]> Jasper's Sandbox

Jasper's Sandbox

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Q = 1.1 Q_{D} + Q_{L} + Q_{S} \pm Q_{E}

Q = 0.9 Q_{D} \pm Q_{E}

V = C_{s} W

C_{s} = 0.67 (\frac{1.2 A_{v} S}{R T^{2/3}}) = \frac{0.80 A_{v} S}{R T^{2/3}}

C_{s} = 0.85 (\frac{2.5 A_{a}}{R}) = \frac{2.12 A_{a}}{R}

T_{a} = C_{T} h_{n}^{3/4}

T_{a} = \frac{0.05 h_{n}}{\sqrt{L}}

T = 2 π \sqrt{\frac{\sum (w_{i} d_{i}^{2})}{g \sum (f_{i} d_{i})}}

F_{x} = C_{v x} V

C_{vx} = \frac{w_{x} h_{x}^{k}}{\sum_{i=1}^{n} w_{i} h_{i}^{k}}

F_{p} = 0.67 (A_{V} C_{C} W_{C})

V_{j} = (\frac{n + j}{n + 1}) (\frac{W_{j}}{W}) 1.2 V

DR = (\frac{k_{b} + k_{c}}{K_{b} . K_{c}}) (\frac{h}{12 E}) V_{c} C_{d}

v_{avg} = (\frac{n_{c}}{N_{c} - n_{f}}) (\frac{V_{j}}{A_{c}})

v_{avg} = \frac{V_{j}}{A_{w}}

f_{br} = (\frac{V_{j}}{s N_{br}}) (\frac{L_{br}}{A_{br}})

Q \leq C

S_{d, C} = \nabla_{C} . H_{R} . \frac{α_{2}}{α_{3}}

OLF = (0.00007) (GLA) + 25

A_{a} = {A_{t} + [A_{t} x I_{f}] + [A_{t} x I_{s}]}

A_{e} = A + (A_{f} x F_{eo})

(\frac{A_{p}}{a_{p}}) + (\frac{A_{u}}{a_{u}}) \leq 1

t + (\frac{4 t}{s} - 1) (t_{e} - t)

t + (\frac{4 t}{s} - 1) (t_{e} - t)

T_{ea} = T_{e} + T_{ef}

T_{e} = \frac{V_{n}}{LH}

R = {(R_{n}^{0.59} + pl)}^{1.7}

R = {(R_{n}^{0.59} + pl)}^{1.7}

R = 130 {[\frac{h (\frac{W'}{D})}{2}]}^{0.75}

R = [C_{1} (\frac{W}{D}) + C_{2}] h

R = R_{o} (1 + {0.03}_{m})

H = 0.11 W + (\frac{p_{c} c_{c}}{144}) (b_{f} d - A_{s})

R = 0.17 {(\frac{W}{D})}^{0.7} + [0.285 (\frac{T_{e}^{1.6}}{K^{0.2}})] [1.0 + 42.7 {\frac{(\frac{A_{s}}{d_{m} T_{e}})}{(0.25 p + T_{e})}}^{0.8}]

h_{2} = h_{1} \frac{[(\frac{W_{1}}{D_{1}}) + 0.60]}{[(\frac{W_{2}}{D_{2}}) + 0.60]}

F = F_{dc} + \frac{K (WAΔP)}{2 (W - d)}

v = 217.2 {[\frac{h (T_{f} - T_{o})}{(T_{f} + 460)}]}^{\frac{1}{2}}

T_{s} = (\frac{Q_{c}}{mc}) + (T_{a})

C = A x 300

1.4 (D + F)

0.9 D + \frac{E}{1.4}

R = 0.08 (A - 150)

R = 23.1 (1 + \frac{D}{L_{o}})

L_{r} = L_{o} R_{1} R_{2}

V_{fm} = \frac{(V_{35} - 10.5)}{1.05}

P_{net} = q_{s} K_{z} C_{net} {I K_{zt}}

R = 5.2 (d_{s} + d_{h})

\bar{N} = \frac{\sum_{i = 1}^{n} d_{i}}{\sum_{i = 1}^{n} \frac{d_{i}}{N_{i}}}

{\bar{N}}_{ch} = \frac{d_{s}}{\sum_{i = 1}^{m} \frac{d_{i}}{N_{i}}}

\sum_{i = 1}^{m} d_{i} = d_{s}

{\bar{s}}_{u} = \frac{d_{c}}{\sum_{i = 1}^{k} \frac{d_{i}}{s_{ui}}}

\sum_{i = 1}^{k} d_{i} = d_{c}

δ_{M} = \frac{C_{d} δ_{max}}{I}

δ_{MT} = \sqrt{{(δ_{M 1})}^{2} + {(δ_{M 2})}^{2}}

T_{T} = wLS \leq α_{T} S

T_{p} = 200 w \leq β_{T}

θ = \frac{P_{x} Δ I}{V_{x} h_{sx} C_{d}}

0.9 D + \frac{E}{1.4}

R = 0.08 (A - 150)

R = 23.1 (1 + \frac{D}{L_{o}})

L_{r} = L_{0} R_{1} R_{2}

V_{fm} = \frac{(V_{3 S} - 10.5)}{1.05}

P_{net} = q_{s} K_{z} C_{net} [I K_{zt}]

R = 5.2 (d_{s} + d_{h})

S_{MS} = F_{a} S_{s}

S_{M 1} = F_{v} S_{1}

S_{DS} = \frac{2}{3} S_{MS}

S_{D 1} = \frac{2}{3} S_{M 1}

{\bar{v}}_{s} = \frac{\sum_{i = 1}^{n} d_{i}}{\sum_{i = 1}^{n} \frac{d_{i}}{v_{si}}}

\bar{N} = \frac{\sum_{i = 1}^{n} d_{i}}{\sum_{i = 1}^{n} \frac{d_{i}}{N_{i}}}

{\bar{N}}_{ch} = \frac{d_{s}}{\sum_{i = 1}^{m} \frac{d_{i}}{N_{i}}}

\sum_{i = 1}^{m} d_{i} = d_{s}

{\bar{s}}_{u} = \frac{d_{c}}{\sum_{i = 1}^{k} \frac{d_{i}}{s_{ui}}}

\sum_{i = 1}^{k} d_{i} = d_{c}

δ_{M} = \frac{C_{d} δ_{max}}{I}

δ_{M} = C_{d} δ_{max}

δ_{MT} = \sqrt{{(δ_{M 1})}^{2} + {(δ_{M 2})}^{2}}

T_{T} = w L S \leq α_{T} S

T_{p} = 200 w \leq β_{T}

θ = \frac{P_{x} Δ I}{V_{x} h_{sx} C_{d}}

d = 0.5 A {1 + {[1 + (\frac{4.36 h}{A})]}^{\frac{1}{2}}}

d = \sqrt{\frac{4.25 Ph}{S_{3} b}}

d = \sqrt{\frac{4.25 M_{8}}{S_{3} b}}

P_{a} = 0.5 P_{u}

f'

σ_{b} = \frac{8 F_{b}^{'}}{t^{2}} \frac{d^{2}}{6}

σ_{Δ} = \frac{384 Δ E^{'}}{5 l^{4}} \frac{d^{3}}{12}

σ_{b} = \frac{8 F_{b}^{'}}{l^{2}} \frac{d^{2}}{6}

σ_{Δ} = \frac{185 Δ E^{'}}{l^{4}} \frac{d^{3}}{12}

σ_{b} = \frac{8 F_{b}^{'}}{l^{2}} \frac{d^{2}}{6}

σ_{Δ} = \frac{131 Δ E^{'}}{l^{4}} \frac{d^{3}}{12}

σ_{b} = \frac{20 F_{b}^{'}}{{3 l}^{2}} \frac{d^{2}}{6}

σ_{Δ} = \frac{105 Δ E^{'}}{l^{4}} \frac{d^{3}}{12}

σ_{b} = \frac{20 F_{b}^{'}}{3 l^{2}} \frac{d^{2}}{6}

σ_{Δ} = \frac{100 Δ E^{'}}{l^{4}} \frac{d^{3}}{12}

σ_{b} = \frac{20 F_{b}^{'}}{3 l^{2}} \frac{d^{2}}{6}

σ_{Δ} = \frac{100 Δ E^{'}}{l^{4}} \frac{d^{3}}{12}

σ_{b} = \frac{20 F_{b}^{'}}{3 l^{2}} \frac{d^{2}}{6}

σ_{Δ} = \frac{116 Δ E^{'}}{l^{4}} \frac{d^{3}}{12}

F_{gw} \leq F_{ga}

F_{g} = W_{o} - D

F_{g} = W_{i} + D + 0.5 S

F_{g} = {0.5 W}_{i} + D + S

F_{g} \leq F_{ga}

F_{gw} < 0.5 F_{ge}

F_{g} < 0.5 F_{ge}

F_{g} < 0.3 F_{ge}

F_{gw} < 0.1 F_{ge}

F_{g} < 0.1 F_{ge}

F_{g} < 0.6 F_{ge}

F_{g} < 0.5 F_{ge}

F_{gi} \leq P G_{Pos}

F_{go} \leq P G_{Neg}

S_{a} = (S_{XS}) (0.4 + \frac{3 T}{T_{0}})

S_{a} = S_{XS}

S_{a} = \frac{S_{X 1}}{T}

T_{0} = \frac{S_{X 1}}{S_{XS}}

DS A_{d} = S_{XS} ((\frac{5}{B_{S}} - 2) \frac{T}{T_{0}} + 0.4)

DS A_{d} = \frac{DSA}{B_{S}}

DS A_{d} = \frac{S_{1}}{(B_{1} T)}

V_{w} = V_{h} {(\frac{33}{h})}^{\frac{1}{7}}

V_{t = 30 \sec} = \frac{V_{t}}{c_{t}}

V_{w} = 1.10 V_{L}

V_{c}^{2} = \frac{1}{T \int_{o}^{T} {(v_{c})}^{2} ds}

E_{vessel} = \frac{1}{2} . \frac{W}{g} . V_{n}^{2}

E_{fender} = C_{b} . C_{m} . E_{vessel}

C_{b} = C_{e} . C_{g} . C_{d} . C_{c}

DT = 1.25 DWT (\frac{d_{actual}}{d_{max}})

C_{e} = \frac{k^{2}}{a^{2} + k^{2}}

C_{m} = 1 + 2 x \frac{d_{actual}}{B}

F_{d} = 1.2 x MBL x [1 + 0.75 (n - 1)]

T = 2 π \sqrt{\frac{m}{k}}

Δ_{d} = S_{A} \frac{T^{2}}{4 π^{2}}

S_{D} = \frac{T^{2}}{4 π^{2}} S_{A}

k_{e} = \frac{4 π^{2}}{T_{d}^{2}} M

F_{u} = k_{e} Δ_{d}

Δ_{d} = \sqrt{Δ_{x}^{2} + Δ_{y}^{2}}

Δ_{x} = Δ_{xy} + 0.3 Δ_{xx}

Δ_{x} = 0.3 Δ_{xy} + Δ_{xx}

\frac{V}{W} \geq 4 \frac{Δ_{d}}{H}

V_{sk} = 1.5 (e / L_{t}) V_{Δ T}

V_{crit} = 1.5 + \frac{L - 2 B}{500 - 2 B} 4.5 (knots)

L_{c} = 2 r \sin α

F = μN

SF = \frac{CRR}{CSR}

\frac{E_{S} I_{S} + 0.25 E_{C} I_{C}}{(E_{S} I_{S} + E_{C} I_{C})}

\frac{e}{h} \leq 0.10

L_{p} = 0.08 L + 0.15 f_{ye} d_{bl} \geq 0.3 f_{ye} d_{bl}

L_{p} = 0.3 f_{ye} d_{bl}

\frac{K D^{6}}{[D^{*}] E I_{e}}

θ_{p} = L_{p} φ_{p} = (φ_{m} - φ_{y})

φ_{m} = \frac{ε_{cm}}{C_{u}}

φ_{y} = \frac{M_{y}}{E I_{c}}

ε_{cu} = 0.005

ε_{cu} = 0.004 + \frac{(1.4 ρ_{s} f_{yh} ε_{sm})}{f_{cc}^{'}} \geq 0.005 ε_{cu} \leq 0.025

V_{design} = 1.4 V_{max}

V_{design} = 1.25 V_{max}

V_{n} = V_{c} + V_{s} + V_{p}

V_{design} \leq 0.85 V_{n}

V_{c} = k \sqrt{f_{c}^{'} A_{e}}

μ_{φ} = \frac{φ}{φ_{y}}

V_{s} = \frac{\frac{π}{2} A_{sp} f_{yh} (D_{p} - c - c_{o}) \cot (θ)}{s}

V_{s} = \frac{A_{h} f_{yh} (D_{p} - c - c_{o}) \cot (θ)}{s}

V_{p} = Φ (N_{u} + F_{p}) \tan α

V_{pile} = (\frac{π}{2}) t f_{y, pile} (D_{p} - c - c_{o}) \cot θ

v_{j} = \frac{0.9 M_{p}}{\sqrt{2} l_{dv} D_{p}^{2}}

p_{t} = \frac{- f_{a}}{2} + \sqrt{{(\frac{f_{a}}{2})}^{2} + v_{j}^{2}}

f_{a} = \frac{N}{{(D_{p} + h_{d})}^{2}}

p_{t} > 5.0 \sqrt{f_{c}^{'}}

p_{t} = 5.0 \sqrt{f_{c}^{'}}

v_{j} = \sqrt{p_{t (p_{t} - f_{a})}}

M_{c} = (\frac{1}{. 90}) \sqrt{2} v_{j} l_{dv} D_{p}^{2} \leq M_{p}

M_{c, r} = 2 A_{s} f_{y} (h_{d} - d_{c}) + N (\frac{D_{p}}{2} - d_{c})

A_{s, deckbottom} = 0.5 . A_{s}

φ_{y}^{'} = \frac{φ_{y} M_{c}}{M_{n}}

φ_{p} = \frac{0.04}{L_{p}}

φ_{u}^{'} = φ_{p} + \frac{φ_{y} M_{c, r}}{M_{n}}

l_{dc} \geq \frac{0.025 . d_{b} . f_{ye}}{\sqrt{f_{c}^{'}}}

f_{ye, r} = f_{ye} + \frac{l_{d}}{l_{dc}}

Δ = \frac{M L^{2}}{3 EI}

φ_{a} = \frac{ε_{a}}{c_{u}}

φ = \frac{M}{EI}

M = \frac{2 ε_{a}}{D_{p}} EI

Δ = \frac{2 ε_{a} L^{2}}{3 D_{p}}

V_{demand} = 1.2 V_{max}

τ_{max} = \frac{10}{9} \frac{V_{demand}}{π . r^{2}}

τ_{capacity} = 2.8 τ_{design}

V_{F} = Q_{c} x Δ t x (\frac{1}{3,600})

A_{a} = (1 + 1_{f} + 1_{s}) x A_{t}

VO = PV x CF

y = \frac{- 3 x}{2} + 55

P_{t} = P_{\sup} - P L_{svc} - P L_{m} - P L_{d} - P L_{e} - P_{sp}

TL \geq R_{1} . R_{2} . R_{3} . UR

R_{3} \leq \frac{TL}{R_{1} . R_{2} . UR}

Q = 181.6 \sqrt{\frac{D^{5} . (P_{1}^{2} + P_{2}^{2}) . Y}{C_{r} . fba . L}}

= 2237 D^{2.623} {[\frac{(P_{1}^{2} - P_{2}^{2}) . Y}{C_{r} . L}]}^{0.541}

Q = 1873 \sqrt{\frac{D^{5} . Δ H}{C_{r} . fba . L}}

= 2313 D^{2.623} {(\frac{Δ H}{C_{r} . L})}^{0.541}

= 0.00354 ST {(\frac{Z}{S})}^{0.152}

C = A x B

I = \sqrt{\frac{TC - (TA + Δ TD)}{RDC (1 + YC) RCA}}

I_{2} = I_{1} \sqrt{\frac{TC - T A_{2} - Δ TD}{TC - T A_{1} - Δ TD}}

I = \sqrt{\frac{TC - (TA + Δ TD)}{RDC (1 + YC) RCA}}

n = \frac{ca}{wa}

n = \frac{ca}{wa}

I_{leff} = \sqrt{I_{1}^{2} X + I_{0}^{2} (1 - x)}

A_{2} = \sqrt{\frac{(0.5) (24)}{12}} x 20 (0.7)

\frac{V_{co}}{V_{a}} = \frac{M_{co}}{M_{air}} = \frac{M_{co}}{M_{o_{2}}} = \frac{M_{o_{2}}}{M_{o_{2}}^{0}} \frac{M_{o_{2}}^{0}}{M_{A}} = \frac{X_{co} M_{o_{2}}}{X_{o_{2}} M_{o_{2}}^{0}} X_{o_{2}}^{0}

\frac{M_{co}}{M_{o_{2}}} = \frac{X_{co}}{X_{o_{2}}}

M_{o_{2}} = M_{o_{2}}^{0} \frac{(\frac{X_{o_{2}}}{X_{o_{2}}^{0}}) - X_{o_{2}}}{1 - X_{o_{2}} - X_{{co}_{2}} - X_{co}}

\dot{Q} = [φ - \frac{0.345 ((1 - φ) 2)}{(\frac{X_{co}}{X_{o_{2}}})}] 17.4 X_{o_{2}}^{0} V_{A} (MW)

\dot{Q}

O_{u} = [1 - {(\frac{T_{s}}{T_{c}})}^{\frac{1}{d}}] 100

O_{d} = [1 - (\frac{T_{s}}{T_{c}})] 100

O_{d} = [1 - {[1 - (\frac{O_{u}}{100})]}^{d}] 100

TE (\frac{R}{r}) (234.5 + t) - 234.5

V_{bz} = R_{p} P_{z} + R_{a} A_{z}

V_{oz} = \frac{V_{bz}}{E_{z}}

V_{ot} = V_{oz}

V_{ot} = V_{oz}

V_{ot} = \sum_{all zones} V_{oz}

Z_{p} = \frac{V_{oz}}{V_{pz}}

V_{ou} = D \sum_{all zones} R_{p} P_{z} + \sum_{all zones} R_{a} A_{z}

D = \frac{P_{s}}{\sum_{all zones} P_{z}}

V_{ot} = \frac{V_{ou}}{E_{v}}

Q = 2610 A_{e} \sqrt{Δ p}

Q = 0.5 A_{gf}

Q = \frac{\sum q}{1.08 Δ T}

Q = 100 \sqrt{G}

V_{1} > (W_{1} - \frac{(V_{2} - V_{1})}{V_{gt}}) V_{gc}

C = f D L

C = 0.8 P_{1} d^{2}

d = 1.12 \sqrt{\frac{C}{P^{1}}}

L = \frac{9 P^{2} d^{5}}{16 C^{2}}

D = \frac{Q^{0.381}}{19.17 {(\frac{Δ H}{Cr x L})}^{0.206}}

D = \frac{Q^{0.381}}{18.93 {[\frac{(P_{1}^{2} - p_{2}^{2}) . Y}{Cr x L}]}^{}}