Determining the Ice-binding Planes of Antifreeze Proteins by Fluorescence-based Ice Plane Affinity

Summary

Antifreeze proteins (AFPs) bind to specific planes of ice to prevent or slow ice growth. Fluorescence-based ice plane affinity (FIPA) analysis is a modification of the original ice-etching method for determination of AFP-bound ice planes. AFPs are fluorescently labeled, incorporated into macroscopic single ice crystals, and visualized under UV light.

Abstract

Antifreeze proteins (AFPs) are expressed in a variety of cold-hardy organisms to prevent or slow internal ice growth. AFPs bind to specific planes of ice through their ice-binding surfaces. Fluorescence-based ice plane affinity (FIPA) analysis is a modified technique used to determine the ice planes to which the AFPs bind. FIPA is based on the original ice-etching method for determining AFP-bound ice-planes. It produces clearer images in a shortened experimental time. In FIPA analysis, AFPs are fluorescently labeled with a chimeric tag or a covalent dye then slowly incorporated into a macroscopic single ice crystal, which has been preformed into a hemisphere and oriented to determine the a- and c-axes. The AFP-bound ice hemisphere is imaged under UV light to visualize AFP-bound planes using filters to block out nonspecific light. Fluorescent labeling of the AFPs allows real-time monitoring of AFP adsorption into ice. The labels have been found not to influence the planes to which AFPs bind. FIPA analysis also introduces the option to bind more than one differently tagged AFP on the same single ice crystal to help differentiate their binding planes. These applications of FIPA are helping to advance our understanding of how AFPs bind to ice to halt its growth and why many AFP-producing organisms express multiple AFP isoforms.

Introduction

The production of antifreeze proteins (AFPs) is an important survival mechanism of some organisms that live in ice-laden environments. Until recently, it was thought that the sole function of AFPs was to prevent or slow the growth of internal ice crystals that would block circulation, cause tissue damage, and osmotic stress. Organisms that cannot tolerate any degree of freezing, such as fish, express AFPs to completely inhibit ice crystal growth¹. Others, such as grass, are freeze tolerant and express AFPs to inhibit ice recrystallization which reduces the formation of large ice crystals in their tissues². Stabilization of membranes in low temperature is yet another function that was suggested for the AFPs³. Recently, a novel role was suggested for the AFP of an Antarctic bacterium, Marinomonas primoryensis, from ice-covered brackish lakes⁴. This AFP is part of a much larger adhesin protein⁵ that is thought to attach the bacterium to ice for better access to oxygen and nutrients⁶. Other microbes are known to secrete AFPs, which might alter the structure of the ice in which they live⁷.

AFPs have been found in some fish, insects, plants, algae, bacteria, diatoms, and fungi. They have remarkably divergent sequences and structures consistent with their evolution from different progenitors on various occasions; and yet they all bind to ice and inhibit its growth by the adsorption-inhibition mechanism⁸. The AFPs each have a specific surface that acts as its ice-binding site (IBS). These have typically been identified by site-directed mutagenesis of surface residues^9-11. The IBS is hypothesized to arrange water molecules in an ice-like pattern that matches specific planes of ice. Thus the AFP forms its ligand before binding to it^{5, 12}. Ice planes can be defined by their Miller indices, and different AFPs can bind to different planes. Thus, type I AFP from winter flounder binds to the 20-21 pyramidal planes¹³, type III AFP binds both primary prism and pyramidal planes using a compound ice-binding surface^11,14, while the spruce budworm AFP, a hyperactive AFP, binds simultaneously to both the primary and basal planes^15,16. Other hyperactive AFPs, such as MpAFP, bind to multiple ice planes as shown by their complete coverage of single ice crystal hemispheres^5,17. It is hypothesized, that the ability of hyperactive AFPs to bind the basal plane, as well as other planes, may account for their 10-fold higher activity over moderately active AFPs¹⁸. Though the efficiency of hyperactive AFPs is well documented, their ability to bind to multiple ice planes is still not understood.

The original method for determining the AFP-bound ice planes was developed by Charles Knight^13,19. In this method, a macroscopic single ice crystal is mounted onto a hollow metal rod (cold finger) and formed into a hemisphere by submerging it into a hemispherical cup filled with degassed water. Then, the hemisphere is submerged into a dilute solution of AFPs and a layer of ice is grown from the AFP solution onto the ice crystal hemisphere over several hours controlled by the temperature of the ethylene glycol circulating through the cold finger. The ice crystal is removed from the solution, detached from the cold finger, and placed in a -10 to -15 °C freezer room. The surface is scraped with a sharp blade to remove the frozen surface film of antifreeze protein solution and the ice crystal is allowed to sublimate for at least 3 hr. After sublimation, the ice planes bound by AFPs can be seen as white etched patterns derived from residual protein. The ice hemisphere can be oriented to its c-axis and a-axes, to locate the basal and prism planes of ice, and determine the Miller indices of the etched patches.

Here we describe a modification of the original method for determining AFP-bound planes of ice, a method we refer to as fluorescence-based ice plane affinity (FIPA)¹¹. The AFPs are fluorescently labeled with either a chimeric tag, such as green fluorescent protein (GFP)^11,16,17,20, or with a fluorescent dye covalently bound to the AFP^5,21. The fluorescently labeled AFPs are adsorbed to a single ice crystal and overgrown using the same experimental procedure as the original ice-etching experiments. The extent of AFP binding to the growing ice hemisphere can be monitored throughout the experiment using an ultraviolet (UV) lamp. After the experiment is complete, the hemisphere can be directly taken off of the cold finger and imaged, without sublimation. However, if desired, the hemisphere can be left to sublimate to visualize a traditional ice etch. Modifications introduced to the FIPA methodology shorten the traditional ice-etching protocol by several hours. Additionally, there is the potential for simultaneously imaging several AFPs, each with a different fluorescent label, to visualize the overlapping patterns of AFP-bound ice planes.

Protocol

1. Growing Single Ice Crystals

1. Take a clean metal pan (15 cm diameter, 4.5 cm high) that fits into, and can float on, an ethylene glycol cooling bath.
2. Prepare polyvinyl chloride (PVC) cylindrical molds, (4.5 cm diameter, 3-4 cm high, 4 mm thick), by sawing sections from a pipe.
   1. Cut a notch, (1 mm wide, 2 mm high) on one side (Figure 1A).
   2. Prepare as many molds that can fit comfortably into the pan (Figure 1B).
      Note: A study showed that polyvinyl alcohol (PVA) can affect ice nucleation²². However, in our open mold PVC system we have not encountered problems of atypical ice formation. 
3. Apply a light film of vacuum grease to the bottom surface ring of each mold, which is the surface with the notch cut out. Seal this greased, notched surface onto a metal pan with the notches oriented away from the center of the pan. Be careful not to fill or obstruct the notches with grease.
4. Add 0.22 μm filtered and degassed/deionized water to the center of pan, but outside of the molds, and allow the water to slowly enter into the molds through the notches. Be careful not to introduce any bubbles. The water layer should be approximately 5 mm deep.
5. Place the pan into a temperature-controlled ethylene glycol bath cooled to -0.5 °C. The pan should be perfectly level. Add ballast weights to the sides of the pan if necessary.
6. After the pan and water have reached -0.5 °C, add a small piece of ice to the middle of the pan, outside of the molds.
   1. This will nucleate ice growth in the supercooled water across the pan and into the molds. The small notch at the bottom of each mold allows only one ice crystal to propagate through, resulting in a single ice crystal in each mold.
   2. Incubate overnight to form a layer of ice.
7. Over the next three days add 13 ml of 4 °C degassed/deionized water to each mold once a day and drop the temperature of the ethylene glycol bath after each addition to -0.8 °C on day one, to -1.1 °C on day two, and to -1.5 °C on day three.
   1. Incubate at those temperatures overnight.
   2. By day four, the molds should be completely filled with ice.
8. Pull the molds off the pan, push the ice crystals out of the molds, and store on a clean surface, such as a weighing boat, in a -20 °C freezer for approximately 1 hr before handling.
9. Rather than preparing many small single ice crystals, a large single ice crystal several liters in volume can be prepared in a constant temperature incubator as described by Knight²³. The large ice crystal can be stored for a year or more if kept covered in a -15 to -20 °C freezer. Portions of single crystal can be cut from the ice block with a saw as required.

2. Determining Singularity and Orientation of the Ice Crystal

1. Determine if the ice expelled from the mold is a single crystal by observing in a freezer room, between two crossed polaroids (Figure 1D).
   1. If the ice crystal is single, then no cracks or discontinuities should be seen, and the light direction should not change within the ice crystal.
      Note: If a freezer room is not available, a cold room can be used instead in all required steps, being cautious to work quickly and handle the ice sparingly.
2. Due to the ice birefringence, one may determine orientation of the c-axis at the same time. Use the following information to determine the orientation:
   1. When the c-axis is exactly parallel to the incident light, in theory, no light will pass through the crossed polaroids. If the incident light is titled slightly from parallel with the c-axis, a uniform multicolor spectrum of light is transmitted through the crystal when it is rotated between the crossed polaroids. This uniform transmittance arises from the optical inactivity of ice I_h along its c-axis²⁴. The basal plane of the ice crystal is normal to the c-axis.
   2. When the c-axis is further from parallel to the incident light and the ice crystal is rotated between the crossed polaroids, the transmitted light will alternate between 0-100% transmittance with every 90° of rotation of the crystal.
   3. Most commonly, the c-axis will be normal to the circular plane of the cylindrical ice crystal.
3. Determine the orientation of the a-axes by ice pitting²⁵ which is done by wrapping the ice crystal tightly in aluminum foil, poking a small hole with a needle through the foil into the ice on the basal plane (normal to the c-axis), and placing it under vacuum for 20 min.
   1. This treatment will produce an etch with hexagonal symmetry on the basal plane, where the a-axes run through the vertices of the six-sided star (Figure 2A).
   2. If desired, the ice crystal can be cut with a saw either parallel or perpendicular to one side of the hexagon to mount it with a primary or secondary prism plane perpendicular to the cold finger, respectively (Figure 3).

3. Adsorption of Fluorescently Labeled Antifreeze Proteins to a Single Ice Crystal

1. Mount a single ice crystal onto the cold finger (Figure 1C) by first boring a cavity into the top of the crystal. To do this, alternate melting the ice with a two aluminum rods of slightly different diameter, but similar to the diameter of the cold finger, to form the cavity into which the cold finger can fit.
2. Cool the cold finger to -0.5 °C, place in the ice cavity, and hold the ice crystal in place until it freezes to the metal (Figure 2B). Avoid air bubbles when attaching the crystal to the finger as they hinder efficient transfer of heat from the finger to the rod.
3. Fill a hemispherical cup that is approximately twice the diameter of the ice crystal with filtered deionized water or buffer, cooled to approximately 4 °C. Submerge the cold finger-bound ice crystal into the cup and remove excess water or buffer such that the top of the ice crystal is approximately level with the liquid layer and the ice is not touching the cup walls.
   1. Cover the cup with insulation and lower the temperature to -5 °C.
   2. Wait approximately 1 hr for the ice crystal to form into a hemisphere, checking its status approximately every 20 min (Figure 2C).
   3. The ice will take the shape of the hemispherical cup by melting and growing the ice crystal, but it should never overgrow to touch the cup walls. There should be at least a 1 cm gap between the wall and hemisphere and the cold finger should not protrude from the ice.
4. Remove the cup from the ice crystal and add the fluorescent protein solution to a final volume of 25-30 ml and desired analysis concentration, being careful to keep the total liquid volume in the cup unchanged. A typical AFP concentration is 0.1 mg/ml.
   1. Resubmerge the ice crystal into the cup so that the top of the ice crystal is at level with the liquid and the ice crystal is not touching the cup walls (Figure 2D).
   2. Drop the cold finger temperature to -8 °C and let the protein solution freeze into the ice crystal for 2-3 hr, stirring the solution often. The ice formed from the protein solution should be at least 5 mm before stopping ice growth.
5. Remove the ice crystal from the cup while still attached to the cold finger. Detach the ice from the latter by warming the coolant through the cold finger to just above 0 °C and wait until the ice crystal melts off.
6. Place the crystal flat side down onto a clean surface, such as a weighing dish, being careful not to touch the newly form ice and store at -20 °C for at least 20 min before handing.

4. Visualization of Antifreeze-protein-bound Planes of Ice

1. Visualization of fluorescence is done in a darkened freezer or cold room, by placing the ice crystal flat side down under lamps with wavelength specific excitation filters to excite the fluorescent label and camera emission filters to block out any other nonspecific light. Based on the pattern, the ice planes that are bound by AFPs can be estimated (Figure 4).
2. If wavelength specific lights are not available a UV light box can be used instead.
3. Traditional ice etches can also be performed simply by allowing the ice hemisphere to sublimate at -20 °C for at least 3 hr, after which residual protein powder may become visible on the ice surface (Figure 5).
4. Step 2.3 can be repeated in order to determine the orientation of the a-axes of the completed ice hemisphere.

Results

Preparation and mounting of the single ice crystal are the two steps of the FIPA procedure where errors are most commonly made. Determining if the prepared ice crystal is single is done by examining it through crossed polaroids (Figure 1D), as outlined in step 2.1 of the protocol section. If a multicrystalline ice crystal is used for the FIPA analysis, the result will be discontinuous binding of the AFPs on the hemisphere without a coherent binding pattern (Figure 6B). If the ice crystal...

Discussion

Development of the ice-etching method by Charles Knight for determination of AFP-bound ice planes greatly advanced studies on the mechanism of ice binding by AFPs. Whereas structures of AFPs could be solved by X-ray crystallography^26,27 there was no obvious method for deducing the complementary surface on ice to which the AFP bound. When type I AFP from winter flounder was initially characterized, it was hypothesized to bind to the primary prism planes of ice²⁸. However, Knight's ground bre...

Materials

List of materials used in this article

Name	Company	Catalog Number	Comments
NESLAB RTE Refrigerating Bath/Circulators	Thermo Scientific	RTE7
Ethylene glycol, Premixed Antifreeze/Coolant	Certified	29-3037-0	Common automotive antifreeze
Cold finger	not available	not available	Custom made with brass (9 cm long, 1.5 cm outer diameter)
Hemispherical cup	not available	not available	Custom made with resin (8 cm outer diameter, 6 cm inner diameter)
High Dual Output Lighting System	Lightools Research	LT-99D2, Illumatools DLS 120 volts AC, LT-9470FX, LT-9549FX	Additional and custom excitation filters can be purchased from Lightools Research
Camera	Canon	EOS 50D
Emission Filters	Lightools Research	LT-9EFPVG, LT-9GFPVG, LT-9RFPVG	Filter ring adapter may be required to fit filter onto camera lens