ASTM E1089-86(2007) PDF

ASTM E1089-86(2007) PDF

Name:
ASTM E1089-86(2007) PDF

Published Date:
03/01/2007

Status:
[ Withdrawn ]

Description:

Standard Test Method for Water Penetration of Flat Plate Solar Collectors by Uniform Static Air Pressure Difference (Withdrawn 2013)

Publisher:
ASTM International

Document status:
Active

Format:
Electronic (PDF)

Delivery time:
10 minutes

Delivery time (for Russian version):
200 business days

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$15
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1.1 This test method covers the determination of the resistance of flat plate solar collectors to water penetration when water is applied to their outer surfaces with a static air pressure at the outer surface higher than the pressure at the interior of the collector.

1.2 This test method is applicable to any flat plate solar collector.

1.3 The proper use of this test method requires a knowledge of the principles of pressure and deflection measurement.

1.4 The values stated in SI units are to be regarded as the standard. The values given in parentheses are for information only.

1.5 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use. Specific precautionary information is contained in Section 6.


File Size : 1 file , 71 KB
Note : This product is unavailable in Russia, Ukraine, Belarus
Number of Pages : 4
Published : 03/01/2007

History

ASTM E1089-86(2007)
Published Date: 03/01/2007
Standard Test Method for Water Penetration of Flat Plate Solar Collectors by Uniform Static Air Pressure Difference (Withdrawn 2013)
$15
ASTM E1089-86(2001)
Published Date: 01/01/2001
Standard Test Method for Water Penetration of Flat Plate Solar Collectors by Uniform Static Air Pressure Difference
$15
ASTM E1089-86(1995)
Published Date: 01/31/1986
Standard Test Method for Water Penetration of Flat Plate Solar Collectors by Uniform Static Air Pressure Difference
$16.2

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