\( \frac{dy^2}{dx^2} = 0 \)
We need to determine the differential equation that represents all non-vertical lines in a plane. A line in the plane can be expressed in the slope-intercept form as \( y = mx + c \), where \( m \) is the slope and \( c \) is the y-intercept. For any line, the slope \( m \) is defined by the derivative \( \frac{dy}{dx} = m \), which signifies that the rate of change of \( y \) with respect to \( x \) is constant.
To find the differential equation, consider the derivative of \( \frac{dy}{dx} \):
The second derivative, \( \frac{d^2y}{dx^2} \), represents the rate of change of the slope. For a straight line, this rate of change is zero since the slope is constant. Therefore, for a non-vertical line, we have:
\(\frac{d^2y}{dx^2} = 0\)
This equation indicates that the second derivative of \( y \) with respect to \( x \) is zero, meaning that the slope (first derivative) of the line does not change as \( x \) changes. Thus, the differential equation of all non-vertical lines in a plane is \( \frac{d^2y}{dx^2} = 0 \).
To find the differential equation of all non-vertical lines in a plane, we begin by considering the standard equation of a line: \(y = mx + c\), where \(m\) is the slope and \(c\) is the y-intercept.
A non-vertical line has a defined slope \(m\), and thus the function \(y(x)\) is differentiable with respect to \(x\). The first derivative \( \frac{dy}{dx} = m \) is a constant since the slope of a line is constant.
To derive the differential equation, we differentiate the slope \( \frac{dy}{dx} \) again with respect to \(x\):
\(\frac{d}{dx}\left(\frac{dy}{dx}\right) = \frac{d}{dx}(m) = 0\)
Thus, the second derivative \( \frac{d^2y}{dx^2} \) is zero, indicating that the rate of change of the slope is zero.
Hence, the differential equation representing all non-vertical lines is:
\(\frac{d^2y}{dx^2} = 0\)
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: