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  1. In summary, \(y(x, t)=A \sin (k x-\omega t+\phi)\) models a wave moving in the positive x-direction and \(y(x, t)=A \sin (k x+\omega t+\phi)\) models a wave moving in the negative x-direction. Equation \ref{16.4} is known as a simple harmonic wave function.

  2. We can use the displacement equations in the x and y direction to obtain an equation for the parabolic form of a projectile motion: \[\mathrm{y=\tan θ⋅x−\dfrac{g}{2⋅u^2⋅ \cos ^2 θ}⋅x^2}\] Maximum Height

  3. Displacement. Displacement \(\Delta\)x is the change in position of an object: \[\Delta x = x_{f} - x_{0}, \label{3.1}\] where \(\Delta\)x is displacement, x f is the final position, and x 0 is the initial position.

  4. In the textbook, it said a wave in the form $y(x, t) = A\cos(\omega t + \beta x + \varphi)$ propagates along negative $x$ direction and $y(x, t) = A\cos(\omega t - \beta x + \varphi)$ propagates along positive $x$ direction.

  5. Calculate position vectors in a multidimensional displacement problem. Solve for the displacement in two or three dimensions. Calculate the velocity vector given the position vector as a function of time. Calculate the average velocity in multiple dimensions.

  6. The equations (a) and (b) represent the transverse wave moving along the X-axis, where y (x,t) gives the displacement of the elements of the string at a position x at any time t. Hence, the shape of the wave can be determined at any given time. y (x, t) = a sin (kx + ωt + φ ),

  7. In summary, y (x, t) = A sin (k x − ω t + ϕ) y (x, t) = A sin (k x − ω t + ϕ) models a wave moving in the positive x-direction and y (x, t) = A sin (k x + ω t + ϕ) y (x, t) = A sin (k x + ω t + ϕ) models a wave moving in the negative x-direction. Equation 16.4 is known as a simple harmonic wave function.