Undergrad "Hence the partial derivatives ru and rv at P are tangential

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SUMMARY

The discussion centers on the concept of partial derivatives ru and rv in the context of a parametrized surface defined by the position function r = r(u, v). It is established that varying u or v independently results in movement along the surface, making the partial derivatives tangential to the surface at point P. The relationship between the partial derivatives and the tangent plane is clarified through the vector cross product, which yields a normal vector to the tangent plane at P. This understanding is crucial for visualizing how surfaces behave in multivariable calculus.

PREREQUISITES
  • Understanding of multivariable calculus concepts, specifically partial derivatives.
  • Familiarity with parametrization of surfaces in three-dimensional space.
  • Knowledge of vector calculus, including cross products and normal vectors.
  • Basic comprehension of tangent planes and their geometric significance.
NEXT STEPS
  • Study the concept of parametrization of surfaces in depth, focusing on examples of r = r(u, v).
  • Learn about the geometric interpretation of partial derivatives and their role in defining tangent planes.
  • Explore vector calculus techniques, particularly the computation of cross products and their applications.
  • Investigate the implications of tangent vectors and normal vectors in higher-dimensional calculus.
USEFUL FOR

Students and professionals in mathematics, particularly those studying multivariable calculus, as well as educators seeking to clarify the geometric interpretation of partial derivatives and tangent planes.

OmegaKV
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I've been looking at the equation for r tilde prime in the image I attached below, but I cannot understand why it is that they say "Hence, the partial derivatives ru and rv at P are tangential to S at P".

g0gYbLr.jpg


How does that equation imply that ru and rv are tangential to P?
 
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When you parametize a surface and have some position function ## r=r(u,v) ## that defines the surface, you can vary u and v independently and any new value of u and/or v (e.g. ## u_1 ## and ## v_1 ##) will give a location ## r=r(u_1,v_1) ## that is also on the surface. As a result, if you allow just u to vary infinitesimally (keeping v constant), you will move along the surface and your direction of motion will be tangent to the (two-dimensional) surface. Likewise, infinitesimal variations in v (keeping u constant) will also cause you to move tangent to the surface, i.e. the motion is somewhere in the plane that is tangent to the surface at that point. Normally the motion caused by varying u and the motion caused by varying v are not colinear. The two partial derivatives (by taking a vector cross product) will give you a vector normal to the tangent plane at that point(i.e. perpendicular to the surface).
 
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Is as in one dimension where the angular coefficient of the tangent line of a function ##f(x)## is the derivative in this point. In this case you have that the surface ##S## is a function of two variables ##f(x,y)## so the partial derivatives generate a plane (not a line!) that is the tangent plane at ##P## ... I simplify a lot with the hope to clarify the concept ...
 

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