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The time rate of change of velocity of an object, or alternately the net force on the object divided by the object's mass.

Mathematical Representation

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\begin

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[ \vec

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= \frac{d\vec{v}}

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\qquad \mbox

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\qquad \vec

=\frac{\sum \vec{F}}

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]\end

One-Dimensional Acceleration

Utility of the One-Dimensional Case

As with all vector equations, the equations of kinematics are usually approached by separation into components. In this fashion, the equations become three simultaneous one-dimensional equations. Thus, the consideration of motion in one dimension with acceleration can be generalized to the three-dimensional case.

Useful Digrammatic Representations

Several diagrammatic representations are commonly used to represent accelerated motion.

  • [*Velocity vs. Time Graph*]
Deceleration

In physics, the term acceleration denotes a vector, as does velocity. When the acceleration of an object points in the same direction as its velocity, the object speeds up. When the acceleration of an object points in the direction opposite the object's velocity, the object slows down. In everyday speech, we would call the first case "acceleration" and the second case "deceleration". In physics, both cases represent acceleration, but with a different relationship to the velocity.

Constant Acceleration
Integration with Respect to Time

If acceleration is constant, the definition of acceleration can be integrated:

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\begin

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[ \int_{v_{\rm i}}^

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dv = \int_{t_{\rm i}}^

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a\: dt ] \end

For the special case of constant acceleration, the integral yields:

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\begin

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[ v - v_

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= a(t-t_

) ] \end

which is equivalent to:

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\begin

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[ v = v_

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+ a (t-t_

) ] \end

We can now substitute into this equation the definition of velocity,

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\begin

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[ v = \frac

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]\end

which gives:

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\begin

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[ \frac

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= v_

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+ a t - a t_

] \end

We can now integrate again:

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\begin

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[ \int_{x_{\rm i}}^

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dx = \int_{t_{\rm i}}^

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\left( v_

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  • at_

+ a t\right)\:dt ] \end

to find:

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\begin

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[ x - x_

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= v_

(t-t_

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) - a t_

(t-t_

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) + \frac

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a( t^

- t_

^

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) ] \end

We finish up with some algebra:

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\begin

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[ x = x_

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+ v_

(t-t_

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) + \frac

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a (t^

- 2 t t_

+ t_

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^

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) ] \end

which is equivalent to:

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\begin

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[ x = x_

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+ v_

(t-t_

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) + \frac

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a (t - t_

)^

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] \end

Integration with Respect to Position

The definition of acceleration can also be integrated with respect to position, if we use a calculus trick that relies on the chain rule. Returning to the definition of acceleration:

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\begin

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[ \frac

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= a ] \end

we would like to find an expression for v as a function of x instead of t. One way to achieve this is to use the chain rule to write:

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\begin

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[ \frac

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\frac

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= a ] \end

We can now elminate t from this expression by using the defnition of velocity to recognize that dx/dt = v. Thus:

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\begin

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[ \frac

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v = a ] \end

which is easily integrated for the case of constant acceleration:

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\begin

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[ \int_{v_{\rm i}}^

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v \:dv = \int_{x_{\rm i}}^

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a \:dx ] \end

to give:

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\begin

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[ v^

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= v_

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^

+ 2 a (x-x_

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) ] \end

The Utility of Constant Acceleration

Stringing together a series of constant velocity segments is not usually a realistic description of motion, because real objects cannot change their velocity in a discontinuous manner. This drawback does not apply to constant acceleration, however. Objects can have their acceleration changed almost instantaneously. Because of this, it is often reasonable to approximate a complicated motion by separating it into segments of constant acceleration.

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