This spring fascinates me. I'll completely uncoil it, except for a few kinks. Now watch as I put it in hot water, 75 degrees or so. Rapidly the spring reforms. Let's watch it again, but close up. I stretch the spring, and then, to slow down the action, use a hairdryer to heat it. This spring is made from night and all wire. The name comes from the elements it contains, and where it was discovered. Nickel, antitanium, and the naval ordinance lab. It's showing what's called the shape of memory effect. A link to this wire was formed at very high temperatures into a spring. This shape setting occurs at temperatures above about 500 degrees Celsius, and then cooled. Almost no matter how it's been at room temperature, it returns to its original shape when heated at 75 degrees Celsius or so. So why does night and all have this memory? The key is understanding how the atoms move in response to stretching and bending of a piece of night and all. Typically, any metal, whether or not, is comprised of small grains that, depending on the material, are microns to nanometers across. And each grain is comprised of atoms arranged in a regular repeating pattern. If this metal rod were held at the top and stretched, then the grains might elongate. And they can do this because the atoms inside move a bit in a metal bond can be formed more easily than a non-metals, and so the atoms slip. Although it's a bit more complicated than applied here, which looks like spherical atoms rolling along each other. It involves defects in the crystal that allow the atoms to move only small amounts. In night and all, though, generally the atoms don't slip. They accommodate the stresses from bending, stretching, compression, and so on in a different way, which produces the memory effect. Here's a simplified two-dimensional version of the atomic structure of night and all, but one that captures the essence of why it has a temperature-dependent memory. The crystallites in the small grains have a nice, tidy, highly symmetric arrangement. They add a seat on the corners of squares. At temperatures above 500 degrees Celsius or so, the night and all can be shaped into whatever form is useful. For example, the spring I showed you earlier. When it cools, the crystal structure, the arrangement of the atoms, changes only slightly. Notice that it's very similar. All the atoms are connected in the same way, but the nice, tidy squares are now rompuses. Notice that even though the atoms move a bit, the overall shape doesn't really change. So, for example, if you fashioned a spring, it still looks like a spring. This doesn't seem very exciting, but this structure has a unique property. It's composed of rompuses that are mirror images. For example, notice the position of the atoms above and below this line are identical, but are reflections of each other. This is called twin structure. You could have all of the rompuses oriented this way, or this way. And as you can now see, when the night and all cools, it forms equal amounts of these two orientations of rompuses. Once oriented this way, and once this way. What produces the memory effect in night and all is that these two orientations can easily be changed from one to the other with very small motions of the atoms. For example, if I take the cooled night and all and change it shape, some of the crystallite smud experience a shear of force across the top. Notice that in response, the atoms move and change the ratio of the two types of rompuses. In this example, they all change to one type. You could imagine that in response to different forces, that in a large enough crystal, there would be hundreds of mixtures of these two rompuses. And many, many more in a three-dimensional structure. But notice this. At all times, the atoms are connected in the same way as in the high-temperature phase, unlike in slip, where atoms can rearrange quite a bit more. So when the temperature is raised again, these rompuses, no matter how they are distributed, return to tidy squares. The only structure that can result is the original structure, and so the night-null reverts to the shape at high-tabourature. There are some clever uses for night-null. For example, this device has fascinated me since childhood. It's a type of engine. Its construction is very simple, a large and small wheel. Each groove done their side. With a loop of night-null wire that runs through the grooves and connects them. To make a run, I just contact the lower edge of the small bottom wheel with water, which I've heated again to 75 degrees Celsius. Then spin the top wheel a bit in the device that runs on its own. It uses the temperature difference between the water and the air to power the engine. When I remove the water, the wheel stops spinning. This engine runs because this loop of night-null wire was originally straight at a very high temperature, so as it's heated, it tries to straighten. To see how that causes the engine to operate, watch what happens as I contact the lower wheel with the heated water. I'll mark the position of the wire on the left with a yellow line. Then when I start the wheel, the wire's distance from the initial position is much greater. It's hard to see, so I'll mark its position with a purple line. This happens because when the bottom wheel comes into contact with a hot water, the section of the wire highlighted here in orange is heated. If it were not in a loop, then the wire would be straight like this. But because it's in a loop, as it tries to straighten, it exerts a force on the wheel, which causes it to turn. Let's break this down. On the right, the air cooled wire returns. It wraps onto the wheel. As the water heats the wire, it starts to straighten, but is restrained by being in a loop. This creates a force at this point on the wheel from this fall grill, which is the last point of contact of the wire on the wheel. This generates a force about the center of the wheel, which is transmitted as torque and sets in motion the engine. Although a lot of night-null-based engines were patented, often the practical uses of night-null are not as a shape memory metal, but as a super elastic material. Let me show you. Compare night-null wire to a piece of copper wire. If I move the copper wire a bit and let it go, it returns to its original position. That's an elastic deformation. But if I go too far, it doesn't return to its original shape, that's plastic deformation. Compare that to this piece of night-null wire. It shows that elastic response for small deviations. But if I do that same extreme deformation and then let go, the wire returns to its original state, even oscillating for a while. If I bend the wire into multiple loops and then release it, it becomes straight. This super-elasticity is closely related to the shape memory effect. Let's compare the two phenomena and look at what's happening at the atomic level. I start with shape memory. Here's a piece of night-null wire that's been conditioned at 500 degrees Celsius or so to be straight. At that very high temperature, the crystal structure in the grains is those tidy, neat squares. As it's cooled to room temperature, the twin structure forms the one with the equal number of left and right rompuses, which you recall doesn't change the overall shape much. Then when I deform the wire, the atoms and the crystallite shift in the grains to some unequal mixture, left and right rompuses. There are hundreds of possibilities. When I heat it with a hairdryer, the tidy, neat squares return and the wire becomes straight again. And then as it returns to room temperature, the twin structure returns, the one with an equal number of both rompuses. Now, let's look at a night-null wire that showed super-elasticity. It's been conditioned so that its crystal structure is those tidy, neat squares at room temperature, they would form the twin structure at minus 15 degrees Celsius, so much lower temperature than the shape memory effect. When I apply an external force to the wire, the crystal lights and the grains deform into the rompuses, whatever, mix of those would allow it to accommodate the reshaping. When I remove the force, then because it's at room temperature, it returns to the tidy squares. Here's an example of a commercial device that uses super-elastic night-null. It's a cage-like metal tube called a stint that's used by a cardiologist. The doctor inserts it into a vessel or duct here it's shown in a coronary artery, and it holds the walls in place. Because these are super-elastic, watch this. I can severely deform it. And when I release it, it returns to its original shape. To use it, a cardiologist chooses a stint with a slightly larger diameter than the vessel wall. It's then crimped to a size smaller than the vessel, inserted and allowed to expand. Because it's larger than the vessel's diameter, it keeps a force on the wall and resists compression. Night-nulls other commercial uses are in high-end products. Premium eyeglasses built from super-elastic night-null, so they can be bent and twisted, yet returned to their original shape. And its used in designs were reducing weight as critical. For example, in the 2014 Chevrolet Corvette, a night-null device replaced a heavy motorized actuator to open and close a vent in the car's trunk. There are thousands of more uses for night-null, and perhaps for other shape memory materials. For example, polymers that exhibit this phenomena are now in development. I'm Bill Hammock, the engineer guy.