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Cruising Velocity and Operational Transit Cost Optimization

Core Definition

Cruising Velocity and Operational Transit Cost Optimization models the financial and energetic trade-offs inherent in moving physical vehicles across a fixed distance DD. Because elapsed travel time scales inversely with velocity (t=D/vt = D/v), fixed-rate temporal costs (e.g., driver wages, vehicle leasing, hotel overhead) decrease monotonically with speed as Ct∝1/vC_t \propto 1/v. Conversely, aerodynamic and hydrodynamic drag forces scale non-linearly with velocity (Fdrag∝v2  ⟹  Pdrag∝v3F_{\text{drag}} \propto v^2 \implies P_{\text{drag}} \propto v^3), causing energetic fuel/battery costs per mile to increase as Cf∝vC_f \propto v or v2v^2. Calculus identifies the unique velocity that balances these conflicting operational pressures.


Concept Explanation

1. Mathematical Formulation of the Total Trip Cost

For a transportation system traveling a fixed transit distance DD at a steady cruising speed vv:

  1. Transit Time:
    t(v)=Dvt(v) = \frac{D}{v}
  2. Time-Dependent Operating Cost: Let ww denote the hourly cost of labor, driver wages, vehicle depreciation, and auxiliary life support systems ($/hour\$ / \text{hour}). The total temporal expenditure is:
    Ctime(v)=w⋅t(v)=wDvC_{\text{time}}(v) = w \cdot t(v) = \frac{w D}{v}
  3. Speed-Dependent Energy/Fuel Cost: Aerodynamic drag force is given by FD=12ρCDAv2F_D = \frac{1}{2}\rho C_D A v^2. The mechanical power required to overcome drag is PD=FD⋅v∝v3P_D = F_D \cdot v \propto v^3.
    The fuel or electrical energy consumed per unit time is proportional to power, meaning hourly fuel cost is modeled by:
    Rfuel(v)=kvn(where typically n=2 or 3)R_{\text{fuel}}(v) = k v^n \quad (\text{where typically } n = 2 \text{ or } 3)
    Multiplying hourly fuel rate by total transit time gives total fuel cost over the trip:
    Cfuel(v)=Rfuel(v)⋅t(v)=(kvn)⋅(Dv)=kDvn−1C_{\text{fuel}}(v) = R_{\text{fuel}}(v) \cdot t(v) = (k v^n) \cdot \left(\frac{D}{v}\right) = k D v^{n-1}
  4. Total Objective Function:
    C(v)=Ctime(v)+Cfuel(v)=wDv+kDvn−1C(v) = C_{\text{time}}(v) + C_{\text{fuel}}(v) = \frac{w D}{v} + k D v^{n-1}

For quadratic hourly fuel models (n=2n = 2, common in commercial truck logistics):

C(v)=Av+Bvwhere A=wD,  B=kDC(v) = \frac{A}{v} + B v \quad \text{where } A = w D, \; B = k D

For cubic hourly fuel models (n=3n = 3, common in marine naval architecture):

C(v)=Av+Bv2where A=wD,  B=kDC(v) = \frac{A}{v} + B v^2 \quad \text{where } A = w D, \; B = k D

Cost ($)
  ^
  |        / Total Cost C(v) = A/v + Bv
  |       /
  |  \   /     * Global Min at v*
  |   \ /
  |    *-----------
  |   / \          \ Time Cost = A/v
  |  /   \          \
  | /     \          \
  +-----------------------------------> Velocity v
           v*

2. The Cost Equipartition Principle

When the hourly energy cost is quadratic (n=2n = 2), the total trip cost is C(v)=Av+BvC(v) = \frac{A}{v} + Bv.
Differentiating with respect to velocity vv:

C′(v)=−Av2+BC'(v) = -\frac{A}{v^2} + B

Setting C′(v)=0C'(v) = 0 yields the optimal cruising velocity:

Av2=B  ⟹  v2=AB  ⟹  v∗=AB\frac{A}{v^2} = B \implies v^2 = \frac{A}{B} \implies v^* = \sqrt{\frac{A}{B}}

Notice what occurs when we evaluate the two individual cost components at this optimal speed v∗v^*:

Ctime(v∗)=Av∗=AA/B=ABC_{\text{time}}(v^*) = \frac{A}{v^*} = \frac{A}{\sqrt{A/B}} = \sqrt{AB}
Cfuel(v∗)=Bv∗=BAB=ABC_{\text{fuel}}(v^*) = B v^* = B \sqrt{\frac{A}{B}} = \sqrt{AB}

The Cost Equipartition Theorem

For any transportation model where hourly propulsion expenditure scales quadratically with speed, the minimum total trip cost occurs at the precise velocity where total labor/time expenditure exactly equals total fuel/energy expenditure:

Ctime(v∗)=Cfuel(v∗)C_{\text{time}}(v^*) = C_{\text{fuel}}(v^*)

3. Verification on Unbounded Domains (The Single Critical Point Rule)

Because velocity is physically positive (v>0v > 0), the operational domain is often modeled on the open interval (0,∞)(0, \infty) or a bounded legal range [vmin⁡,vmax⁡][v_{\min}, v_{\max}].
Taking the second derivative:

C′′(v)=2Av3+2B(or 2Av3>0)C''(v) = \frac{2A}{v^3} + 2B \quad (\text{or } \frac{2A}{v^3} > 0)
Since A,B,v>0A, B, v > 0, C′′(v)>0C''(v) > 0 strictly for all positive velocities. By the Single Critical Point Rule (formalized in First Derivative Test), the stationary point v∗v^* is guaranteed to be the unique absolute minimum across the entire domain.


Engineering Applications & Context

In UNLV engineering disciplines, cruising velocity optimization governs mission planning and fleet routing:

  • Mechanical & Automotive Engineering: Electric vehicle (EV) commercial delivery vans optimize highway cruising speeds to balance driver wages against battery discharge limits and recharge downtime.
  • Aerospace Engineering & Aviation: Airline flight dispatchers program the Flight Management System (FMS) "Cost Index" (CI=Time CostFuel CostCI = \frac{\text{Time Cost}}{\text{Fuel Cost}}) to continuously calculate optimal cruising Mach numbers that minimize total direct operating costs per flight hour.
  • Ocean & Marine Engineering: Container shipping lines implement "slow steaming" policies, mathematically reducing ship transit speed by 15–20%15\text{--}20\% across trans-oceanic legs to slash bunker fuel expenses by up to 50%50\%.
  • Autonomous Robotics: Autonomous Underwater Vehicles (AUVs) and long-endurance solar drones optimize forward velocity to maximize range and battery mission duration.

Example Problems

Example Problem 1: Long-Haul Freight Truck Optimization

A long-haul transport truck operates on a 300-mile300\text{-mile} highway route. The driver earns a flat wage of $36/hour\$36/\text{hour}. When cruising at a steady speed vv (in mph\text{mph}), diesel fuel costs v2100\frac{v^2}{100} dollars per hour. The truck operates within the legal speed interval v∈[40,75] mphv \in [40, 75]\text{ mph}. Find the cruising speed that minimizes the total trip cost, and calculate the cost at that speed.

Solution

Step 1: State governing formulas

  • Total Trip Cost Function:
    C(v)=Time×(Hourly Wage+Hourly Fuel)=Dv(w+v2k)=wDv+DkvC(v) = \text{Time} \times (\text{Hourly Wage} + \text{Hourly Fuel}) = \frac{D}{v} \left(w + \frac{v^2}{k}\right) = \frac{w D}{v} + \frac{D}{k} v
    (Defined in Cruising Velocity and Operational Transit Cost Optimization.)

Step 2: Substitute problem parameters
Given distance D=300 milesD = 300\text{ miles}, wage w=$36/hrw = \$36/\text{hr}, fuel coefficient k=100k = 100:

C(v)=300v(36+v2100)=10,800v+3vfor v∈[40,75]C(v) = \frac{300}{v}\left(36 + \frac{v^2}{100}\right) = \frac{10,800}{v} + 3v \quad \text{for } v \in [40, 75]

Step 3: Differentiate and find critical numbers

C′(v)=−10,800v2+3C'(v) = -\frac{10,800}{v^2} + 3
Set C′(v)=0C'(v) = 0:
10,800v2=3  ⟹  3v2=10,800  ⟹  v2=3,600  ⟹  v=60 mph\frac{10,800}{v^2} = 3 \implies 3v^2 = 10,800 \implies v^2 = 3,600 \implies v = 60\text{ mph}
v=60 mphv = 60\text{ mph} lies strictly within the legal interval [40,75][40, 75].

Step 4: Execute Closed Interval Method

  • At minimum speed (v=40 mphv = 40\text{ mph}):
    C(40)=10,80040+3(40)=270+120=$390C(40) = \frac{10,800}{40} + 3(40) = 270 + 120 = \$390
  • At maximum speed (v=75 mphv = 75\text{ mph}):
    C(75)=10,80075+3(75)=144+225=$369C(75) = \frac{10,800}{75} + 3(75) = 144 + 225 = \$369
  • At critical speed (v=60 mphv = 60\text{ mph}):
    C(60)=10,80060+3(60)=180+180=$360C(60) = \frac{10,800}{60} + 3(60) = 180 + 180 = \$360

Conclusion:
The optimal cruising speed is 60 mph60\text{ mph}, yielding a minimum total operating cost of $360\$360.
(Notice that labor cost $180\$180 exactly equals fuel cost $180\$180, confirming the Cost Equipartition Theorem.)


Example Problem 2: Marine Container Cargo Transit

A commercial container ship navigates a 400-nautical-mile400\text{-nautical-mile} voyage. Crew and hotel electrical operations cost $500/hour\$500/\text{hour}. Due to hydrodynamic hull resistance at sea, bunker fuel costs 0.25v30.25 v^3 dollars per hour at cruising velocity vv (in knots). If navigational constraints require v∈[6,18] knotsv \in [6, 18]\text{ knots}, find the velocity minimizing total voyage cost.

Solution

Step 1: State governing formulas

Step 2: Substitute parameters
D=400 nmiD = 400\text{ nmi}, w=$500/hrw = \$500/\text{hr}, k=0.25k = 0.25:

C(v)=400v(500+0.25v3)=200,000v+100v2for v∈[6,18]C(v) = \frac{400}{v}(500 + 0.25 v^3) = \frac{200,000}{v} + 100 v^2 \quad \text{for } v \in [6, 18]

Step 3: Differentiate and find critical numbers

C′(v)=−200,000v2+200vC'(v) = -\frac{200,000}{v^2} + 200 v
Set C′(v)=0C'(v) = 0:
200v=200,000v2  ⟹  200v3=200,000  ⟹  v3=1,000  ⟹  v=10 knots200 v = \frac{200,000}{v^2} \implies 200 v^3 = 200,000 \implies v^3 = 1,000 \implies v = 10\text{ knots}

Step 4: Verify absolute minimum

  • At v=6 knotsv = 6\text{ knots}: C(6)=200,0006+100(36)≈33,333.33+3,600=$36,933.33C(6) = \frac{200,000}{6} + 100(36) \approx 33,333.33 + 3,600 = \$36,933.33
  • At v=18 knotsv = 18\text{ knots}: C(18)=200,00018+100(324)≈11,111.11+32,400=$43,511.11C(18) = \frac{200,000}{18} + 100(324) \approx 11,111.11 + 32,400 = \$43,511.11
  • At v=10 knotsv = 10\text{ knots}: C(10)=200,00010+100(100)=20,000+10,000=$30,000C(10) = \frac{200,000}{10} + 100(100) = 20,000 + 10,000 = \$30,000

The optimal cruising speed is 10 knots10\text{ knots}, minimizing voyage operating expenses to $30,000\$30,000.


Connections & References