approx 17.4 \cdot HRC - 0.0275 \cdot HRC^2 + 133$$
These conversions are essential in materials engineering because different industries and standards specify hardness on different scales. Heat treatment specifications often use HRC, incoming material certifications may report HB, and research laboratories prefer HV for its scale-independent geometry. Being able to translate between scales allows engineers to compare specifications, verify material properties, and ensure quality compliance across supply chains.
Each hardness test measures indentation resistance differently:
Because the indenter shapes and load levels differ, conversions between scales are empirical and based on extensive testing databases. ASTM E140 provides standard conversion tables for steel, non-ferrous metals, and other materials. The polynomial approximations used in this calculator are fitted to the ASTM E140 data for carbon and alloy steels.
The approximate UTS relationship $$\sigma_{UTS} \approx 3.45 \times HB \text{ (in MPa)}$$ is a widely used empirical correlation valid for carbon and low-alloy steels in the range 120-450 HB. It is less accurate for highly alloyed steels, non-ferrous metals, and hardness values outside this range.
Important limitations: conversions are most accurate for carbon and alloy steels. For stainless steels, aluminum alloys, copper alloys, and other materials, the conversion factors differ. Always specify which standard table was used when reporting converted hardness values.
The converted values are approximations based on empirical correlations for carbon and alloy steels. Accuracy is typically ±2 HRC or ±5% for HB and HV within normal ranges. The HRC scale is only valid above approximately 20 HRC (below this, use Rockwell B scale). The approximate UTS uses the standard 3.45× multiplier for Brinell hardness and should be treated as a rough estimate — always verify with actual tensile testing for critical applications.
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A steel at 45 HRC (typical for tool steels and high-strength fasteners) corresponds to approximately 452 HB / 565 HV with an estimated UTS around 1560 MPa.
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At 200 HB (typical for normalized AISI 1045 steel), HRC is below the reliable range (< 20 HRC). The approximate UTS of 690 MPa aligns well with published values for this condition.
Different scales were developed for different applications. Brinell (1900) was first and is good for bulk materials. Rockwell (1914) is faster since hardness is read directly from the machine. Vickers (1921) works across all hardness ranges and is geometry-independent. Each has advantages depending on sample size, material, and testing environment.
No. Conversions between scales are empirical approximations based on testing databases (primarily ASTM E140). They are most accurate for carbon and alloy steels and may be significantly off for non-ferrous metals, stainless steels, or materials with unusual strain-hardening behavior. Accuracy is typically ±2 HRC or ±5%.
Rockwell C scale is defined for 20-70 HRC. Below 20 HRC, the indentation is too shallow for accurate measurement, and Rockwell B scale (1/16" ball, 100 kgf) should be used instead. Above 70 HRC is extremely hard (diamond-like coatings) and requires special techniques.
For carbon and low-alloy steels, the approximation $$UTS \approx 3.45 \times HB$$ (in MPa) is reliable within about 10% for 120-450 HB. This relationship does not apply to non-ferrous metals, austenitic stainless steels, or highly cold-worked materials, where the hardness-strength correlation is different.
Vickers microhardness (HV with loads of 10-1000 gf) is best for thin samples, coatings, and individual grains. The sample must be at least 10× thicker than the indent depth. Brinell is unsuitable for thin materials because the large ball creates a deep, wide indent. Rockwell superficial scales (15N, 30N, 45N) can also work for thin parts.
Brinell hardness depends on the applied force, ball diameter, and material of the ball (steel or tungsten carbide). Standard conditions for steel use a 10 mm tungsten carbide ball at 3000 kgf (HBW 10/3000). Using different conditions gives different values, so the test conditions must always be reported with the result.
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