First, let's consider the following velocity vs. time graph which shows a constant acceleration:
Since the slope of this graph is the acceleration, and since the slope of this graph is constant, the acceleration represented here is constant.
Also, remember that the area under this graph is the displacement, or change in position, of the object.
Now, let's consider a time period over which this acceleration occurs. We will concern ourselves with a time period from t1to t2:
At t1 we will say that the velocity is v1.
And at t2 we will say that the velocity is v2:
Now, recall that the area under this graph is the displacement of the object. So the area under the graph from t1 to t2 represents the displacement of the object over the time
period from t1 to t2.
Notice that this area is a trapezoid, here shaded blue:
In general, the area of a trapezoid equals one-half times the sum of the bases times the height. This
trapezoid, one might say, is "on its side" since
the bases are vertical and the height is horizontal.
Now, back to our v vs. t graph.
Notice that Base 1 is v1, Base 2 is v2, and that the Height is the time period from t1 to t2.
The formula for the area of the trapezoid is:
We will call the time period from t1
to t2 to be simply t. That is:
t = t2 - t1
So, the height of the trapezoid is t, and
the two bases are v1 and v2. Therefore,
the area of the trapezoid is:
Area = ½(v1 + v2)
t
Now, we remember that the area of a
v vs. t graph is the change in position, or the
displacement, and that displacement is symbolized with Δx.
Therefore, this:
Area = ½(v1 + v2)
t
Becomes:
Δx = ½(v1 + v2)
t
Now, as far as the acceleration over the
time period t is concerned, v1 is the velocity at
the start of the acceleration. That is, v1 is the
first or original velocity; so, the symbol v1 and
the symbol vi mean the same thing; that is:
vi = v1
And v2 is the velocity at the
end of the acceleration. That is, v2 is the final
velocity, and the symbols v2 and vf
mean the same thing; that is:
vf = v2
So, this:
Δx = ½(v1 + v2)
t
Is the same as:
Δx = ½(vi + vf)
t
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