The Equine Foot, Biomechanical and Anatomical Form Function. Hoof Balance and Symmetry, a Review of Current Theory. M. N. Caldwell FWCF¹* & D. Duckett FWCF² ¹The School of Veterinary Nursing & Farriery Science, Myerscough College, Myerscough Hall, Bilsborrow, Preston, Lancashire, PR3 0RY ². 709 Tennis Avenue, Ambler. PA. 19002. U.S.A. *¹ Tel: 01995 642000 ext; 2057 Mob: 07792374551 emails; markncaldwell@btinternet.com or mcaldwell@myerscouch.ac.uk Word count does not include figures and references. 3758 Key words: Farriery, anatomy, biomechanical, conformation, hoof trimming, foot balance, hoof capsule, pathology. Summary Farriery attempts to maintain equilibrium within the foot by trimming to achieve an illdefined and subjective empirical interpretation of “Static Foot Balance” (Hickman & Humphrey 1987; Stashak 2002). This interpretation of foot balance is mostly derived from historical texts (Dollar & Wheatley 1898; Russell 1897; & Lungwitz 1891; 1897). In nature shape and form of a structure relate directly to function. The hoof capsule is such an example of this concept. The primary functions of the hoof capsule and its associated structures are to absorb impact shock during locomotion, assist in the transfer of weight from the skeletal column and protect the underlying structures whilst providing grip during locomotion (Butler 2005). This paper reviews the anatomical and biomechanical considerations of the current foot balance model. It explores the relationship between the anatomical structures and the mechanical function within the foot and reviews the farriery considerations of our understanding of both static and dynamic foot balance models. It appears that the physics of load distribution casts doubt on the validity of theoretical foot balance model given the range of biomechanical variations within the population. Further investigation needs to be undertaken into the common morphometrics that might constitute a range of normal. 1 Introduction A fundamental principle of farriery is to achieve equilibrium of static and dynamic forces acting on internal structures within the foot and lower limb. External influences should be neutralised by internal forces with the form of the foot maintained so as not to inhibit its natural function. Farriery attempts to maintain equilibrium within the foot by trimming to achieve an ill-defined and subjective empirical interpretation of “Static Foot Balance” (Hickman & Humphrey 1987; Stashak 2002). This interpretation of foot balance is mostly derived from historical texts (Dollar & Wheatley 1898; Russell 1897; & Lungwitz 1891). Today’s modern domesticated horse is far from the forces of nature that historically shaped and controlled their development. Horses are more reliant than ever on the knowledge and skill of the hoof care professional with an understanding of the anatomy, physiology and function of the lower limb, foot and all its component parts. The composition, position and functional relationship of the component parts of the foot are so densely compacted that within the hoof capsule there is little room for manoeuvre. In nature shape and form of a structure relate directly to function. The hoof capsule is such an example of this concept. A horse’s natural protection against predators is “fright and flight” the hind quarters of the horse are a compact mass of large loco motor muscles which are designed primarily to propel the horse quickly forward. The front limbs are designed to primarily support the horse through impact, deceleration and loading during locomotion (Back & Clayton 2001). Movement is effected via neurological impulses causing the limbs to retract or protract. To minimise the energy required for this movement the limbs are as light weight as practical and are manoeuvred via a series of levers and pulleys. The pulleys are the joints, which are 2 held together with a complex array of ligaments. The levers are the tendons which, together with the ligaments, act like a coil spring releasing stored energy when movement is necessitated. In simple terms every time the limb is loaded the elasticated collagen fibres that make up the tendons and ligaments store energy which is released when the limb needs to be lifted and propelled forward. Anatomical Considerations The gross anatomy of the foot and limb is well documented. In farriery the foot of the horse is referred to as the keratinized hoof capsule and its contents. The hoof capsule is a continuation of modified epidermal tissue which forms a firm yet flexible protective layer surrounding the skeletal components at the distal extremity of the limb (Kempson. 1987). The primary functions of the hoof capsule and its associated structures are to absorb impact shock during locomotion, assist in the transfer of weight from the skeletal column and protect the underlying structures whilst providing grip during locomotion (Butler 2005). Each epidermal structure has a different density and hardness dependent upon its primary function and is produced by its own corresponding dermal layer and gains its strength and flexibility from its chemical composition and moisture content. The outer layer of hoof wall is rich in disulphides giving additional strength. The sole and frog are rich in sulfhydryl a group which gives these structures greater elasticity (Pollitt 1988) which gives flexibility. The average growth rate of 6-8mm per month (Stashak 2002) is said to be equal to the wear of the foot at the bearing border ground interface (Back and Clayton. 2001). The horn itself is composed of densely packed, longitudinally aligned, horn tubules which are generated from tiny projections of the dermis known as papillae (Fig 3). 3 These tubules are cemented together by intertubular horn cells which proliferate from germinative cells of the dermis between the papillae. The intertubular horn is formed at right angles to the tubular horn and gives the hoof wall a mechanically stable, multidirectional, fibre-reinforced composite (Bertram and Gosline, 1987). Interestingly hoof wall is stiffer and stronger at right angles to the direction of the tubules. This contradicts the usual assumption that the ground reaction force is transmitted proximally up the hoof wall parallel to the tubules. The hoof wall appears to be reinforced by the tubules but it is the intertubular material that accounts for most of its mechanical strength stiffness and fracture toughness. The tubules are three times more likely to fracture than intertubular horn (Leach, 1980; Bertram and Gosline 1986). Contrary to common misconception these tubules are not aligned randomly but appear to be arranged in 4 distinct zones and differing in “tubule density” from the inner most layers to the outer layer (Reilly et al. 1996). The highest tubular density is at the outermost layer (fig 4). Since the ground reaction force is transmitted proximally up the wall (Thomason et al 1992) the construction of the epidermal structures appears to be part of the mechanism that allows the transfer of impact load across the hoof wall from the rigid, high tubule density, outer wall to the more plastic, low tubule density, inner wall. The material properties of hoof are said to have plastic elastic characteristics (Reilly et al; 1996). These characteristics allow for deformation under stress and then return to original form following a limited period of strain. Maximum stress for prolonged periods of strain reduces the elastomeric property and the structures ability to return to its original form. Projecting from the inner wall are some 600-900 primary laminae each with 100-200 secondary epidermal laminae (Pollitt. 1988). The primary epidermal laminae are 4 produced by the dermis of the coronary corium. The secondary epidermal laminae are produced by a germinative layer of the epidermis of the laminar corium. The primary and secondary epidermal laminae interdigitate, dovetail, with the corresponding dermal lamellae. The dermal lamellae originate from the laminar corium surrounding the parietal surface of P3 and the lower border of the ungual cartilages. This relationship of interdigitation of laminae is thought to allow for the partial suspension of P3 within the hoof capsule and the transference of tensile forces radially from P3 (Reilly 2006) (Fig 5). As hoof wall continues to grow distally the primary epidermal laminae are allowed to slide past the secondary epidermal laminae. The process involves the remodelling of the epidermis around the proliferation of new cells. The basement membrane which surrounds the secondary dermal laminae is thought to release itself via tissue inhibiting desmosomes and demisomes (Pollitt.1998). At the solar border the sole and wall are separated by the white line. The white line is produced by epidermal primary lamellae and the terminal papillae at the distal fringe of P3. The white line is a flexible junction between both horny structures allowing for movement between the two structures during load bearing. The soles concavity combined with the shape of the frog are implicated not only as an anti-slip device (Butler 2005; Stashak 2002) but are said to play a major role in the anti-concussive mechanism. It is generally accepted that the horses mass is distributed through the limbs with 60% being supported by the fore limbs and 40% through the hind limbs (Butler, 2005:, Back & Clayton, 2001; Williams & Deacon 1999). Both hind and front limbs play a role in support and propulsion however the primary role of each differs. Front feet are generally larger and rounder with less concavity 5 to the soles to provide a greater surface to dissipate impact shock. Hind feet have a less acute dorsal hoof wall angle and a more concave sole. This configuration is best suited for grip and rapid propulsion, pushing as they dig into the ground. The frog is a wedged shaped mass of elasticated horn. Located at the basal surface of the solar margin it is occupies the space between the sole and bars uniting either side its longitudinal axis to form the collateral sulci. It extends palmadorsal from the heel bulbs approximately 2/3rd the length of the bearing surface (Ovnicek 1995). The so called true point of frog, where solar horn and frog horn merge, lies distal to the internal insertion of the deep digital flexor tendon (DDFT). Given its close relationship to the bars, and the composition and topography of the internal frog stay, it is more likely to act as an expansion mechanism for the heels during impact (Emery et al. 1977) whilst serving to protect the DDFT, digital cushion, distal sesamoidean bone and its associated bursae. Occupying the space between the large flexible ungual cartilages, which are attached to the palmar processes of P3 and distal to the DDFT, lies the digital cushion and venous plexus (Fig 2). The digital cushion is a large mass of highly elastic fibro fatty cartilage forming the heel bulbs. It is said that venous blood is flow is assisted by compression of the cartilages through the interactive mechanism of the frog and digital cushion during the impact and loading phases of the stride (Hickman & Humphreys 1987, Pollitt, 1988 and Butler, 2005). Bowker (1988) referred to this hydraulic compression of the vascular bundles as hemodynamic flow. Ratzlaff et al; (1985) and Bowker (1988) suggested that this action assists in the absorption of impact shock. Bowker argued that there is a complex inter-relationship between the ungual cartilages and the digital cushion. The medial projection on each ungual 6 cartilage is thrust upward by the bars on contact causing being transferred through the venous plexus dissipates high frequency energy waves reducing impact shock on the bone and ligaments of the foot. Bowker noted that horses with good foot conformation had more blood vessels in caudal aspect their feet than those with a history of foot problems. Bowker (1988) also noted that the digital cushion was made of fat and an elasticated fibro cartilaginous material. Fibro cartilage is made up, in part, by a protein called collagen. Collagen makes up the fibres found within tendons and ligaments and whose mechanical properties allow for the storage of energy. Physiological Considerations The relationship between the anatomical and mechanical function of the structures within the foot is integral to our understanding of static and dynamic foot balance. The biomechanical function of the individual anatomical structures within the foot are dependent on the ability of all of them to work in harmony for the good of the whole. This relationship is called a “mechanism”. The mechanisms within the foot enable the horse to travel at great speed over long distances and across varied terrain. As the foot makes contact with the ground up to 90% of the external shock is dissipated before it reaches P1 (Douglas et al 1998). A pluralistic approach to understanding the anti-concussive mechanism of the hoof recognises more than one ultimate principle. The foot’s internal and external structures combined exhibit three functional characteristics that allow for the dissipation of forces during operation of the foot mechanism described. (Barrey, 1990) 7 1. The absorption of impact and rapid deceleration forces through friction, resistance, and the elastic properties of structures that deform under load. 2. The dissipation of ground reaction force via pressure resistance to force and stress resistance through the material properties of the wall 3. Plastic structural characteristics that allow for the return to original form following deformation. During the stance phase the horse’s weight is transferred through the limb to the distal interphalangeal articulation. Because of the distal phalanx’s (P3) unique attachment to the hoof capsule via the laminar interdigitation, this weight is transferred to the wall radially as tensile forces (Reilly 2006). The dermal epidermal laminar interface acts partially as a suspensory apparatus for P3. The tensile forces are transferred distally along the hoof wall (Fig 5) and converted into pressure at the ground bearing border by ground reaction force vectors (GRFV). Both the sole and frog have a supporting role following initial contact and impact phases of the stride. At the first point of impact, this is usually heel first or flat the hoof is rapidly decelerated by the vertical landing forces. Heel first landing is accentuated at faster gaits (Back, et al, 1995). Horizontal movement is rapidly reduced to zero within milliseconds of impact. The shape and geometry of the foot changes as it comes under load. Following initial impact Bowker (1988) suggested a hemo-dynamic flow theory. He argued that there is a complex inter-relationship between the ungual cartilages and the digital cushion. At the point of impact the collateral cartilages are thrust upward by the heel buttresses and bars, causing negative pressure in the digital cushion draining blood from the front to the back of the foot, creating 8 hydrostatic cushioning. Simultaneously tendons and ligaments under load store excess energy from the vertical loading and fetlock extension. During the loading phases the proximal dorsal wall flattens and moves palmar distal, the heels expand (Fig 6) whilst the sole and frog flatten under load following the outward movement of the quarters (Douglas. et al. 1998, Lungwitz 1891). The relatively flexible laminar attachment at the heels compared with the toe allows greater expansion caudally. The frog descends with the sole until it contacts the ground. Known as the pressure theory (Hickman & Humphrey 1987; Butler 2005) this movement simultaneously compresses the digital cushion. Colles (1989) noted that in some horses with reduced frog pressure, such as those recently shod, the heel actually contracted under load. The Depression theory suggests that under the influence of weight during impact and loading that P3 is rotated palmardistally. This is more likely to be linked to hyperextension of the distal interphalangeal joint (DIPJ) caused by GRF vectors following heel first landing (Rooney 1969). This rapid deceleration of the foot by vertical landing forces and horizontal braking forces immediately post impact have been associated with the pathology of disease (Raddin, et al; 1972; Viitanen, et al; 2003). As the fetlock reaches the maximum extension required for the force applied the stored energy is used to accelerate retraction of the fetlock through to mid stance. Foot geometry and bearing borders are returned to their original position (Back & Clayton 2001). Theoretical Considerations in Static Foot Balance The English dictionary defines Balance: as ‘the harmony of design and proportion” or “stability produced by even distribution of weight on each side of the vertical axis”. Both definitions could easily be applied to the equine foot. Trimming and shoeing 9 are said to have marked effects on the performance and soundness of the equine athlete. Ideally, trimming optimizes the interaction between the hoof and ground during locomotion (Balch, et al 1998). Since the hoof is a three-dimensional structure, it should be balanced in both the (X) mediolateral and (Y) dorsopalmar planes whilst maintaining proportions through the proximodistal axis (Z) with its centre of mass (COM) remaining in equilibrium (Fig 8). For the purposes of biomechanical study the COM for the foot has been calculated from previous studies of cadavers (Springs & Leach; 1986). Body segments were weighed and calculated as a proportion of the overall body weight and then suspended at a point of balance. These points were then referenced to anatomical landmarks identifiable on the live horse for analysis purposes (Back & Clayton, 2001). Static foot balance refers to the alignment and spatial orientation of the foot and limb in the static mid stance position as a three dimensional object. All three dimensional objects have three axes and six co-ordinates. The dimensions of the foot are measured along these axes to the point where the X and Y axis intersect each other at along the longitudinal Z axis. This is an important concept in retaining static balance as it assumes equal weight / force at both coordinates of the axis. Dorsopalmar (lateral projection) The phalangeal axis of the adult horse is a natural conformation that can only be altered either by injury or surgery. However, the hoof axis in relation to the pastern axis can and often is, altered either by neglect on the part of the owner, or worse 10 still, by inadequate farriery practice. Textbooks tend to be misleading, all too often quoting the ideal front foot angle as being between 45º and 50º (Hickman & Humphrey 1987). (Turner 1988; 1992; Stashak 2002; and Butler 2005). stated that the heels should be parallel to the toe angle. More importantly both should present parallel to the internal dynamic structures the mid-line of the phalanges. A perpendicular line dropped from the centre of rotation of the DIPJ should bisect the ground bearing border equally (Colles 1983; 1989; Balch et al, 1997; O’ Grady & Poupard 2003). Dorsopalmar (Solar View) When viewed at its solar margin the following should be noted: The hoof wall is thickest and is most dense around the toe region, thinning as it wraps around the quarters arriving at the buttress to become the last weight bearing point of the foot. This is roughly adjacent to the widest point of the frog, before inverting on itself to form the bars which then terminate at the approximate centre of rotation of the coffin joint (Colles 1983; 1989; Balch et al, 1991; 1997; O’ Grady & Poupard 2003). The centre of weight distribution through the hoof capsule is said to be approximately 1cm palmar of the trimmed point of frog (Ovnicek 2003). A perpendicular line drawn from the buttress to the toe will intersect the medial and lateral optimum points of break-over (Duckett 1990; Caldwell 2001). Mediolateral The height of wall from coronary band to ground bearing border should be the same at any 2 opposite points (Russell 1897; Stashak 2002 and Butler 2005) with both the bearing border and coronary borders perpendicular to the longitudinal axis of the limb. 11 Discussion Farriery is an empirical craft with much of its knowledge and tradition handed down from one generation to the next. Much of what is quoted in standard farriery text regarding the hoof represent the mean approximation and should at best be regarded as “guidelines” to work within. It has long been accepted practice in farriery to relate the morphology of the hoof and its bearing border (BB) shape to an ideal form which is symmetrical around its longitudinal axis (Stashak, 2002; Butler, 2005). The reality of biological systems is that small-to-moderate asymmetries are present in the majority of structures. The BB shape is no exception. It has been well documented that external influences (Thomason 1998) can have an effect on the hoof’s shape. Leach and Zoerb (1983) noted that the percentage of total body weight acting through the forelimbs of adult horses is approximately 60% and as a result front feet are reportedly larger and rounder with less concavity to the soles to provide a greater surface to dissipate weight. According to Wolfe’s Law (1986) biologic systems such as hard and soft tissues become distorted in direct correlation to the amount of stress imposed upon them. Horn is said to posses both “elastic” and “plastic” deformation characteristics. The compressive forces (C) and the tensile components (T) in reaction with ground reaction force vectors (GRF) stress the horn over time until it reaches its yield strength (Hall 1953; 2003). At this point plastic deformation begins, for example collapsed heels. Once the process has begun, plastic deformation is not generally reversible. Hoof wall is thickest at the toe, the region of greatest friction, and thins gradually towards the heels with the medial quarter thinner than lateral (Pollitt, 12 1998). The wall is oblique to the direction of the GRF. The centre of pressure (COP) location and point of force (POF) trajectory (Wilson et al; 1988) are said to be influenced by external factors, such as conformation. By extending the moment arm the stress time line will influence the magnitude of force on the axial coordinates is likely to be a significant factor in both structural orientation and integrity and lead to permanent plastic deformation. The resultant increase in torque application from an increase in moment induces stress by moving the pressure towards the limbs longitudinal axis (Hall 1953). The resulting stress from pressure being applied externally to the cross section of the limb would seem to cause distortion of those soft tissue structures within the foot compromising both their integrity and biomechanical function. The physics of weight distribution and support suggest that each hoof capsule would take not only a different form around the bearing border but throughout its structure dependant on the forces applied to it. It would further indicate that pressure applied outside the hoof’s ability to absorb might restrict the dermal structures responsible for regeneration. 13 Conclusion It appears that the physics of load distribution cast doubt on the validity of theoretical foot balance model given the range of biomechanical variations within the population. Further investigation needs to be undertaken into the common morphometrics that might constitute a range of normal. The affects of farriery protocols on the structure, function, loading and movement of the equine foot are not fully understood. If we are to fully understand farriery’s role in lameness resolution clearly a more appropriate definition of the term foot balance needs to be recorded. 14 References Back, W., Schamhardt, H.C., Hartman, W. and Barneveld, A. (1995a) Kinematic differences between the distal portions of the forelimb and hindlimbs of horses at trot. Am. J. vet. Res. 56, 1522-1528. Balch, O.K., Ratzlaff, M., Hyde, M., Grant, B. and White, K. (1988) Correlation of equine forelimb hoof impact patterns to changes in the medio-lateral balance of the hoof. Anat. Histol. Embryol. 17, 361-362. Balch, O., White, K. and Butler, D. (1991) Factors involved in the balancing of Equine Hooves. J. AM. Vet. Med. Ass 198, 1980-1989 Balch, O.K., Butler, D. and Collier, A. (1997) Balancing the normal foot: hoof preparation, shoe fit and shoe modification in the performance horse. Equine Vet. Educ. 9, 143-154. Barrey, E. (1990) Investigation of the vertical force distribution in the equine forelimb with an instrumented horseboot. Equine vet. J., Suppl. 9, 35-38. Bertram, J.E.A. and Gosline, J.M. (1986). Fracture toughness design in horse hoof keratin. J. exp. Biol. 125, 29-47. Bertram, J.E.A. and Gosline, J.M. (1987). Functional design of horse hoof keratin: the modulation of mechanical properties through hydration effects. J. exp. Biol. 130,121-136. Butler K.D. (2005) The Principles of Horseshoeing 3. Butler Publishing. Maryville, Missouri Bowker, R. M., Van Wulfen, K. K., Springer, S. E., & Linder, K. E. (1998), Functional anatomy of the cartilage of the distal phalanx and digital cushion in the equine foot and a hemodynamic flow hypothesis of energy dissipation, Am.J.Vet.Res., vol. 59, no. 8, pp. 961-968. Caldwell. M. N. (2001) The Horses Foot: Function and Symmetry, Proceedings1st UK farriers Convention, Equine Vet. Jour. Publishing, 28-33 Colles, C. M. (1983), Interpreting radiographs 1: the foot, Equine Vet. J., vol. 15, no. 4, pp. 297-303. Colles, C. M. (1989). The relationship of frog pressure to heel expansion, Equine Vet. J., vol. 21, no. 1, pp. 13-16. Clayton H. M. (2004) The Dynamic Horses. Sport Horse Publications. Mason Dollar, J. A. W. (1898): A handbook of horseshoeing. Neill and Co, Edinburgh, Britain Douglas, J.E., Biddick, T.L., Thomasson, J. J. And Jofriet, J.C. (1998) Stress / strain behaviour of the equine laminar junction. J. Exp Biol. 201: 2287 - 2297 15 Emery, L. (1977) Horseshoeing Theory and Hoof Care, Lea & Febiger, Philadelphia, pp 65-68, 74-76. Hall, S. (1953, 2003) Basic Biomechanics. McGraw-Hill. New York. pp 70-74 Hickman J. and Humphrey M (1987) Hickman’s Farriery. J.A. Allen & Co. London Kempson. S.A. (1987). Scanning Electron Microscope Observations of Hoof Horn. Vet. Rec. 120. 568-570 Leach, D.H. and Zoerb, G.C. (1983) Mechanical properties of the Equine Hoof Wall Tissue. Am. J. of Vet. Res. 44, 2190-2194 Lungwitz, A. (1891). The changes in the form of the horse’s hoof under the action of the body-weight. J. comp. Path. Ther. 4, 191–211 O'Grady, S. E. & Poupard, D. A. (2003), Proper physiologic horseshoeing, Vet.Clin.North Am.Equine Pract., vol. 19, no. 2, pp. 333-351. Ovnicek G, Erfle JB, Peters DF. (1995). Wild horse hoof patterns offer a formula for preventing and treating lameness, in Proceedings. 41st Annu ConvAmAssoc Equine Practnr 1995; 258–263. Ovnicek, G. D., Page, B. T., & Trotter, G. W. 2003, Natural balance trimming and shoeing: its theory and application, Vet.Clin.North Am.Equine Pract., vol. 19, no. 2, pp. 353-77, vi. Pollitt. C. C. (1998). The Anatomy and Physiology of the Hoof Wall. Equine Vet. Educ. Manual 4, 3-10 Radin. E.L., Paul. I.L. and Rose. R.M (1972). The Role of Mechanical Factors in the Pathogenesis of Primary Osteoarthritis. Lancet. 519-522 Ratzlaff,M.H., Shindrel, R.M. and Debowes, R.M. (1985) Changes in Digital Venous Pressures of Horses Moving at Walk and Trot. Am. J. vet. Res. 46: 1545-1549 Reilly, J.D., Cottrell, D.F., Martin, R.J. and Cuddeford, D. (1996) Tubule Density in Equine Hoof Horn. Biomechanics 4, 23-36 Reilly, J. D. 2006. The Hoof Capsule in Curtis. S. A. Corrective Farriery; A Text Book of Remedial Farriery Volume 2 Newmarket Farriery Consultancy. pp. 343 – 376 Rooney J.R., (1969) Lameness of the forelimb, in: Mechanics of lameness in horses, The Williams and Wilkins Company, Baltimore, , pp. 114-196. Russell, W. (1897) Scientific Horseshoeing. Roberet Clark Co., Cincinnati, Ohio. P93-99 Stashak, T.S. (Ed.) (2002) Trimming and shoeing for balance and soundness. In: Adam’s Lameness in Horses, 5th edn. Lippincott Williams & Wilkins, Philadelphia. pp 1110-1113. 16 Thomason, J.J., Biewener, A.A. and Bertram, J.E.A. (1992) Surface strain on the equine hoof wall in vivo: implications for the material design and functional morphology of the wall. J. Exper. Biol. 166,145-165. Turner TA, Stork C. (1988) Hoof abnormalities and their relation to lameness, in Proceedings. 34th Annu Conv Am Assoc Equine Practnr pp ;293-297. Viitanen MJ, Wilson AM, McGuigan HR, Rogers KD, May SA. (2003) Effect of foot balance on the intra-articular pressure in the distal Interphalangeal joint in vitro. Equine Vet J. 2003 Mar;35(2):184Williams and Deacon (1999) No Foot No Horse. Kenilworth Press Ltd. Buckinghamshire. Wilson, A. M., Seelig, T.J., Shield, R.A. and Silverman, B.W. (1998). The Effects of Foot Imbalance on Point of Force Application in the Horse. Equine. Vet. J. 30: 540545 17 Illustrations Figure 1 to Figure 8 PROXIMAL PHALANX P1 MIDDLE PHALANX SDFT DDFT FIG. 2 P2 CDET CSL DIGITAL CUSHION PHALANX DS CORIUM OF FROG FRONTAL PLANE at section1 (Denoix. 2000), FROG CORONARY CORIUM DISTAL DERMAL LAMELLA P3 EPIDERMAL LAMELLA SOLAR CORIUM WALL SOLE WHITE LINE FIG.1. Sagittal section of the foot illustrating some of the important anatomical structures contained within the hoof capsule. The red dotted line is the frontal plane at section 1 (Denoix. 2000). 18 Coronary Coria P2 Collateral cartilages Coronary venous plexus Digital Cushion Frog stay Bars Frog PLANTER PALMER DISTAL OBLIQUE VIEW FIG.2 Transverse section through heel bulbs illustrates some of the important anatomical structures contained within the hoof capsule. In this plane the collateral cartilages, coronary plexus, coronary corium, digital cushion, frog stay and solar corium are all visible within the hoof capsule whilst externally the wall, frog, bars and collateral sulci are visible. 19 . Fig 3 Each dermal papillae fits a corresponding hole within the coronary groove and produces individual horn tubules. 20 P3 LC DL EL ZONE 4 ZONE 3 ZONE 2 ZONE 1 Fig 4 A transverse section through the hoof and internal structures. The section is taken from the region of mid toe. Illustrated are P3, the laminar corium (LC) attached to the parietal surface of P3 the primary dermal (DL) and epidermal (EL) lamellar interdigitation, (secondary lamellar are not visible at this magnification) the stratum internum and medium demonstrating the 4 zones of density (1, 2, 3 & 4). 21 TENSILE FORCES W LI P BEARING BORDER Fig 5 Weight of P3 (W) is transferred to the wall as tensile forces via the dermal epidermal laminar interface (LI). The LI acts as a suspensory apparatus for the distal phalanx (P3). The tensile forces are transferred distally along the hoof wall (Green Arrow) and converted into pressure (P) at the ground bearing border or the bearing border shoe interface (Budras et al. 1998) 22 Coronary Plexus Lateral Digital Vein Laminar Plexus Coronary Plexus Solar Plexus Fig 7 Lateral Venogram of a normal foot illustrates the complexity and magnitude of the venous return system of the equine foot. Clearly visible are the coronary, solar and laminar venous plexus. (www.thehorse.com) 23 z YAW y x x y PITCH ROLL z Fig 8 Diagrammatic representation of 3 dimensional static foot balance. X axis represents mediolateral coordinates viewed dorsopalmar / plantar and Y axis dorsopalmar viewed mediolateral whilst Z represents the proximodistal (longitudinal) axis of the foot. Movements around the dorsopalmar axis Y are referred to as “Roll” (indicated by the blue arrow). Movements around the mediolateral axis X are referred to as “Pitch” (indicated by the red arrows). Movements around the longitudinal axis Z are referred to as “Yaw” (indicated by the green arrow). 24