曲线 CC 的方程为 y=ekxekx−e−kxy = \frac{e^{kx}}{e^{kx} - e^{-kx}},其中 x≠0x \ne 0 且 k∈R, k≠0k \in \mathbb{R},\ k \ne 0。

  1. (i)

    证明 CC 没有驻点。

  2. (ii)

    求曲线 CC 在 y=2y = 2 处的切线方程。

  3. (iii)

    已知 k=1k = 1,求第 (ii) 问中的切线与 y 轴之间的锐角。

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完整解法

6(i)

1. Differentiate the equation of the curve using the quotient rule and simplify.

Using the quotient rule:
dydx=[ddx(ekx)](ekx−e−kx)−(ekx)[ddx(ekx−e−kx)](ekx−e−kx)2\frac{dy}{dx} = \frac{\left[\frac{d}{dx}(e^{kx})\right](e^{kx} - e^{-kx}) - (e^{kx})\left[\frac{d}{dx}(e^{kx} - e^{-kx})\right]}{(e^{kx} - e^{-kx})^2}
dydx=(kekx)(ekx−e−kx)−(ekx)(kekx+ke−kx)(ekx−e−kx)2\frac{dy}{dx} = \frac{(k e^{kx})(e^{kx} - e^{-kx}) - (e^{kx})(k e^{kx} + k e^{-kx})}{(e^{kx} - e^{-kx})^2}
Expanding the terms in the numerator:
dydx=ke2kx−ke0−(ke2kx+ke0)(ekx−e−kx)2\frac{dy}{dx} = \frac{k e^{2kx} - k e^0 - (k e^{2kx} + k e^0)}{(e^{kx} - e^{-kx})^2}
dydx=−2k(ekx−e−kx)2\frac{dy}{dx} = \frac{-2k}{(e^{kx} - e^{-kx})^2}

2. State the condition for stationary points and deduce that none exist.

For stationary points, we require dydx=0\frac{dy}{dx} = 0.
Since k≠0k \neq 0, the numerator −2k≠0-2k \neq 0.
Therefore, dydx≠0\frac{dy}{dx} \neq 0 for all valid xx, demonstrating that CC has no stationary points.

答案

As dydx=−2k(ekx−e−kx)2≠0\frac{dy}{dx} = \frac{-2k}{(e^{kx} - e^{-kx})^2} \neq 0, CC has no stationary points.

6(ii)

1. Find the $x$-coordinate of the point where $y = 2$.

ekxekx−e−kx=2\frac{e^{kx}}{e^{kx} - e^{-kx}} = 2
Multiply the numerator and denominator by ekxe^{kx} to simplify the equation:
e2kxe2kx−1=2\frac{e^{2kx}}{e^{2kx} - 1} = 2
2e2kx−2=e2kx  ⟹  e2kx=22e^{2kx} - 2 = e^{2kx} \implies e^{2kx} = 2
2kx=ln⁡2  ⟹  x=ln⁡22k2kx = \ln 2 \implies x = \frac{\ln 2}{2k}

2. Find the gradient function $\frac{dy}{dx}$ (typically derived in part (i)).

Applying the quotient rule to y=e2kxe2kx−1y = \frac{e^{2kx}}{e^{2kx} - 1}:
dydx=(e2kx−1)(2ke2kx)−(e2kx)(2ke2kx)(e2kx−1)2\frac{dy}{dx} = \frac{(e^{2kx} - 1)(2k e^{2kx}) - (e^{2kx})(2k e^{2kx})}{(e^{2kx} - 1)^2}
dydx=2ke4kx−2ke2kx−2ke4kx(e2kx−1)2=−2ke2kx(e2kx−1)2\frac{dy}{dx} = \frac{2k e^{4kx} - 2k e^{2kx} - 2k e^{4kx}}{(e^{2kx} - 1)^2} = \frac{-2k e^{2kx}}{(e^{2kx} - 1)^2}

3. Evaluate the gradient of the tangent at $e^{2kx} = 2$.

Substitute e2kx=2e^{2kx} = 2 directly into the derivative to find the gradient mm:
m=−2k(2)(2−1)2=−4km = \frac{-2k(2)}{(2 - 1)^2} = -4k

4. Form the equation of the tangent.

Using the point-slope form y−y1=m(x−x1)y - y_1 = m(x - x_1) with the point (ln⁡22k,2)\left(\frac{\ln 2}{2k}, 2\right):
y−2=−4k(x−ln⁡22k)y - 2 = -4k\left(x - \frac{\ln 2}{2k}\right)
y−2=−4kx+4kln⁡22ky - 2 = -4kx + \frac{4k \ln 2}{2k}
y−2=−4kx+2ln⁡2y - 2 = -4kx + 2\ln 2
y=−4kx+2ln⁡2+2y = -4kx + 2\ln 2 + 2

答案

y=−4kx+2ln⁡2+2y = -4kx + 2\ln 2 + 2

6(iii)

1. State the gradient of the tangent when $k = 1$.

From part (ii), the gradient of the tangent at y=2y = 2 is determined to be m=−4km = -4k.
Substituting k=1k = 1:
m=−4(1)=−4m = -4(1) = -4

2. Calculate the acute angle between the tangent and the y-axis.

Let α\alpha be the acute angle the tangent makes with the x-axis.
tan⁡α=∣−4∣=4\tan \alpha = |-4| = 4
α=tan⁡−1(4)≈75.964∘\alpha = \tan^{-1}(4) \approx 75.964^\circ
Since the x-axis and y-axis are perpendicular, the acute angle between the tangent and the y-axis is:
90∘−75.964∘=14.036∘≈14.0∘90^\circ - 75.964^\circ = 14.036^\circ \approx 14.0^\circ

答案

14.0∘14.0^\circ (or 0.2450.245 rad)

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