曲线 CC 的参数方程定义为: x=atan⁡t,y=asec⁡2tsin⁡t,−π4<t<π4,x = a\tan t, \qquad y = a\sec^{2}t\sin t, \qquad -\frac{\pi}{4} < t < \frac{\pi}{4}, 其中 aa 为正常数。

  1. (a)

    证明 tan⁡t1+tan⁡2t=sin⁡t\dfrac{\tan t}{\sqrt{1+\tan^{2}t}} = \sin t。

  2. (b)

    利用 (a) 的结论或通过其他方法,求出 CC 的直角坐标方程,形式为 y=f(x)y=f(x),并化简你的答案。

  3. (c)

    证明 f(−x)=−f(x)f(-x) = -f(x)。由此画出 CC 的草图。

  4. (d)

    求由 CC、x轴以及直线 x=−Ax=-A 和 x=Ax=A(其中 0<A<a0 < A < a)所围成区域的面积的准确值,答案用 AA 和 aa 表示。

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完整解法

6(a)

1. Apply the Pythagorean identity to the expression under the square root.

LHS=tan⁡t1+tan⁡2t\text{LHS} = \frac{\tan t}{\sqrt{1+\tan^{2}t}}
=tan⁡tsec⁡2t= \frac{\tan t}{\sqrt{\sec^{2}t}}

2. Simplify the denominator based on the given domain and express the ratio in terms of sine and cosine.

For −π4<t<π4-\frac{\pi}{4} < t < \frac{\pi}{4}, sec⁡t>0\sec t > 0, so sec⁡2t=sec⁡t\sqrt{\sec^{2}t} = \sec t.
=tan⁡tsec⁡t= \frac{\tan t}{\sec t}
=(sin⁡tcos⁡t)(1cos⁡t)= \frac{\left(\frac{\sin t}{\cos t}\right)}{\left(\frac{1}{\cos t}\right)}
=sin⁡t=RHS= \sin t = \text{RHS}

答案

Shown\text{Shown}

6(b)

1. Express $y$ entirely in terms of $\tan t$ using a trigonometric identity and the result from part (a).

Using the identity sec⁡2t=1+tan⁡2t\sec^2 t = 1 + \tan^2 t, we rewrite the expression for yy:
y=a(1+tan⁡2t)sin⁡ty = a(1 + \tan^2 t)\sin t

From part (a), substitute sin⁡t=tan⁡t1+tan⁡2t\sin t = \frac{\tan t}{\sqrt{1 + \tan^2 t}}:
y=a(1+tan⁡2t)(tan⁡t1+tan⁡2t)y = a(1 + \tan^2 t) \left( \frac{\tan t}{\sqrt{1 + \tan^2 t}} \right)
y=atan⁡t1+tan⁡2ty = a\tan t \sqrt{1 + \tan^2 t}

2. Substitute $x$ to eliminate $t$ and simplify to find the cartesian equation.

From x=atan⁡tx = a\tan t, we have tan⁡t=xa\tan t = \frac{x}{a}. Substituting this into our equation for yy:
y=a(xa)1+(xa)2y = a \left( \frac{x}{a} \right) \sqrt{1 + \left( \frac{x}{a} \right)^2}
y=x1+x2a2y = x \sqrt{1 + \frac{x^2}{a^2}}
y=xa2+x2a2y = x \sqrt{\frac{a^2 + x^2}{a^2}}

Since aa is a positive constant, a2=a\sqrt{a^2} = a. Thus, simplifying gives:
y=xaa2+x2y = \frac{x}{a}\sqrt{a^2 + x^2}

答案

y=xaa2+x2y = \frac{x}{a}\sqrt{a^2 + x^2}

6(c)

1. Determine the cartesian equation $f(x)$ from part (b) and its domain, which are required for this part.

From part (b), we know x=atan⁡t  ⟹  tan⁡t=xax = a\tan t \implies \tan t = \frac{x}{a}.
Thus, 1+tan⁡2t=1+x2a2=a2+x2a21+\tan^2 t = 1+\frac{x^2}{a^2} = \frac{a^2+x^2}{a^2}.
Using the result from (a),
sin⁡t=x/aa2+x2a2=xa2+x2\sin t = \frac{x/a}{\sqrt{\frac{a^2+x^2}{a^2}}} = \frac{x}{\sqrt{a^2+x^2}}
y=asec⁡2tsin⁡t=a(a2+x2a2)(xa2+x2)=xaa2+x2y = a\sec^2 t \sin t = a\left(\frac{a^2+x^2}{a^2}\right)\left(\frac{x}{\sqrt{a^2+x^2}}\right) = \frac{x}{a}\sqrt{a^2+x^2}
Since −π4<t<π4-\frac{\pi}{4} < t < \frac{\pi}{4}, the domain is −a<x<a-a < x < a.
Therefore, f(x)=xaa2+x2f(x) = \frac{x}{a}\sqrt{a^2+x^2}.

2. Show that $f(-x) = -f(x)$.

Substitute −x-x into f(x)f(x):
f(−x)=(−x)aa2+(−x)2f(-x) = \frac{(-x)}{a}\sqrt{a^2+(-x)^2}
f(−x)=−xaa2+x2f(-x) = -\frac{x}{a}\sqrt{a^2+x^2}
f(−x)=−f(x)f(-x) = -f(x)
This shows that f(x)f(x) is an odd function.

3. Sketch the curve $C$.

The curve passes through the origin (0,0)(0,0).
Since f(−x)=−f(x)f(-x) = -f(x), the graph has rotational symmetry about the origin.
At the domain limits x→±ax \to \pm a:
When x→ax \to a, y→aaa2+a2=a2y \to \frac{a}{a}\sqrt{a^2+a^2} = a\sqrt{2}.
When x→−ax \to -a, y→−a2y \to -a\sqrt{2}.
Since f′(x)=2x2+a2ax2+a2>0f'(x) = \frac{2x^2+a^2}{a\sqrt{x^2+a^2}} > 0 and f′′(x)=x(2x2+3a2)a(x2+a2)3/2f''(x) = \frac{x(2x^2+3a^2)}{a(x^2+a^2)^{3/2}}, the curve is strictly increasing, concave downwards for −a<x<0-a < x < 0 and concave upwards for 0<x<a0 < x < a.
(Note: The sketch is a smooth curve passing through (0,0)(0,0), ending with open circles at (−a,−a2)(-a, -a\sqrt{2}) and (a,a2))(a, a\sqrt{2})).

答案

Proof that f(−x)=−f(x)f(-x) = -f(x) as shown in the steps.

The sketch of CC is a smooth, strictly increasing curve defined on −a<x<a-a < x < a, starting from an open circle at (−a,−a2)(-a, -a\sqrt{2}), passing through the origin (0,0)(0,0) as a point of inflexion, and ending at an open circle at (a,a2)(a, a\sqrt{2}). Due to f(−x)=−f(x)f(-x) = -f(x), the graph exhibits rotational symmetry about the origin.

6(d)

1. Derive the Cartesian equation $y=f(x)$ (from part b) needed for the integration.

From part (a), sin⁡t=tan⁡t1+tan⁡2t\sin t = \dfrac{\tan t}{\sqrt{1+\tan^2 t}}.
Given x=atan⁡t  ⟹  tan⁡t=xax = a\tan t \implies \tan t = \dfrac{x}{a}, so sin⁡t=x/a1+(x/a)2=xa2+x2\sin t = \dfrac{x/a}{\sqrt{1+(x/a)^2}} = \dfrac{x}{\sqrt{a^2+x^2}}.
y=asec⁡2tsin⁡t=a(1+tan⁡2t)sin⁡t=a(1+x2a2)xa2+x2=xaa2+x2y = a\sec^2 t \sin t = a\left(1+\tan^2 t\right)\sin t = a\left(1+\dfrac{x^2}{a^2}\right)\dfrac{x}{\sqrt{a^2+x^2}} = \dfrac{x}{a}\sqrt{a^2+x^2}.
Thus, f(x)=xaa2+x2f(x) = \dfrac{x}{a}\sqrt{a^2+x^2}.

2. Set up the definite integral for the area using the function's odd symmetry.

From part (c), f(−x)=−f(x)f(-x) = -f(x), so the curve has odd symmetry about the origin. The region bounded by x=−Ax=-A and x=Ax=A consists of two identical areas (one above and one below the xx-axis).
Area=∫−A0∣f(x)∣ dx+∫0A∣f(x)∣ dx=2∫0Af(x) dx\text{Area} = \int_{-A}^{0} |f(x)|\,dx + \int_{0}^{A} |f(x)|\,dx = 2\int_{0}^{A} f(x)\,dx
Area=2∫0Axaa2+x2 dx\text{Area} = 2\int_{0}^{A} \dfrac{x}{a}\sqrt{a^2+x^2}\,dx

3. Evaluate the definite integral using a standard integration rule.

Area=1a∫0A2x(a2+x2)1/2 dx\text{Area} = \dfrac{1}{a} \int_{0}^{A} 2x(a^2+x^2)^{1/2}\,dx
=1a[(a2+x2)3/23/2]0A= \dfrac{1}{a} \left[ \dfrac{(a^2+x^2)^{3/2}}{3/2} \right]_{0}^{A}
=23a((a2+A2)3/2−(a2+02)3/2)= \dfrac{2}{3a} \left( (a^2+A^2)^{3/2} - (a^2+0^2)^{3/2} \right)
Since a>0a > 0, (a2)3/2=a3(a^2)^{3/2} = a^3.
Area=23a((a2+A2)3/2−a3)\text{Area} = \dfrac{2}{3a}\left( (a^2+A^2)^{3/2} - a^3 \right)

答案

23a((a2+A2)3/2−a3)\dfrac{2}{3a}\left( (a^2+A^2)^{3/2} - a^3 \right)

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