Oscillating Plane and Z axis - Energy Balance

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SUMMARY

The discussion focuses on the relationship between the osculating plane, defined by the principal unit tangent and normal vectors, and the inertial Cartesian z-axis. The key equations derived involve the angles and distances related to the tangent and normal vectors, specifically ds*sin(theta) = dz and dn*cos(theta) = dz. The user seeks to justify the geometric relationship, questioning whether the z-axis is always within the osculating plane. The conclusion drawn is that the z-axis is generally not in the osculating plane, and direction cosines provide a more general framework for understanding these relationships.

PREREQUISITES
  • Understanding of osculating planes in differential geometry
  • Familiarity with principal unit tangent and normal vectors
  • Basic knowledge of energy and force balance equations in fluid mechanics
  • Concept of direction cosines in three-dimensional geometry
NEXT STEPS
  • Study the derivation of energy balance equations in fluid mechanics
  • Explore the properties of osculating planes in differential geometry
  • Learn about direction cosines and their applications in 3D geometry
  • Investigate the relationship between tangent and normal vectors in kinematics
USEFUL FOR

Students and professionals in engineering, particularly those focused on fluid mechanics, kinematics, and differential geometry, will benefit from this discussion.

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Hello,

I have a few questions regarding the osculating plane, which I understand to be the plane generated by the Principal unit tangent vector and principal unit normal vector (both are orthogonal), and the inertial Cartesian z-axis.

Ultimately, I plan to understand the geometric/kinematic equations necessary to derive an energy balance of an element starting from a force balance. Also, elementary fluid mechanics textbooks often show this derivation and it seems the z-axis is in the osculating plane.

Here are the equations (image attached). Let the angle between the z-axis in the normal vector be 'theta', let the differential distance in the direction of the motion (tangent vector) be 'ds' and let the differential distance in the direction of normal be 'dn'.

ds*sin(theta) = dz <--- this is the one needed to convert force balance in the z direction into an energy balance.

dn*cos(theta) = dz <---- this one indicates to me that the osculating plane has the z-axis within itI don't really need help with the force balance I just need justification for the geometry.

For instance, is this always/generally true? I feel like the z-axis is not always in the osculating plane. Thus, wouldn't Direction cosines be more general? Thank you
 

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I will say that generally the z axis is not in the osculating plane. However, the angle, theta, the tangent direction, s, makes with a arbitrary horizontal axis, h1, (that is orthogonal to z axis) is the same angle the normal direction makes with the z axis or equivalently it makes a 90-theta angle with another horizontal axis, h2, (that too is orthogonal to z axis).

These two horizontal axes h1 and h2 are not necessarily x or y, but may coincide with them.
 

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