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Equation (4.7.17):
N sub f = N(S) = left { lpile{( {S sub 1}over S ) sup m S > S sub 0 above inf S < S sub 0}

Equation (4.7.18):
DELTA eta = n ( X over{S sub 1}) sup m {GAMMA (a + m over h ; ({S sub
0}over X ) sup h )} over{GAMMA (a)}

Equation (4.7.19): eta = n ( D over{S sub 1}) sup m {GAMMA (d + m over k ; ({S sub 0}over D ) sup j )} over{GAMMA (d)}

Equation (4.7.20): eta = sum n(C) over N(C)

Equation (4.7.21):
N sub f = N(S) = left { lpile{({S sub 1} over S ) sup m S > S sub 0 above ({S' sub 1}over S ) sup m' S < S sub 0}

Equation (4.7.22): m' mark = m + 2

Equation (4.7.23):
N(S sub 0 ) lineup = 1 cdot 10 sup 7

Equation (4.7.24):
S sub 0 lineup = 10 sup{- 7 over m} S sub 1 = S' sub 1 10 sup{- 7 over m+2}

Equation (4.7.25):
S' sub 1 lineup = S sub 1 ( {S sub 1}over{S sub 0}) sup{- 2 over m+2} = S sub 0 ({S sub 1}over{S sub 0} ) sup{m over m+2} = S sub 1 10 sup{- 14 over m(m+2)}

Equation (4.7.26): eta = n "{" ( D over{S sub 1}) sup m {GAMMA (d + m over k ; ({S sub 0}over
D ) sup k )} over{GAMMA (d)} +
( D over{S' sub 1}) sup m+2 {gamma (d + m+2 over k ; ({S sub 0}over D ) sup k )} over{GAMMA (d)} "}"

Equation (4.7.27):
N sub f = N(S) = left { lpile{N sub 0 e sup{- S over B} above inf } for lpile{S (>= S sub 0 above S ( 0

Equation (4.7.65): u = n{DELTA eta}bar - 1 over h psi (a) = n xi bar + sqrt n sigma sub xi
{psi (a)}over{sqrt{psi ' (a)}}

Equation (4.7.66): a mark approx n over{lambda sup 2}

Equation (4.7.67): h lineup approx - n lambda over{sigma sub xi}

Equation (4.7.68): u lineup approx n "{" xi bar - {sigma sub xi}over lambda ln [ n over{lambda sup 2a} ] "}"

Equation (4.7.69): (xxx) rho ( eta , t) = 1 over sqrt{2 pi n} 1 over{sigma sub xi} e sup{- {( eta - n xi bar ) sup 2}over{2 n sigma sub xi sup 2}} t = n T

Equation (4.7.70): j = eta over L roman or eta = j L

Equation (4.7.71):
Pr ( eta = j L ) = Pr (j; n) = ( cpile{n above j} ) p sup j (1 - p) sup n-j n (>= j

Equation (4.7.72): p = (1 - p) = 1 over 2

Equation (4.7.73):
Pr(j; n) = ( cpile{n above j} ) 1 over{2 sup n}

Equation (4.7.74):
{eta sub n}bar = L n p and sigma sub eta sup 2 = L sup 2 n p (1 - p)

Equation (4.7.75):
{sigma sub eta}over{eta bar} = 1 over sqrt n sqrt{{1 - p}over p}

Equation (4.7.76):
L = xi bar (1 + nu sup 2 ) and p = 1 over{1 + nu sup 2}

Equation (4.7.77):
L = {M sub 2 ( xi )}over{M sub 1 ( xi )} and p = {M sub 1 ( xi ) sup
2}over{M sub 2 ( xi )}

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