28.11.2012 Views

Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

ON ELECTROMAGNETIC THIRRING<br />

PROBLEMS<br />

Markus K<strong>in</strong>g<br />

Institute of Theoretical Physics<br />

University of Tüb<strong>in</strong>gen, D–72076 Tüb<strong>in</strong>gen, Germany<br />

Herbert Pfister<br />

Institute of Theoretical Physics<br />

University of Tüb<strong>in</strong>gen, D–72076 Tüb<strong>in</strong>gen, Germany<br />

Keywords: Thirr<strong>in</strong>g problem, exact solutions.<br />

1. INTRODUCTION<br />

The st<strong>and</strong>ard Thirr<strong>in</strong>g problem <strong>de</strong>scribes the (non–local) <strong>in</strong>fluence<br />

of rotat<strong>in</strong>g masses on the <strong>in</strong>ertial properties of space–time, especially<br />

the so–called dragg<strong>in</strong>g of <strong>in</strong>ertial frames <strong>in</strong>si<strong>de</strong> a rotat<strong>in</strong>g mass shell<br />

relative to the asymptotic frames. It is then a natural question to ask<br />

whether <strong>and</strong> how properties other than <strong>in</strong>ertial ones are also <strong>in</strong>fluenced<br />

by rotat<strong>in</strong>g masses, <strong>and</strong> the first (non–<strong>in</strong>ertial <strong>and</strong> non–gravitational)<br />

properties which come here to one’s m<strong>in</strong>d, are surely electromagnetic<br />

phenomena.<br />

In<strong>de</strong>ed there exists a whole series of papers [1, 2, 3, 4, 5] on mo<strong>de</strong>ls<br />

where a charge sits <strong>in</strong>si<strong>de</strong> a slowly rotat<strong>in</strong>g mass shell (mass M, radius<br />

R), <strong>and</strong> where the rotationally <strong>in</strong>duced magnetic field is calculated <strong>and</strong><br />

discussed, typically for small ratios M/R <strong>and</strong>/or An especially<br />

remarkable but confus<strong>in</strong>g fact is that Cohen’s results [2] are <strong>in</strong> complete<br />

agreement with Machian expectations whereas Ehlers <strong>and</strong> R<strong>in</strong>dler [4]<br />

<strong>in</strong>terpret their results to be “<strong>in</strong> fact Mach–negative or, at best, Mach–<br />

neutral”.<br />

We exam<strong>in</strong>e a class of mo<strong>de</strong>ls consist<strong>in</strong>g of two spherical shells of radii<br />

<strong>and</strong> the first one carry<strong>in</strong>g a nearly arbitrary charge but no<br />

rest mass, the second one be<strong>in</strong>g nearly arbitrary massive but electrically<br />

neutral. The only restriction on the parameters is that the systems<br />

should be free of s<strong>in</strong>gularities <strong>and</strong> horizons. To these shells we apply<br />

small but otherwise arbitrary “stirr<strong>in</strong>g” angular velocities <strong>and</strong><br />

<strong>Exact</strong> <strong>Solutions</strong> <strong>and</strong> <strong>Scalar</strong> <strong>Fields</strong> <strong>in</strong> <strong>Gravity</strong>: Recent Developments<br />

Edited by Macias et al., Kluwer Aca<strong>de</strong>mic/Plenum Publishers, New York, 2001 281

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!