MHB 2.1.2 AP calculus Exan particle move along the x-axis

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The particle's velocity is given by the equation $v(t) = 6t - t^2$. To find the total distance traveled from time $t = 0$ to $t = 3$, the absolute value of the velocity must be integrated over this interval. The calculation shows that at $t = 3$, the velocity is 9, indicating the particle is moving in a positive direction. The position function is derived as $p(t) = 3t^2 - \frac{t^3}{3} + C$, confirming the relationship between position, velocity, and acceleration. The total distance traveled can be computed using the integral of the absolute value of the velocity function.
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A particle moves along the x-axis. The velocity of the particle at time t is $6t - t^2$.
What is the total distance traveled by the particle from time $t = 0$ to $t = 3$
ok we are given $v(t)$ so we do not have to derive it from a(t) since the initial $t=0$ we just plug in the $t=3$ into $v(t)$ so
$6(3) - (3)^2=18-9=9$.
I thot I might of posted this earlier but I could not find it:rolleyes:
 
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Hmmm... $p(t)=3t^2-\frac{t^3}{3}+C$ (Wondering)
 
isn't that for a(t) ??
 
$p'(t)=v(t),\quad v'(t)=a(t)$
 
total distance = $\displaystyle \int_{t_1}^{t_2} |v(t)| \, dt$
 
There are probably loads of proofs of this online, but I do not want to cheat. Here is my attempt: Convexity says that $$f(\lambda a + (1-\lambda)b) \leq \lambda f(a) + (1-\lambda) f(b)$$ $$f(b + \lambda(a-b)) \leq f(b) + \lambda (f(a) - f(b))$$ We know from the intermediate value theorem that there exists a ##c \in (b,a)## such that $$\frac{f(a) - f(b)}{a-b} = f'(c).$$ Hence $$f(b + \lambda(a-b)) \leq f(b) + \lambda (a - b) f'(c))$$ $$\frac{f(b + \lambda(a-b)) - f(b)}{\lambda(a-b)}...

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