Comparison of old and new ISO 9050 and ISO 10292 standards

The tables below compare the results calculated in accordance with the previous editions (ISO 9050:2003 and ISO 10292:1994) and the latest editions (ISO 9050:2026 and ISO 10292:2026) for five typical glass types. The five glass samples used for this comparison are the same as those featured on our NFRC/EN/ISO test method comparison page.

Example 1: Clear & uncoated laminated glass

Glass configuration: 6 mm clear glass + 1.52 mm PVB + 6 mm clear glass

Spectral transmittance and reflectance curves
ISO 9050:2003
ISO 10292:1994
ISO 9050:2026
ISO 10292:2026
Visible light transmittance0.8650.865
Visible light reflectance, front0.0770.077
Visible light reflectance, back0.0770.077
Solar direct transmittance0.6750.671
Solar direct reflectance, front0.0640.064
Solar direct reflectance, back0.0650.065
Total solar energy transmittance (TSET)0.7430.731
Shading coefficient (SC)0.8540.840
U-value [W/(m2K)]5.355.11

Example 2: Tinted & uncoated glass

Glass configuration: 8 mm tinted glass

Spectral transmittance and reflectance curves
ISO 9050:2003
ISO 10292:1994
ISO 9050:2026
ISO 10292:2026
Visible light transmittance0.3680.368
Visible light reflectance, front0.0480.048
Visible light reflectance, back0.0530.053
Solar direct transmittance0.3620.360
Solar direct reflectance, front0.0470.048
Solar direct reflectance, back0.0520.052
Total solar energy transmittance (TSET)0.5140.494
Shading coefficient (SC)0.5910.567
U-value [W/(m2K)]5.685.41

Example 3: Tinted & laminated glass with hard low-e coating

Glass configuration: 6 mm tinted glass + 1.52 mm PVB + 6 mm glass with hard low-e on #4

Spectral transmittance and reflectance curves
ISO 9050:2003
ISO 10292:1994
ISO 9050:2026
ISO 10292:2026
Visible light transmittance0.3270.327
Visible light reflectance, front0.0530.053
Visible light reflectance, back0.0870.087
Solar direct transmittance0.2430.242
Solar direct reflectance, front0.0510.051
Solar direct reflectance, back0.0920.091
Total solar energy transmittance (TSET)0.3700.341
Shading coefficient (SC)0.4260.393
U-value [W/(m2K)]3.853.31

Example 4: Clear DGU with soft low-e coating

Glass configuration: 8 mm clear glass with soft low-e on #2 + 12 mm air space + 5 mm low iron glass + 1.52 mm PVB + 5 mm low iron glass

Spectral transmittance and reflectance curves
ISO 9050:2003
ISO 10292:1994
ISO 9050:2026
ISO 10292:2026
Visible light transmittance0.7010.701
Visible light reflectance, front0.1300.130
Visible light reflectance, back0.1360.136
Solar direct transmittance0.3060.311
Solar direct reflectance, front0.4660.455
Solar direct reflectance, back0.4180.405
Total solar energy transmittance (TSET)0.3350.341
Shading coefficient (SC)0.3850.392
U-value [W/(m2K)]1.531.50

Example 5: Tinted DGU with soft low-e coating

Glass configuration: 6 mm tinted glass with soft low-e #2 + 12 mm air space + 6 mm clear glass

Spectral transmittance and reflectance curves
ISO 9050:2003
ISO 10292:1994
ISO 9050:2026
ISO 10292:2026
Visible light transmittance0.2670.267
Visible light reflectance, front0.0980.098
Visible light reflectance, back0.2430.243
Solar direct transmittance0.1380.140
Solar direct reflectance, front0.1470.145
Solar direct reflectance, back0.4070.401
Total solar energy transmittance (TSET)0.1930.191
Shading coefficient (SC)0.2220.220
U-value [W/(m2K)]1.571.56

Portable High-Pressure Measurement with the Delta OHM HD2124.2 and TP704-500BAI

Related instruments pressure transmitters

Shown below is the HD2124.2 data logger with the TP704-500BAI probe for absolute pressure measurement up to 500 bar. The instrument also measures temperature and is compatible with a wide range of interchangeable Pt100 temperature probes for different measurement applications.

Related instruments

HD9008T7AC air temperature transmitter with 4-20 mA output

Related instruments Temperature & humidity

Shown below is the HD9008T7AC air temperature transmitter with 4-20 mA output. When used outdoors, it is recommended to pair the transmitter with a solar radiation shield (e.g., HD9007-A1) to minimize environmental effects such as solar radiation and rain.

Related instruments

HD2717T.DR temperature & humidity transmitter with S.TV vertical probe

Related instruments Temperature & humidity

Shown below is the HD2717T.DR temperature and humidity transmitter, equipped with an S.TV vertical probe.

The HD2717 series features data logging capability and relay outputs, making it suitable for HVAC applications that require monitoring and control (regulation) functions.

Related instruments

Can daylight reflectance test be performed on curved surfaces?

Specular reflection follows the law of reflection, which states that the angle of incidence is equal to the angle of reflection, measured with respect to the local surface normal.

For a flat surface, the surface normal is uniform across the entire area. As a result, incident light is reflected in a single, well-defined direction, allowing the specular component to be reliably captured by the instrument.

For a curved surface, the surface normal varies from point to point. According to the law of reflection, the direction of reflected light therefore also varies across the surface. Instead of a single direction, the specular reflection is spread over a range of angles.

Daylight reflectance instruments measure reflection within a defined geometry. For curved surfaces, part of the specular reflection falls outside this geometry. As a result, the instrument misses part of the specular component, leading to an underestimation of the specular daylight reflectance.

In practice:

  • For curved surfaces with a strong specular component, the measurement error can be significant. Results should therefore be interpreted with caution.
  • For curved surfaces with a weak specular component, the impact is negligible, and measurements may still be acceptable

In summary, daylight reflectance testing can be performed on curved surfaces, but the accuracy, particularly for the specular component, may be limited.

PRO 131.2 2-channel handheld thermocouple thermometer

Related instruments Temperature & humidity

Shown below is the PRO131.2, a 2-channel handheld thermocouple thermometer, with two probes connected.

The PRO131.2 offers higher accuracy compared to the ECO 130 entry-level thermocouple thermometer. It also supports multiple thermocouple types, whereas the ECO 130 is limited to K-type thermocouples only.

An alternative model, PRO135.2, is available with an additional data logging feature, making it suitable for applications requiring temperature recording over time.

Related instruments

Is Solar reflectance index (SRI) applicable to translucent materials?

Related services Solar reflectance index (SRI)

The concept of Solar Reflectance Index (SRI) is not directly applicable to translucent materials, such as fabrics and membranes. Please refer to this post for a simple way to check if a material is translucent using mobile phone flashlight.

This limitation is explicitly reflected in the title of ASTM E1980:

ASTM E1980: Standard Practice for Calculating Solar Reflectance Index of Horizontal and Low-Sloped Opaque Surfaces

The scope clearly specifies opaque surfaces only. Therefore, applying ASTM E1980 to calculate the SRI of translucent materials is not technically valid.

This post explains the key challenges involved in determining the SRI of translucent materials and discusses practical workarounds.

The challenges

There are three main challenges when attempting to determine the SRI of translucent materials:

1. Solar energy transmission

Solar radiation interacting with a material follows the relationship:

solar reflectance + solar transmittance + solar absorptance = 1

For opaque materials, solar transmittance = 0, so solar absorptance can be derived directly from solar reflectance.

However, for translucent materials:

  • Both solar reflectance and solar transmittance need to be measured
  • Solar absorptance can only be determined after accounting for transmission

This adds complexity to the characterization process.

2. Infrared radiation transmission

Thermal emittance is commonly measured using ASTM C1371. However, this method assumes the material is opaque.

For translucent materials:

  • Infrared radiation may pass through the sample
  • The measured emittance can be influenced by the substrate or background behind the material

As a result, the measurement may not represent the intrinsic property of the material itself.

3. SRI calculation model

The SRI calculation defined in ASTM E1980 is based on a heat balance model that assumes:

  • No solar transmission
  • Surface-only energy exchange

Because translucent materials allow radiation to pass through:

  • The underlying heat transfer model becomes invalid
  • The calculated SRI does not accurately represent real thermal behavior

Practical workarounds

Although SRI cannot be directly applied, there are practical approaches to characterize translucent materials:

1. Make the system opaque

The translucent material can be mounted onto an opaque substrate to form a composite system. This prevents solar and infrared radiation transmission
Standard SRI measurement methods can then be applied

Please note that the result represents the SRI of the system, not the standalone material.

2. Test the material by assuming it is opaque

In some cases, translucent materials may be tested using the same procedures as opaque materials, effectively assuming that the material is opaque during the SRI measurement.

This approach can still provide meaningful results when the material has low solar transmittance, such that only a small portion of the incident solar radiation passes through the sample. Under these conditions, the measured SRI may still serve as a useful practical indicator of surface thermal behaviour.

However, the transmitted solar component is not properly accounted for in the measurement. Therefore, results obtained using this approach should be interpreted with caution, particularly for materials with significant solar transmission.

3. Measure optical properties separately

It is still possible to characterize the optical behaviour of translucent materials by measuring solar reflectance, solar transmittance, and solar absorptance separately.

This approach provides a more complete physical understanding of the material. The measured optical properties can then be used in thermal models, other than the SRI model, for further analysis.

PBS880D BAROsense barometric pressure transmitter with static port

Related instruments pressure transmitters

Shown below is a PBS880D BAROsense barometric pressure transmittance with a static port:

The PBS880D BAROsens is a barometric pressure transmitter designed for accurate atmospheric pressure measurements.

It has a standard measuring range of 800 to 1100 mbar. An alternative version is available with a range of 600 to 1100 mbar. The device provides a 4–20 mA output, with additional output options such as 0–10 V available upon request.

The unit is equipped with a static port, which minimizes the influence of dynamic pressure caused by wind, making it suitable for open-field measurements. The static port comes with a mounting bracket and can be installed on poles with diameters of up to 50 mm.

Related instruments

HD32.8.8 8-channel thermocouple data logger

Related instruments Temperature & humidity

Shown below is an HD32.8.8 thermocouple data logger. It supports up to eight thermocouple probes and is compatible with all standard thermocouple types using miniature connectors.

For applications requiring more thermocouple input channels, the HD32.8.16 variant supports up to 16 thermocouple probes.

Related instruments