Matched set of golf clubs

Claim 2

A correlated set of more than two golf clubs in which the golf clubs have different lengths and each has a shaft representing an x axis with a grip having a preselected wristcock axis at one end and a club head having a center of mass at the other end, one of said clubs being selected as a master club having the desired characteristics for the golfer and all of the clubs but the master club having an added mass rigidly secured to the golf club at a point one half the distance between the wristcock axis of the grip and the center of mass of the clubhead, each of the clubs having the same overall mass despite their difference in length, the mass of the club head and the mass of the added mass rigidly secured at the midpoint being so computed that the first moment of each club in the correlated set is within fifteen one-hundredths of a percent (0.15%) of the first moment of each adjacent club in the set and the second moment of each club in the correlated set is within fifteen one-hundredths of a percent (0.15%) of the second moment of each adjacent club in the set, with the first and second moments of each club being measured about said wristcock axis.

Claim 3

The set of clubs of claim 1 in which the remaining clubs are correlated with said master club by adjustment of the values of the mass of the club head and the mass of the added mass of each of said remaining clubs.

Claim 4

The set of clubs of claim 2 in which a further mass is disposed in each of the clubs adjacent the wristcock axis and in which the values of the further mass, the added mass and the mass of the club head of each of the clubs are computed so as to provide for the same overall mass, the same first moment about the wristcock axis and the same second moment about said wristcock axis.

Claim 5

The set of clubs of claim 3 in which the relationship between the various masses is represented by the equation, M.sub.ci -M.sub.bi =A.sub.i +m.sub.i +μ.sub.i where μ i is the mass of the further mass disposed in club i at x=0, μ.sub.i =M.sub.ci -M.sub.bi -A.sub.i -m.sub.i M ci is the total mass of club i after matching, M bi is the total mass of club i before matching, A i is the change in mass of club i at x=L i , ##EQU10## m i is the mass of the added mass secured in club i at x=L i /2, ##EQU11## I cj is the second moment of the master club j after matching, ##EQU12## T cj is the period of a physical pendulum of the master club j measured about the wristcock axis of master club j (x=0) after matching g is the acceleration due to gravity, S cj is the first moment of the master club j after matching, S.sub.cj =M.sub.cj D.sub.cj M cj is the total mass of the master club j after matching, D cj is the distance from the wristcock axis (x=0) to the center of mass of the master club j along the shaft (x axis) after matching, I bi is the second moment of club i before matching ##EQU13## T bi is the period of a physical pendulum of club i measured about the wristcock axis of club i (x=0) before matching, S bi is the first moment of club i before matching S.sub.bi =M.sub.bi D.sub.bi D bi is the distance from the wristcock axis (x=0) to the center of mass of club i along the shaft (x axis) before matching, L i is the coordinate of the center of mass of the club head of club i along the shaft (x axis).

Claim 6

The set of clubs of claim 2 in which a further mass is disposed in each of the clubs adjacent the wristcock axis and in which the mass of the further mass, the mass of the added mass and the mass of the club head of each of the clubs are computed so as to provide the same overall mass and so that the first moment and second moment for each club in the correlated set are within fifteen one-hundredths of a percent (0.15%) of the respective moments of each adjacent club in the set.

Claim 7

The set of clubs of claim 5 in which the relationship between the various masses is represented by the equation M.sub.ci -M.sub.bi =A.sub.i +m.sub.i +μ.sub.i where μ.sub.i =M.sub.ci -M.sub.bi -A.sub.i -m.sub.i M ci is the total mass of club i after matching, M bi is the total mass of club i before matching, A i is the change in mass of club i at x=L i ##EQU14## m i is the mass of the added mass secured in club i at x=L i /2, ##EQU15## I cj is the second moment of the master club j after matching, ##EQU16## T cj is the period of a physical pendulum of the master club j measured about the wristcock axis of master club j (x=0) after matching, g is the acceleration due to gravity, S cj is the first moment of the master club j after matching, S.sub.cj =M.sub.cj D.sub.cj M cj is the total mass of the master club j after matching, D cj is the distance from the wristcock axis (x=0) to the center of mass of the master club j along the shaft (x axis) after matching, I bi is the second moment of club i before matching, ##EQU17## T bi is the period of a physical pendulum of club i measured about the wristcock axis of club i (x=0) before matching, S bi is the first moment of club i before matching, S.sub.bi =M.sub.bi D.sub.bi D bi is the distance from the wristcock axis (x=0) to the center of mass of club i along the shaft (x axis) before matching, L i is the coordinate of the center of mass of the club head of club i along the shaft (x axis), M.sub.ci =(1+r.sub.i)M.sub.cj S.sub.ci =(1+q.sub.i)S.sub.cj I.sub.ci =(1+p.sub.i)I.sub.cj r i is a relaxing factor for total mass, q i is a relaxing factor for first moment, p i is a relaxing factor for second moment.

Claim 8

The set of clubs of claim 6 in which relaxing factors r i , q i , and p i are so selected such that μ i =0.0.

Claim 11

The method of claim 8 in which there is provided the further step of correlating the remaining clubs of the set with said master club by adjustment of the values of the mass of the club head and the mass of the added mass in each of said remaining clubs.

Claim 12

The method of claim 9 in which there is provided the further steps of (a) disposing a further mass in each of the clubs adjacent the wristcock axis, and (b) computing for each club the mass of the further mass, the mass of the club head, and the mass of the added mass rigidly secured at the midpoint so that each of the clubs despite their difference in length, has substantially the same overall mass and the first moment about said wristcock axis and second moment about said wristcock axis for each club in the correlated set are within fifteen one-hundredths of a percent (0.15%) of the respective moments of each adjacent club in the set.

Claim 13

The method of claim 10 in which there is provided the further step of defining the relationship between the various masses by the equation M.sub.ci -M.sub.bi =A.sub.i +m.sub.i +μ.sub.i where .sub.i =M.sub.ci -M.sub.bi -A.sub.i -m.sub.i M ci is the total mass of club i after matching, M bi is the total mass of club i before matching, A i is the change in mass of club i at x=L i ##EQU18## m i is the mass of the added mass secured in club i at x=L i /2, ##EQU19## I cj is the second moment of the master club j after matching, ##EQU20## T cj is the period of a physical pendulum of the master club j measured about the wristcock axis of master club j (x=0) after matching, g is the acceleration due to gravity, S cj is the first moment of the master club j after matching, S.sub.cj =M.sub.cj D.sub.cj M cj is the total mass of the master club j after matching, D cj is the distance from the wristcock axis (x=0) to the center of mass of the master club j along the shaft (x axis) after matching, I bi is the second moment of club i before matching, ##EQU21## T bi is the period of a physical pendulum of club i measured about the wristcock axis of club i (x=0) before matching, S bi is the first moment of club i before matching, S.sub.bi =M.sub.bi D.sub.bi D bi is the distance from the wristcock axis (x=0) to the center of mass of club i along the shaft (x axis) before matching, L i is the coordinate of the center of mass of the club head of club i along the shaft (x axis), M.sub.ci =(1+r.sub.i)M.sub.cj S.sub.ci =(1+q.sub.i)S.sub.cj I.sub.ci =(1+p.sub.i)I.sub.cj r i is a relaxing factor for total mass, q i is a relaxing factor for first moment, p i is a relaxing factor for second moment.

Claim 14

The method of claim 11 in which there is provided the further step of selecting the values for the relaxing factors r i , q i , and p i such that μ i =0.0.

Claim 15

The method of claim 9 in which there is provided the further steps of (a) disposing a further mass in each of the clubs adjacent the wristcock axis, and (b) computing for each club the mass of the further mass, the mass of the club head, and the mass of the added mass rigidly secured at the midpoint so that each of the clubs, despite their difference in length, has the same overall mass, the same first moment about the wristcock axis, and the same second moment about said wristcock axis.

Claim 16

The method of claim 13 in which there is provided the further step of defining the relationship between the various masses by the equation M.sub.ci -M.sub.bi =A.sub.i +m.sub.i +μ.sub.i where μ i is the mass of the further mass disposed in club i at x=0, μ.sub.i =M.sub.ci -M.sub.bi -A.sub.i -m.sub.i, M ci is the total mass of club i after matching, M bi is the total mass of club i before matching, A i is the change in mass of club i at x=L i ##EQU22## m i is the mass of the added mass secured in club i at x=L i /2, ##EQU23## S cj is the second moment of the master club j after matching, ##EQU24## T cj is the period of a physical pendulum of the master club j measured about the wristcock axis of master club j (x=0) after matching g is the acceleration due to gravity, S cj is the first moment of the master club j after matching, S.sub.cj =M.sub.cj D.sub.cj M cj is the total mass of the master club j after matching, D cj is the distance from the wristcock axis (x=0) to the center of mass of the master club j along the shaft (x axis) after matching, I bi is the second moment of club i before matching ##EQU25## T bi is the period of a physical pendulum of club i measured about the wristcock axis of club i (x=0) before matching, S bi is the first moment of club i before matching, S.sub.bi =M.sub.bi D.sub.bi D bi is the distance from the wristcock axis (x=0) to the center of mass of club i along the shaft (x axis) before matching, L i is the coordinate of the center of mass of the club head of club i along the shaft (x axis).