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Authors  Formulations 

Price, 1984 [8]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})(1 − ε) + a_{4}T_{j}Δε 
Prata and Platt, 1991 [14]  ${T}_{s}={a}_{0}+{a}_{1}\frac{{T}_{i}}{\mathit{\epsilon}}+{a}_{2}\frac{{T}_{j}}{\mathit{\epsilon}}+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Vidal, 1991 [15]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Ulivieri et al., 1992 [16]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(1 − ε) + a_{4}Δε 
Sobrino et al., 1993 [17]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})^{2} + a_{4}(1 − ε) + a_{5}Δε 
Sobrino et al., 1994 [18]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\mathit{\epsilon}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Coll et al., 1997 [19]  T_{s} = T_{i}+ a_{0} + a_{1}(T_{i} − T_{j}) + a_{2}(T_{i} − T_{j})^{2} + a_{3}(1 − ε) + a_{4}Δε 
Service  Price per order Flat rate Australia wide 
Delivery time^ After dispatch 


Saver Delivery (Tracked) via Australia post 
$5.99  210 days  
Express Delivery^{#~} (Tracked) via StarTrack Express 
$9.99  12 days 
Reddit user  Region  Rank  Stream Link 

/u/WeekndNA  NA  Challenger  Weeknd 
/u/herdisleah  NA  Diamond  Herdisleah 
/u/niko44  NA  Diamond  Niko44 
/u/bladesaslegs  NA  Diamond  BladesAsLegs 
/u/Roefel19  EUW  Diamond  Roefel 
/u/xMetix  EUW  Diamond  xMetix 
/u/Kirazono  NA  Diamond  Kirazono 
/u/Cyrex_  EUW  Diamond  Best Camille EU 
/u/VayneFTWayne  NA  Diamond  BestCamilleMid 
Parcel Weight  New Zealand  Hong Kong  US & Canada  United Kingdom 

Up to 1kg 
$30 
$35 
$40 
$45 
1.5kgs 
$35 
$45 
$50 
$60 
2kgs 
$40 
$50 
$60 
$70 
2.5kgs 
$45 
$60 
$70 
$80 
3kgs 
$50 
$65 
$75 
$90 
3.5kgs 
$55 
$75 
$85 
$100 
4kgs 
$60 
$80 
$95 
$105 
4.5kgs 
$65 
$85 
$100 
$115 
5kgs 
$70 
$95 
$110 
$125 
Authors  Formulations 

Price, 1984 [8]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})(1 − ε) + a_{4}T_{j}Δε 
Prata and Platt, 1991 [14]  ${T}_{s}={a}_{0}+{a}_{1}\frac{{T}_{i}}{\mathit{\epsilon}}+{a}_{2}\frac{{T}_{j}}{\mathit{\epsilon}}+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Vidal, 1991 [15]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Ulivieri et al., 1992 [16]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(1 − ε) + a_{4}Δε 
Sobrino et al., 1993 [17]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})^{2} + a_{4}(1 − ε) + a_{5}Δε 
Sobrino et al., 1994 [18]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\mathit{\epsilon}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Coll et al., 1997 [19]  T_{s} = T_{i}+ a_{0} + a_{1}(T_{i} − T_{j}) + a_{2}(T_{i} − T_{j})^{2} + a_{3}(1 − ε) + a_{4}Δε 
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