ASTM D6110-08
Standard Test Method for Determining the Charpy Impact Resistance of Notched Specimens of Plastics

Standard No.
ASTM D6110-08
Release Date
2008
Published By
American Society for Testing and Materials (ASTM)
Status
Replace By
ASTM D6110-10
Latest
ASTM D6110-18
Replace
ASTM D6110-06
Scope

Before proceeding with this test method, refer to the material specification for the material being tested. Any test specimen preparation, conditioning, dimensions and testing parameters required by the materials specification shall take precedence over those required by this test method. Table 1 of Classification D 4000 lists the ASTM materials standards that currently exist. If there is no material specification, then the requirements of this test method apply.

The pendulum impact test indicates the energy to break standard test specimens of specified size under stipulated conditions of specimen mounting, notching (stress concentration), and pendulum velocity at impact.

For this test method, the energy lost by the pendulum during the breakage of the specimen is the sum of the energies required to initiate fracture of the specimen; to propagate the fracture across the specimen; to throw the free ends of the broken specimen (toss energy); to bend the specimen; to produce vibration in the pendulum arm; to produce vibration or horizontal movement of the machine frame or base; to overcome friction in the pendulum bearing and in the indicating mechanism, and to overcome windage (pendulum air drag); to indent or deform, plastically, the specimen at the line of impact; and to overcome the friction caused by the rubbing of the striking nose over the face of the bent specimen.

Note 58212;The toss energy, or the energy used to throw the free ends of the broken specimen, is suspected to represent a very large fraction of the total energy absorbed when testing relatively dense and brittle materials. No procedure has been established for estimating the toss energy for the Charpy method.

For tough, ductile, fiber-filled, or cloth-laminated materials, the fracture propagation energy is usually large compared to the fracture initiation energy. When testing these materials, energy losses due to fracture propagation, vibration, friction between the striking nose and the specimen has the potential to become quite significant, even when the specimen is accurately machined and positioned, and the machine is in good condition with adequate capacity (see Note 6). Significant energy losses due to bending and indentation when testing soft materials have also been observed.

Note 68212;Although the frame and the base of the machine must be sufficiently rigid and massive to handle the energies of tough specimens without motion or excessive vibration, the pendulum arm cannot be made very massive because the greater part of its mass must be concentrated near its center of percussion at its striking nose. Locating the striking nose precisely at the center of percussion reduces the vibration of the pendulum arm when used with brittle specimens. Some losses due to pendulum arm vibration (the amount varying with the design of the pendulum) will occur with tough specimens even when the striking nose is properly positioned.

In a well-designed machine of sufficient rigidity and mass, the losses due to vibration and friction in the pendulum bearing and in the indicating mechanism will be very small. Vibrational losses are observed when wide specimens of tough materials are tested in machines of insufficient mass, or in machines that are not securely fastened to a heavy base.

Since this test method permits a variation in the width of the specimens and since the width dictates, for many materials, whether a brittle, low-energy break (as evidenced by little or no drawing down or necking and by a relatively low energy absorption) or a ductile, high-energy break (as evidenced by considerable drawing or necking down in the region behind the notch and by a relatively high energy absorption) will occur, it is necessary that the width be stated in the specification covering that material and that th........

ASTM D6110-08 history

  • 2018 ASTM D6110-18 Standard Test Method for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2017 ASTM D6110-17 Standard Test Method for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2010 ASTM D6110-10 Standard Test Method for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2008 ASTM D6110-08 Standard Test Method for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2006 ASTM D6110-06 Standard Test Method for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2005 ASTM D6110-05a Standard Test Method for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2005 ASTM D6110-05 Standard Test Methods for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2004 ASTM D6110-04e1 Standard Test Methods for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2004 ASTM D6110-04 Standard Test Methods for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 2002 ASTM D6110-02 Standard Test Methods for Determining the Charpy Impact Resistance of Notched Specimens of Plastics
  • 1997 ASTM D6110-97 Standard Test Methods for Determining the Charpy Impact Resistance of Notched Specimens of Plastics



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