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求证曲线R(t)=(sec t, sec t tan t)的曲率恰在两点处为零

Alright, let's walk through this proof step by step. I'll break it down into clear, manageable parts so you can follow along easily.

Proof that the curve ( \mathbf{R}(t) = (\sec t, \sec t \tan t) ) has exactly two points with zero curvature on ( (-\pi/2, \pi/2) )

First, let's start with the curvature formula for parametric curves:
For a curve defined by ( \mathbf{R}(t) = (x(t), y(t)) ), the curvature ( k(t) ) is given by:

k(t) = |x'(t)y''(t) - x''(t)y'(t)| / (x'(t)^2 + y'(t)^2)^{3/2}

Curvature is zero if and only if the numerator is zero (the denominator is always positive in our domain, since ( \sec t = 1/\cos t ) is defined and non-zero here, so the derivatives ( x'(t) ) and ( y'(t) ) can't both be zero). So we just need to solve ( x'(t)y''(t) - x''(t)y'(t) = 0 ).


Step 1: Compute all first and second derivatives

Let's calculate each derivative one by one using trigonometric rules and the product rule:

  • For ( x(t) = \sec t ):
    • First derivative: ( x'(t) = \sec t \tan t )
    • Second derivative:
      x''(t) = \sec t \cdot \sec^2 t + \tan t \cdot \sec t \tan t = \sec^3 t + \sec t \tan^2 t = \sec t (\sec^2 t + \tan^2 t)
      
  • For ( y(t) = \sec t \tan t ):
    • First derivative:
      y'(t) = \sec t \cdot \sec^2 t + \tan t \cdot \sec t \tan t = \sec^3 t + \sec t \tan^2 t = \sec t (\sec^2 t + \tan^2 t)
      
    • Second derivative (differentiate term by term):
      d/dt [sec^3 t] = 3 \sec^2 t \cdot \sec t \tan t = 3 \sec^3 t \tan t
      d/dt [sec t \tan^2 t] = \sec t \cdot 2 \tan t \sec^2 t + \tan^2 t \cdot \sec t \tan t = 2 \sec^3 t \tan t + \sec t \tan^3 t
      y''(t) = 3 \sec^3 t \tan t + 2 \sec^3 t \tan t + \sec t \tan^3 t = \sec t \tan t (5 \sec^2 t + \tan^2 t)
      

Step 2: Simplify the numerator expression

Substitute the derivatives into ( x'(t)y''(t) - x''(t)y'(t) ):

x'(t)y''(t) - x''(t)y'(t) = [\sec t \tan t \cdot \sec t \tan t (5 \sec^2 t + \tan^2 t)] - [\sec t (\sec^2 t + \tan^2 t) \cdot \sec t (\sec^2 t + \tan^2 t)]

Factor out the common ( \sec^2 t ) term:

= \sec^2 t \left[ \tan^2 t (5 \sec^2 t + \tan^2 t) - (\sec^2 t + \tan^2 t)^2 \right]

Now expand and simplify the bracket:

  1. Expand the first term: ( 5 \sec^2 t \tan^2 t + \tan^4 t )
  2. Expand the second term: ( (\sec^2 t + \tan^2 t)^2 = \sec^4 t + 2 \sec^2 t \tan^2 t + \tan^4 t )
  3. Subtract the second from the first:
    5 \sec^2 t \tan^2 t + \tan^4 t - \sec^4 t - 2 \sec^2 t \tan^2 t - \tan^4 t = 3 \sec^2 t \tan^2 t - \sec^4 t
    

Factor out ( \sec^2 t ) again:

= \sec^2 t (3 \tan^2 t - \sec^2 t)

The full numerator becomes:

\sec^2 t \cdot \sec^2 t (3 \tan^2 t - \sec^2 t) = \sec^4 t (3 \tan^2 t - \sec^2 t)

Step 3: Solve for zero curvature

In ( -\pi/2 < t < \pi/2 ), ( \sec t \neq 0 ), so ( \sec^4 t \neq 0 ). We only need to solve:

3 \tan^2 t - \sec^2 t = 0

Use the Pythagorean identity ( \sec^2 t = 1 + \tan^2 t ):

3 \tan^2 t - (1 + \tan^2 t) = 0 \\
2 \tan^2 t - 1 = 0 \\
\tan^2 t = 1/2 \\
\tan t = \pm \frac{\sqrt{2}}{2}

Step 4: Find the corresponding curve points

In ( (-\pi/2, \pi/2) ), each ( \tan t ) value maps to exactly one ( t ):

  • When ( \tan t = \sqrt{2}/2 ):
    ( \cos t = \frac{2}{\sqrt{2^2 + (\sqrt{2})^2}} = \frac{\sqrt{6}}{3} ), so ( \sec t = \frac{\sqrt{6}}{2} ).
    ( y = \sec t \tan t = \frac{\sqrt{6}}{2} \cdot \frac{\sqrt{2}}{2} = \frac{\sqrt{3}}{2} ).
    This gives the point ( \left( \frac{\sqrt{6}}{2}, \frac{\sqrt{3}}{2} \right) ).
  • When ( \tan t = -\sqrt{2}/2 ):
    ( \sec t ) remains ( \frac{\sqrt{6}}{2} ) (secant is an even function), and ( y = -\frac{\sqrt{3}}{2} ).
    This gives the point ( \left( \frac{\sqrt{6}}{2}, -\frac{\sqrt{3}}{2} \right) ).

These are the only two points in the domain where curvature is zero—since ( \tan t ) is one-to-one on ( (-\pi/2, \pi/2) ), there are no other solutions.

内容的提问来源于stack exchange,提问作者user380605

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最近更新时间:2026.05.19 06:27:29