to be published in European Journal of Physics

Observation of magnetic field lines in the vicinity of asuperconductor with the naked eye
Yoshihiko Saito
Nakanoshima Science Laboratory, Osaka Science Museum, Osaka-shi
530-0005 Japan
E-mail: saito_sci-museum.jp
Abstract. This paper describes a new method of demonstration about superconductivity.
A GdBaCuO high temperature superconductor of 60 mm in diameter and 10 mm inheight, a sintered NdFeB cubic magnet with the edge length of 100 mm, and iron wires
coated by colored vinyl are used to visualise the magnetic field lines in the vicinity ofthe superconductor, when it is placed in a magnetic field. The spatial distributions ofiron wires make it understandable how the magnetism of superconductivity causes thelevitation and suspension of conventional demonstrations. This paper is intended to beread especially by teachers of undergraduate courses and educators of science museums
or science centers.

1. Introduction
Superconductivity is a phenomenon occurring in certain materials generally at low
temperatures, characterized by the two distinct properties of (1) exactly zero electrical resistanceand (2) the expulsion of the interior magnetic field. The latter property is called Meissner effect[1], and makes the superconductor exhibit perfect diamagnetism. The former property,
combined with the discovery of high-temperature superconductors (HTSs) in and after 1986 [2],aroused the expectations of applying the superconductivity technology in industry.
As soon as the discovery of HTS took place, the method to demonstrate the Miessner effect
was presented [3] and apparatus were developed [4, 5]. Discussion of rigid levitation andsuspension of an HTS by a magnet also followed soon, by taking account of the pinning effect[6] (this effect is explained in Appendix). These demonstrations have allowed the generalaudience to observe the effects of superconductivity in larger scale and to come to a better
understanding of the related physics than before. (Note that the practical HTSs used in the
recent large scale demonstration show the diamagnetism caused by the pinning effect muchstronger than that caused by the Meissner effect [7]; see Appendix for details.)
Examples of such conventional demonstrations, which the author has prepared in anespecially large scale, are given in figures 1 and 2. Figure 1 shows a demonstration of repulsion,in which a sintered NdFeB ring magnet (hereafter called ring magnet) is repelled by a
GdBaCuO HTS. The magnetic flux density of the ring magnet is about 0.4 T at the surface. A

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pair of chopsticks restricts horizontal movements of the ring magnet to make it float just above
the HTS. Without this restriction, the magnet cannot levitate but goes away from above the HTS
and falls down onto the table. Figure 2 shows a demonstration of the stable holding of an HTS
at approximately constant distances from the ring magnet. Namely, in the continuous shots, an
HTS is seen held (a) under, (b) on a side of, and (c) over a ring magnet, at almost the same
relative positions with respect to the magnet. Note that any restriction of horizontal movements
as shown in figure 1 is not necessary for this levitation. The physical explanations of these
phenomena are given in section 2. These demonstrations can be presented successively to show
the difference between the two phenomena of repulsion and stable holding. From theseprocedures, however, it is hard to understand the physics in the vicinity of the HTS and magnet.

Figure 1. Conventional demonstration of repulsion in a large scale. A ring magnet is repelled byan HTS, which is immersed in liquid nitrogen for cooling. A pair of chopsticks restricts
horizontal movements of the magnet.

(a)

(b)

(c)

Figure 2. Conventional demonstration, in a large scale, of holding an HTS. An HTS (the white
object) can be kept (a) below, (b) on a side of, and (c) above a ring magnet (the black object
held by a hand) at approximately constant distances from the magnet.
For educational purposes, it is desirable that the magnetic field lines be visible for suchsuperconductors to make the underlying physics understandable. Quantitative analysis has been
done extensively [6, 8-9], and visualisation of real superconducting phenomena has been
discussed. Tonomura et al., for example, demonstrated visualisation of magnetic field lines insuperconductor at the vortex level by using electron holography and digital phase analysis [10].
While being useful for basic research and industrial applications, these methods cannot easily be
used for demonstration to general audience and students because of high technicality.

to be published in European Journal of Physics

The present author has studied new methods of demonstration, which requires no specialized
device or skills and therefore are easily prepared and conducted by non-experts for educationaluse, and has discussed a simple method to visualise external magnetic field lines repelled by the
HTS in the previous papers [11], showing that the phenomena of the effect are easily observed
without a supplementary device. The present paper describes the results of the exploration ofdemonstrating magnetic field lines connected to the pinned flux in the HTS as well as therepelled field lines. The latter and the former field lines related to repulsion and stable holding
shown in figures 1 and 2, respectively. The new demonstrations are considered useful for giving
qualitative understanding of these phenomena to the observers.
It is often explained that the repulsion of the magnet as shown in figure 1 and the holding of
the HTS as shown in figure 2 are caused by the Meissner effect. However, the latterphenomenon is caused obviously by the pinning effect (see subsection 2.2), and the former
phenomenon is also considered possibly by the pinning effect [7] (see Appendix).
2. Visualisation of magnetism in superconductivity
In this section, the author discusses visualisation of magnetic field lines in the vicinity of the
HTS in two scenarios shown in figures 1 and 2. The HTS used was fabricated by Nippon SteelCorporation [12], and is 60 mm in diameter and 10 mm in height. The HTS is immersed in an
external magnetic field, which is produced by a sintered NdFeB cubic magnet with the edge
length of 100 mm (hereafter called cube magnet). This cube magnet is of the type used innuclear magnetic resonance imaging, and the magnetic flux density is about 0.5 T at the surface(figure 3). The magnetic field lines are observed through iron wires of 0.3-mm diameter coatedby colored vinyl, so-called twist tie.
Figure 3 shows that the pieces of wire in acrylic cases stand against the gravity under the
influence of the magnetic field. Light fragments of wire are easily aligned to magnetic fieldlines with minor friction against the acrylic case, and point in the direction tangent to magnetic
field lines. Thus the distribution of the wires reflects the magnetic field strengths at different
places. Simple tapping of the acrylic case is enough to reduce the friction momentarily to thenegligible level and to get an arrangement of wires close to the real density distribution. The
underlying principle of this method is identical to that of the well-known iron filings, and theeffect of the gravitational force is negligible compared with that of the magnetic force in thevicinity of the magnet.
Visualisation of magnetic field lines in the vicinity of the HTS causing repulsion and pinningare described in the following subsections.

to be published in European Journal of Physics

Figure 3. Demonstration of magnetic field lines. Iron wires in transparent acrylic cases show
magnetic field lines coming out of a cubic magnet with the edge length of 100 mm. The
magnetic flux density of the magnet is about 0.5 T at the surface.
2.1. Repulsion of external field
Two pictures of figure 4 show demonstrations of the magnetic field near an HTS placed
above the cube magnet, similarly to the scenario shown in figure 1. The HTS is immersed inliquid nitrogen, which in turn is in a Styrofoam container. In figure 4 (a), the wires initiallyplaced directly above the HTS are pushed out by the magnetic field to their present positions;
namely, the distributions of wires shows that there is no magnetic field line just above the HTS.
In figure 4 (b), the distribution of wires shows the magnetic field lines in the spaces surrounding
the HTS; namely, how magnetic field is repelled by the presence of the HTS. These
distributions of wires correspond to two views of figure 5 (b), which is the schematic diagram of
the repulsion by an HTS placed in the magnetic field shown by figure 5 (a). Thus, figures 4(a)and (b) are effective demonstrations of the diamagnetism by the use of magnetic field lines.

(a)

(b)

Figure 4. Repulsion of magnetic field lines. (a) An HTS is immersed in liquid nitrogen in a
Styrofoam container. A cube magnet is located under the container. Wires to show the magnetic
field lines are put on a transparent plastic plate, which in turn is placed on the container. Thosewires that were initially put above the HTS are pushed out by the magnetic field to the positions

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now seen in the picture. (b) Small plastic cases containing wires are placed above and below the
HTS. Large plastic cases with wires are placed below the lowest small plastic case. The cube
magnet is placed below the lower large plastic case. The distributions of wires again show that
there is no magnetic field line passing through the HTS.

(a)

(b)

Figure 5. Schematic diagrams of the repulsion of magnetic field lines. The external magnetic
field lines coming out of a magnet, as shown in (a), are repelled by the presence of an HTS, asin (b). These diagrams have been drawn on the basis of a theoretical consideration.
From the demonstrations of figure 4, the explanation of the phenomenon shown in figure 1
can be derived as follows: The magnetic field lines emanating from the ring magnet in figure 1
are repelled by the HTS. If the magnet gets closer to the HTS, the distortion of the magnetic
field grows, and the distortion energy becomes higher, causing the repulsion of the magnet, andaccordingly levitation under the restriction of horizontal movement. Note that the HTS in figure
5 (b) seems to levitate without the restriction. If the horizontal component of the repulsive force
is directed to the center of the magnet, levitation will occur without the restriction. The early
demonstrations of levitation were of such kind. In fact, a small HTS can levitate without the
restriction above the ring magnet. Such levitation and the stable holding as shown in figure 2 aredifferent phenomena. The latter is explained in the next subsection.
It might be supposed that figure 5 shows the Meissner effect. In the case of the practical HTS
used here, however, the pinning effect is considered to be responsible for the observed repulsionof the external field [7] (see Appendix for details).
2.2. Pinning of external field
To obtain the HTS in the scenario shown in figure 2, an HTS is cooled in the presence of amagnetic field, which is produced by the ring magnet placed above the HTS as shown in figure
6. The magnetic field in the HTS does not change by cooling. After cooling and taking away ofthe magnet, the magnetic flux in the HTS stays there because of pinning (see Appendix for
details).

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Figure 6. Schematic diagram of arrangement to produce the pinning of magnetic flux. Aftercooling, the magnetic field lines before cooling are pinned in the HTS.
Figures 7 and 8 show demonstrations of the magnetic field lines around the HTS with pinned
magnetic flux when the HTS is placed at different positions with respect to the cube magnet.
Schematic diagrams to explain these demonstrations are given in figures 9 and 10. Details ofthese figures are explained below.
In figure 7, wires show magnetic field lines when the HTS is moved horizontally above the
cube magnet. The magnetic field due to the HTS itself reflects the flux distribution of the ringmagnet when the HTS was cooled in the arrangement of figure 6. Figures 7 (a) and (c)demonstrate respectively that when the HTS is brought to the left and right, the magnetic fieldlines are distorted so as to be connected tangentially with the internal magnetic field lines of the
HTS as shown in figures 9 (a) and (c). Inside the HTS, however, the magnetic flux is pinned, sothat the field lines stay as they are.

(a)

(b)

(c)

Figure 7. Change in magnetic field lines above the HTS in which magnetic flux is pinned, as
observed when the HTS is put (a) above left, (b) just above and (c) above right with respect tothe cube magnet. The HTS is put in the Styrofoam container of figure 6. It can be understoodfrom this demonstration that the magnetic field trapped in the HTS is held fixed regardless ofchange in external field.

to be published in European Journal of Physics

(a)

(b)

Figure 8. Magnetic field lines above HTS with pinned magnetic flux, in a varying external
magnetic field strength. The HTS, put in the Styrofoam container of figure 6, is placed above a
cube magnet. The distance between the HTS and the magnet is 190 mm in (a), and 60 mm in (b).
Flux pinning in the HTS was caused in advance by a ring magnet in the arrangement of figure 6.
It can be understood from this demonstration that the trapped magnetic field is held fixed inposition regardless of change in external field.

(a)

(b)

(c)

Figure 9. Schematic diagrams of the pinning effect resisting the horizontal movement in an
external magnetic field. The external magnetic field lines are deformed for tangential
connection with the field lines in the HTS. The HTS is shifted horizontally (a) to the left and (c)to the right, but the internal magnetic field is not altered because of the pinning effect. These
diagrams have been drawn on the basis of a theoretical consideration.

(a)

(b)

(c)

Figure 10. Schematic diagrams of magnetic field lines around an HTS with flux pinning, placedat different distances from a magnet. The bound magnetic field lines are connected with theexternal magnetic field lines, but the internal magnetic field is not altered because of the pinningto be published in European Journal of Physics

effect. These diagrams have been drawn on the basis of a theoretical consideration.
In figure 8 (a), the HTS is placed at a distance of 190 mm above the cube magnet. The
corresponding magnetic field lines around the HTS are schematically drawn in figure 10 (a).
Because the magnetic field due to the HTS is stronger than that caused by the cube magnet atthe position of the HTS, the field lines near the HTS make closed loops. When the HTS islowered to a distance of 60 mm as shown in figure 8 (b), the magnetic field lines from the partof the cube magnet just below the HTS become connected to the internal field lines of the HTS,
as shown in figure 10 (c), and those outside that part are expelled by the diamagnetism. In either
condition, the trapped magnetic field lines are unaltered.
By the demonstration of figures 7 and 8, it can be understood that the magnetic field lines are
fixed inside the HTS, showing the macroscopic pinning (see Appendix in detail). From thesedemonstrations, the phenomena in figure 2, i.e., the holding of an HTS at approximately
constant distances, can also be understood as follows: Before cooling by the arrangement shownin figure 6, the magnetic field lines emanating from the north pole of the ring magnet penetrate
the HTS, and stream into the south pole. In this situation, the magnetic field is in the groundstate. After cooling, any change in the relative position between the HTS and the ring magnet
distorts the ground state magnetic field and increases the energy of the field, because themagnetic field lines are pinned inside the HTS. In other words, a restoring force acts the HTS
for any change in the relative position between the HTS and the ring magnet. Because of thetight pinning effect of the practical HTS and the large magnetic flux density of the ring magnet(0.1 T at the HTS), the restoring force is so strong that the effect of the gravitational force isnegligible. Therefore, the relative position before cooling is stable, and thus the stable holdingof the HTS at approximately constant distances is made possible.
So far the author has described methods to visualise the magnetic field in the vicinity of an
HTS in an applied external magnetic field by means of fragments of wires. Although it is notpossible directly to observe the microscopic picture of vortex lattices of the pinning effect (seeAppendix), macroscopic results of the pinning effect can easily be demonstrated by the use ofaccessible materials.
3. Concluding remarks
The author has developed a simple and easily accessible method to visualise the repulsion
and pinning of the magnetic field lines by an HTS. By the use of this method, the breakdown ofsuperconductivity can also be demonstrated when the HTS above the cube magnet in figure 7 iswarmed in the room temperature environment. Several movies have been prepared and posted at
a Web site [13] to help readers obtain a better picture of the demonstration described in thispaper. The movies are made to supply much information on superconductivity to non-experts,

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and the effectiveness has been demonstrated at Osaka Science Museum, Osaka, Japan, wherevisitors not only enjoy the less intuitive physics phenomena, but also deepen theirunderstandings by picturing the magnetic field lines surrounding the HTS and the magnets intheir minds. This demonstration should also be useful in introductory courses onsuperconductivity, because the method presented is simple, easy to set up and use, and thedevice is large enough to be observed by relatively large audience at once. The HTS and the
cube magnet as used here are presently available only in Japan, namely, from Technology
Research Laboratories, Nippon Steel Corporation [14], and Jishakukobo [15], respectively.
Even if the equivalents of these were not found, the demonstration would be possible withscaled-down equipment.
Acknowledgments.
The author would like to express his gratitude to Nippon Steel Corporation (NSC) for theirsupport in the design of the device and supplying the GdBaCuO bulk HTS. He is grateful to Dr.
Hidekazu Teshima (Advanced Technology Research Laboratories, NSC) for his coping withdifficulties in the process of this research and his report for the practical GdBaCuO HTS. He
also thanks Ms. Misato Hayashida and Dr. Tatsuo Tabata (Emeritus Professor of Osaka
Prefecture University) for their helpful comments on physics and improvements in English.
Appendix. Basics of superconductivity
In this appendix, we give a brief description of the basics of superconductivity and introduce
the pinning effect at microscopic level [16].
Two types of superconductors, i.e., Types I and II, are known. A Type I superconductor,
when it is placed in an external magnetic field weaker than a critical value Hc, is in the
superconducting state (called Meissner state) and shows the Meissner effect, i.e., the expulsionof the interior magnetic field. In a magnetic field stronger than Hc, it is in the normal state, atwhich superconductivity is destroyed. A Type II superconductor is in the Meissner state for amagnetic field weaker than a critical value Hc1; in the vortex lattice state for a magnetic field
between Hc1 and a second critical value Hc2 (Hc1 < Hc2); and in the normal state for a fieldstronger than Hc2. In the vortex lattice state, the magnetic flux from the external field is notcompletely expelled but the superconductor is still superconducting. At the microscopic level,
quantized flux lines penetrate into the superconductor through the normal state core of vortex.
The interactions of such vortices form a vortex lattice [10, 17]. Thus the Type II superconductorin the vortex lattice state allows the field to penetrate, while the penetration is completely
forbidden in the Meissner state. The values of Hc1 and Hc2 depend on temperature; namely, thesevalues increase when temperature is decreased. All known HTSs are of Type II. A Type IIsuperconductor shows the phenomenon where magnetic flux becomes trapped or “pinned”

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inside the material. This is called pinning effect, and is possible when there are defects that act
to resist the movement of the vortex to some extent just like the static friction force and to trap
the vortex lattice in the crystalline structure of the superconductor.
The practical HTS used in this work includes finely dispersed non-superconductor crystal in
the matrix of the pure GdBaCuO crystal HTS [12]. The non-superconductor crystals make thepinning effect very tight. In other words, non-superconductor crystals cause the strong static
friction for the magnetic field lines. This tight pinning effect exhibits the holding of the HTS as
shown in figure 2 as well as the powerful repulsion of the eternal magnetic field, which could bea few T from experience [18]. It cannot be claimed that the repulsion of the magnet shown infigure 2 and that of the wires in figure 4 are caused by the Meissner effect [7]. The reason is asfollows: Though the value of Hc1 of the GdBaCuO HTS is not in the review work of the author,
in the case of YBaCuO HTS, Hc1 at liquid nitrogen temperature is 10–20 mT [19]. Therefore,
the repulsion of the external magnetic field by the Meissner effect can be seen up to about 10–
20 mT. However, the magnetic flux densities at the surface of the HTS in figures 2 and 4 areabout 50 mT and 30 mT, respectively. These values are higher than Hc1 of YBaCuO. In any case,the practical GdBaCuO HTS exhibits the repulsion of the magnetic field lines caused by thetight pinning effect much stronger than the one caused by the Meissner effect.
If the HTS is cooled in the presence of a magnetic field, the magnetic field in the HTS does
not change at the naked-eye level by cooling because of the pinning effect. Physically speaking,a continuous magnetic field in the HTS changes to discrete ones, i.e., bundles of the quantizedmagnetic flux lines penetrating vortices. The HTS in the scenario shown in figure 2 was
obtained by this method, i.e., by cooling under the ring magnet as shown in Figure. 6. The
details of the scenario are as follows. When any region in the HTS is cooled to such atemperature that Hc2 is above the applied magnetic field strength (note that Hc2 increases as thetemperature is decreased), the vortex lattice state is achieved in that region, and the magnetic
field lines that pass through normal state cores inside the HTS are fixed by the pinning effect.
Thus, the HTS becomes the vortex lattice state with non-uniform vortex density. This state does
not change even if the HTS is cooled further or if the ring magnet is taken away, because themagnetic field lines are pinned.
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