Let the curve be \( y = f(x) \), and suppose it passes through the point \( (x, y) \), with the tangent at this point having slope \( m = \frac{dy}{dx} \).
The general equation of the tangent line at point \( (x, y) \) is: \[ Y - y = m(X - x) \]
Let’s find where this tangent cuts the x-axis and y-axis.
So the intercepts are: \[ A = \left(x - \frac{y}{m}, 0\right), \quad B = \left(0, y - mx\right) \]
Now consider the segment AB. The midpoint of this segment is: \[ \left( \frac{x - \frac{y}{m}}{2}, \frac{y - mx}{2} \right) \]
We are given that the point of contact \( (x, y) \) is the midpoint. So equating coordinates:
\[ x = \frac{x - \frac{y}{m}}{2}, \quad y = \frac{y - mx}{2} \]
Now solve both equations. Start with the first:
Multiply both sides by 2: \[ 2x = x - \frac{y}{m} \Rightarrow x = -\frac{y}{m} \Rightarrow m = -\frac{y}{x} \]
Now use this in the second equation:
\[ y = \frac{y - mx}{2} \Rightarrow 2y = y - mx \Rightarrow y = -mx \]
Substitute \( m = -\frac{y}{x} \): \[ y = -\left(-\frac{y}{x}\right)x = y \] So both conditions are satisfied.
So we conclude: \[ \frac{dy}{dx} = m = -\frac{y}{x} \Rightarrow \frac{dy}{dx} = -\frac{y}{x} \]
This is a separable differential equation: \[ \frac{dy}{y} = -\frac{dx}{x} \Rightarrow \int \frac{dy}{y} = -\int \frac{dx}{x} \Rightarrow \ln|y| = -\ln|x| + C \Rightarrow \ln|y| + \ln|x| = C \Rightarrow \ln|xy| = C \Rightarrow xy = C' \]
The general solution is: \[ xy = C \]
Use the point \( (3, 2) \) to find the constant: \[ 3 \cdot 2 = 6 \Rightarrow C = 6 \]
\[ \boxed{xy = 6} \]
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is:
A cylindrical tank of radius 10 cm is being filled with sugar at the rate of 100π cm3/s. The rate at which the height of the sugar inside the tank is increasing is:
A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: