A ship 250m long moves in seawater, whose density is 1030 kg/m³. A 1:125 model of this ship is to be tested in wind tunnel. The velocity of air in the wind tunnel around the model is 20m/s and the resistance of the ship is 50N. Determine the velocity and resistance of the ship in seawater.

Fluid Mechanics Problem Solution

Problem Statement

A ship 250m long moves in seawater, whose density is 1030 kg/m³. A 1:125 model of this ship is to be tested in wind tunnel. The velocity of air in the wind tunnel around the model is 20m/s and the resistance of the ship is 50N. Determine the velocity and resistance of the ship in seawater. The density of air is 1.24 kg/m³. Take the kinematic viscosity of seawater and air as 0.012 stokes and 0.018 stokes respectively.

Given Data

Length of prototype (Lp) 250 m
Density of seawater (ρp) 1030 kg/m³
Kinematic viscosity of seawater (υp) 0.012 stokes = 0.012 × 10-4 m²/s
Length of model (Lm) 250/125 = 2 m
Density of air (ρm) 1.24 kg/m³
Kinematic viscosity of air (υm) 0.018 stokes = 0.018 × 10-4 m²/s
Velocity of model (Vm) 20 m/s
Resistance of model (Fm) 50 N

Solution Approach

To determine the velocity and resistance of the ship in seawater, we’ll use the principles of dynamic similarity. Specifically, we’ll apply Reynolds’ model law to determine the velocity of the prototype, and then use force relationships to determine the resistance.

Calculations

Determining Velocity Using Reynolds’ Model Law

Step 1: According to Reynolds’ model law, the Reynolds number for both the model and prototype should be equal:

Remodel = Reprototype
(Vm Lm)/υm = (Vp Lp)/υp

Step 2: Substituting the given values:

(20 × 2)/(0.018 × 10-4) = (Vp × 250)/(0.012 × 10-4)

Step 3: Solving for Vp (velocity of prototype):

Vp = (20 × 2 × 0.012 × 10-4)/(0.018 × 10-4 × 250)
Vp = (20 × 2 × 0.012)/(0.018 × 250)
Vp = 0.48/4.5 = 0.1066 m/s

Velocity of Ship (Vp) = 0.1066 m/s

Determining Resistance

Step 4: The relationship between forces (resistance) can be determined using the force ratio:

Resistance = mass × acceleration = ρL3 × V/t = ρL2 × L/t × V = ρL2V2

Step 5: Setting up the force ratio between prototype and model:

Fp/Fm = (ρpLp2Vp2)/(ρmLm2Vm2)

Step 6: Substituting the given values:

Fp/50 = (1030 × 2502 × 0.10662)/(1.24 × 22 × 202)

Step 7: Solving for Fp (resistance of prototype):

Fp/50 = (1030 × 62500 × 0.011364)/(1.24 × 4 × 400)
Fp/50 = 731446.5/1984 = 368.7
Fp = 50 × 368.7 = 18435 N

Resistance of Ship (Fp) = 18436 N

Detailed Explanation

Principle of Dynamic Similarity

This problem applies the principle of dynamic similarity, which allows engineers to predict the behavior of a full-scale prototype based on tests conducted on a scaled model. For the results to be valid, certain dimensionless parameters must be equal between the model and the prototype.

Reynolds Number Similarity

In this case, we used Reynolds number similarity, which is essential when viscous forces are significant. The Reynolds number (Re) represents the ratio of inertial forces to viscous forces:

Re = (Inertial forces)/(Viscous forces) = (ρVL)/μ = VL/ν

By ensuring the Reynolds numbers are equal, we create dynamically similar flow conditions between the model and prototype.

Force Scaling Relationship

The resistance force scales with the square of the velocity, the square of the length, and the density. This scaling relationship is derived from dimensional analysis and the understanding that:

F ∝ ρL2V2

Model Testing in Different Fluids

This problem presents an interesting case where the model is tested in air while the prototype operates in water. This approach is common when testing large marine vessels, as it can be more practical and cost-effective than testing in water. The different fluid properties (density and viscosity) are accounted for in the scaling relationships.

Practical Applications

The wind tunnel testing approach used in this problem has several practical advantages:

  • Cost efficiency: Air testing facilities are often less expensive to operate than water testing facilities
  • Visibility: Air testing allows for better visualization of flow patterns
  • Scalability: Allows testing of very large marine vessels that would be impractical to test as water models
  • Control: Environmental conditions can be more precisely controlled in wind tunnels

Analysis of Results

The calculated ship velocity of 0.1066 m/s (approximately 0.21 knots) seems relatively slow for a large ship, but this could be appropriate depending on the specific type of vessel and its operating conditions. The resistance force of 18436 N is substantial, reflecting the significant drag forces that must be overcome by the ship’s propulsion system.

These results provide naval architects with critical information for:

  • Designing appropriate propulsion systems
  • Estimating fuel consumption
  • Optimizing hull design to reduce resistance
  • Predicting performance characteristics under various operating conditions

It’s worth noting that while Reynolds number similarity was used in this problem, complete dynamic similarity would require matching other dimensionless parameters as well, such as the Froude number (for free surface effects) and potentially others depending on the specific phenomena being studied.

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