Daniel B. answered 03/15/23
A retired computer professional to teach math, physics
As a matter of notation, let vx and vy be the x- and y- components of v.
That is
vx(t) = t + sin(t) + cos(t)
vy(t) = 2t - 6
a)
The position function s(t) is the integral of velocity.
s(t) = ( ∫(t + sin(t) + cos(t))dt, ∫(2t - 6)dt )
= ( t²/2 - cos(t) + sin(t) + C, t² - 6t + D )
for any constants C and D.
Those two constants are determined from the initial condition.
(-1, -1) = s(0) = (0²/2 - cos(0) + sin(0) + C, 0² - 6×0 + D) = (-1 + C, D)
Therefore C = 0, D = -1.
So the function of the position is
s(t) = (t²/2 - cos(t) + sin(t), t² - 6t - 1)
b)
The particle will be on the x-axis whenever the y-coordinate is 0.
t² - 6t - 1 = 0
t = (6 ± √(6² + 4))/2 = 3 ± √10
The particle will be on the x-axis at two times, first at time 3-√10 then 3+√10
c)
v(0)) = (0 + sin(0) + cos(0), 2×0 - 6) = (1, -6)
That means it is moving in the positive x-direction and negative y-direction.
That is, right and down.
d)
Let sx(t) and sy(t) be the x and y-coordinates of s(t).
Then the tangent to the curve s(t) is the function
s'(t) = dsy/dsx = (dsy/dt)/(dsx/dt) = vy/vx = (t + sin(t) + cos(t))/(2t - 6)
The tangent line at time t = 0 going through the point (-1,-1) will be of the form
y + 1 = s'(0)(x + 1)
We can evaluate
s'(0) = (0 + sin(0) + cos(0))/(2×0 - 6) = -1/6