Book contents
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 The linear oscillator driven by thermal noise and with electrical damping
- 3 External sources of noise and design of experiments
- 4 The weak principle of equivalence
- 5 Verification of the weak principle of equivalence for free particles
- 6 Newtonian attractions of extended bodies
- 7 Experimental tests of the inverse square law
- 8 The constant of gravitation
- 9 Conclusion
- References
- Index
5 - Verification of the weak principle of equivalence for free particles
Published online by Cambridge University Press: 10 October 2009
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 The linear oscillator driven by thermal noise and with electrical damping
- 3 External sources of noise and design of experiments
- 4 The weak principle of equivalence
- 5 Verification of the weak principle of equivalence for free particles
- 6 Newtonian attractions of extended bodies
- 7 Experimental tests of the inverse square law
- 8 The constant of gravitation
- 9 Conclusion
- References
- Index
Summary
Introduction
Although the weak principle of equivalence has been verified for ordinary macroscopic matter to very high precision, two questions remain open:
Is the principle valid for antimatter? Although indirect evidence from virtual antimatter in nuclei and short-lived antiparticles suggests that antimatter may have normal gravitational properties, no direct tests of the validity of the weak principle of equivalence for antimatter have been made.
Is the principle valid for microparticles? As the test bodies in macroscopic experiments are formed of neutrons, protons and electrons bound in nuclei, there is no doubt about the validity of the weak principle of equivalence for bound particles. However, the possibility of the principle of equivalence being violated for free particles should be studied.
Two main features characterize laboratory tests of the weak principle of equivalence for free elementary particles, both the consequence of their small masses. (1) When forces on substantial masses of bulk material are compared, a null experiment based on comparing different test bodies of two kinds of material can be devised. That is not possible for microscopic particles, and the gravitational accelerations have to be measured directly and subsequently compared with the acceleration of ordinary bulk matter to obtain the Eötvös coefficient. (2) The gravitational forces are very weak, even in the field of the Earth (which is the strongest attractive field), and so the accuracy of any experiment is very poor compared with Eötvös-type experiments using bulk masses.
- Type
- Chapter
- Information
- Gravitational Experiments in the Laboratory , pp. 97 - 108Publisher: Cambridge University PressPrint publication year: 1993