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Mathematics 15 Online
OpenStudy (anonymous):

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OpenStudy (anonymous):

A car travelling at 72km/h decelerates uniformly at 2m/s^2. Calculate (a)the distance it goes before it stops (b)the time it takes to stop (c)the distance it travels during the first and third seconds

OpenStudy (anonymous):

@LarsEighner

OpenStudy (ikram002p):

uniformy means its linear

OpenStudy (ikram002p):

so 2m/s is the slope x(72)=0 so u have a point and slope, write the equation of distance x and speed v

OpenStudy (anonymous):

No , i want to solve it using equations of motion

OpenStudy (ikram002p):

oh well not expert :P

OpenStudy (larseighner):

Okay, if you are even vaguely familiar with calculus: acceleration is the second derivative with respect to time velocity is the first derivative with respect to time. displacement is basic function. you have acceleration is -2 m/s^2 integrate that and you have velocity(t) = 72km/h + (-2 m/s^2)t Please do the conversion here. The metric system makes my skin crawl. and displacement(t) - (72 km/h)(t) + (1/2)(-2 m/s)(t) + initial displacement. If you ever get confused, use dimensional analysis to check. displacement is length velocity is length/time acceleration is length/time^2

OpenStudy (anonymous):

You r great , i will be reading this , i am familiar with that not to worry

OpenStudy (larseighner):

Linear (classical) motion cheat sheet: \[ \large \int adt = at + C \] The antiderivative of acceleration is velocity with respect to time. The constant \(C = v_0\), the initial velocity. The dimension of acceleration is length / (time x time). The integral of acceleration with respect to time (i.e velocity) therefore has dimensions of length/ time. \[ \large \int (at + v_0)dt = {1 \over 2}at^2 + v_0t + C \] The antiderivative of velocity with respect to time is displacement. s is often used for displacement. Do not mistake this s for "speed." Use d in your own work to avoid confusion. In this case \(C = s_0 \) the original displacement The dimension of displacement is length. Going the other way: \[ \large {d \over {dt}} s(t) = v(t) \] \[ \large {d \over {dt}} v(t) = a \]

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