Skip to main content

Superconductors and Friction

I spent most of yesterday travelling between Austin and College Station, but I did manage to get a little bit of research in.  I'm looking for other experiments related to Hirsch's theories we can do in conjunction to the search for H-rays.  One of the measurable predictions of Hirsch's theory is a change in the coefficient of sliding friction when a material enters it's superconducting state.


New to the lab book?  Scroll to the bottom for background and a summary of the experiment.

Hirsch mentions[1] that a finding of reduced friction in superconductors might be evidence in support of his hole theory of superconductivity.

Furthermore, the electronic layer outside the surface
is likely to affect the friction properties of the superconductor,
by providing a ‘lubricating layer’ on top
of which another material would slide. As a matter of
fact, an abrupt drop in sliding friction between a lead
surface and solid nitrogen has been observed when Pb
enters the superconducting state [15]. We infer that
this effect is due to the physics of the electron layer
outside the surface discussed here, and hence that a
friction drop should be observed for all superconductors.

He cites, ([15] above), an experiment reported by Dayo, Alnasrallah, and Krim[2] as having actually shown a drop in the sliding friction between Pb and solid nitrogen in a liquid helium reservoir.  The experimental setup for the DAK experiment is shown in picture 2.



A quartz resonator was covered with thin film of Pb and then nitrogen was adsorbed into the surface of the Pb.  By measuring the quality factor of the underlying quartz resontaor, the researchers claimed they were able to monitor the friction between the Pb and the layer of nitrogen.  If the nitrogen could easily slide across the Pb, then the underlying resonator could vibrate more easily than if it could not.  This apparatus described has been used freqently in friction research and is know as a quartz crystal microblalnce.  DAK reported that when the Pb entered it's usperconducting state, there was a large, almost discontinuous, reduction in the coefficient of sliding friction between the Pb and the nitrogen.

There are issues however...  Renner, Rutledge, and Taborek, repeated the DAK experiment and got a null result.  Krim replied stating that the RRT experient had used a contaminated sample.  The important takeaway for the work here is that if Krim is correct, then additional friction experiments would require more resources than we currently have at hand.

A similar test has been done with YBCO, by Krim and Altfeder[5].  The results showed that there was a roughly linear reduction between YBCO and a Fe surface as the temperature of the YBCO approached the critical temperature, but that friction held steady once the YBCO entered the superconducting state.



References

1.  Hirsch on superconductors and friction [open access]
http://arxiv.org/abs/cond-mat/0301611

2.  A. Dayo, W. Alnasrallah, J. Krim, Phys. Rev. Lett. 80 (1998)
1690.

3.  More theoretical work on the DAK experiment
http://arxiv.org/abs/cond-mat/9905264

4.  R. L. Renner, J. E. Rutledge, and P. Taborek, preceding
Comment, Phys. Rev. Lett. 83, 1261 (1999).
http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.83.1261

5.  YBCO and friction
http://scitation.aip.org.lib-ezproxy.tamu.edu:2048/content/aip/journal/jap/111/9/10.1063/1.4717983

6.  Friction on Wikipedia
https://en.wikipedia.org/wiki/Friction


Background
Hirsch's theory of hole superconductivity proposes a new BCS-compatible model of Cooper pair formation when superconducting materials phase transition from their normal to their superconducting state[1].  One of the experimentally verifiable predictions of his theory is that when a superconductor rapidly transitions, (quenches), back to its normal state, it will emit x-rays, (colloquially referred to here as H-rays because it's Hirsch's theory).

A superconductor can be rapidly transitioned back to its normal state by placing it in a strong magnetic field.  My experiment will look for H-rays emitted by both a Pb and a YBCO superconductor when it is quenched by a strong magnetic field.
This series of articles chronicles both the experimental lab work and the theory work that’s going into completing the experiment.

The lab book entries in this series detail the preparation and execution of this experiment… mostly.  I also have a few theory projects involving special relativity and quantum field theory.  Occasionally, they appear in these pages.

Call for Input
If you have any ideas, questions, or comments, they're very welcome!

References

1.  Hirsch, J. E., “Pair production and ionizing radiation from superconductors”, http://arxiv.org/abs/cond-mat/0508529 

Comments

Popular posts from this blog

The Valentine's Day Magnetic Monopole

There's an assymetry to the form of the two Maxwell's equations shown in picture 1.  While the divergence of the electric field is proportional to the electric charge density at a given point, the divergence of the magnetic field is equal to zero.  This is typically explained in the following way.  While we know that electrons, the fundamental electric charge carriers exist, evidence seems to indicate that magnetic monopoles, the particles that would carry magnetic 'charge', either don't exist, or, the energies required to create them are so high that they are exceedingly rare.  That doesn't stop us from looking for them though! Keeping with the theme of Fairbank[1] and his academic progeny over the semester break, today's post is about the discovery of a magnetic monopole candidate event by one of the Fairbank's graduate students, Blas Cabrera[2].  Cabrera was utilizing a loop type of magnetic monopole detector.  Its operation is in concept very sim

Cool Math Tricks: Deriving the Divergence, (Del or Nabla) into New (Cylindrical) Coordinate Systems

Now available as a Kindle ebook for 99 cents ! Get a spiffy ebook, and fund more physics The following is a pretty lengthy procedure, but converting the divergence, (nabla, del) operator between coordinate systems comes up pretty often. While there are tables for converting between common coordinate systems , there seem to be fewer explanations of the procedure for deriving the conversion, so here goes! What do we actually want? To convert the Cartesian nabla to the nabla for another coordinate system, say… cylindrical coordinates. What we’ll need: 1. The Cartesian Nabla: 2. A set of equations relating the Cartesian coordinates to cylindrical coordinates: 3. A set of equations relating the Cartesian basis vectors to the basis vectors of the new coordinate system: How to do it: Use the chain rule for differentiation to convert the derivatives with respect to the Cartesian variables to derivatives with respect to the cylindrical variables. The chain

More Cowbell! Record Production using Google Forms and Charts

First, the what : This article shows how to embed a new Google Form into any web page. To demonstrate ths, a chart and form that allow blog readers to control the recording levels of each instrument in Blue Oyster Cult's "(Don't Fear) The Reaper" is used. HTML code from the Google version of the form included on this page is shown and the parts that need to be modified are highlighted. Next, the why : Google recently released an e-mail form feature that allows users of Google Documents to create an e-mail a form that automatically places each user's input into an associated spreadsheet. As it turns out, with a little bit of work, the forms that are created by Google Docs can be embedded into any web page. Now, The Goods: Click on the instrument you want turned up, click the submit button and then refresh the page. Through the magic of Google Forms as soon as you click on submit and refresh this web page, the data chart will update immediately. Turn up the: