Solution

ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2004/iii/paper-77/1/i/solution

The Lighthill elongated-body theory approximation treats each cross-section of a slender swimmer as a locally two-dimensional potential flow problem. The transverse dimension is small compared with the length and the scale over which cross-sections vary. The displacement and slope are small enough to linearize the impermeability condition about a straight body. The Reynolds number is sufficiently large for lateral loading to be dominated by fluid inertia; viscosity, axial friction and higher-order end corrections are neglected at this order. This reactive approximation must be distinguished from the viscous resistive-force theory used for a flagellum.
In coordinates translating with the swimmer, the undisturbed fluid passes in the positive direction at speed . Applying the impermeability condition to the moving centre plane gives the transverse fluid velocity
The local added mass is defined so that the transverse fluid hydrodynamic impulse per unit axial length is . A fixed body-coordinate interval receives an impulse flux at its leading end and loses the corresponding flux at its trailing end. Its rate of change of impulse plus the net outward impulse flux is therefore
This is the transverse force exerted by the body on the fluid. By Newton's third law, the transverse force exerted by the fluid on the body has the opposite sign:
The distinction is essential here: the printed positive expression is labelled as the force on the fish, so that label and expression are inconsistent. For example, take a uniform cross-section and a rigid lateral displacement . The swimmer must accelerate fluid of added mass , which reacts on it with force , not . Thus the positive expression is recovered exactly with the force-on-fluid convention; the physically consistent force on the fish is the negative expression. In the following parts, denotes so that the beam balance uses a genuine external force on the fish.

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