Suppose r(t) is the rate at which some quantity changes, in units per unit of time. Over a short time interval of length Δt the rate hardly changes, so the quantity changes by about r(t)Δt. A Riemann sum adds these small changes across [a,b], and in the limit the sum becomes the integral.
Where the rate is negative the quantity decreases, and the integral subtracts that decrease. So the integral is an amount gained minus an amount lost, not a total of everything that happened.
Equal widths
When the table lists the rate at equally spaced times, every subinterval has the same width Δt. The sums of the earlier lessons then apply as they stand.
Unequal widths
Measurements are often taken at uneven times. Then there is no common width to factor out, and each term of the sum carries its own width. The rest of this lesson uses one table of that kind.
A cyclist rides along a straight road. The velocity v(t), in meters per minute, is positive when the cyclist rides east and negative when the cyclist rides west, where t is measured in minutes. The function v is continuous, and selected values are shown.
t (minutes)
0
3
5
9
15
18
v(t) (meters per minute)
260
200
150
80
−40
−100
A midpoint sum from a table
A midpoint sum needs the rate at the middle of each subinterval. A table supplies it only when the midpoint is one of the listed times, so the subintervals are chosen to fit the table. They are usually fewer and wider than the table's own.
Too big or too small
The table shows v only at six times, and says nothing about what it does in between. So a claim about an overestimate or an underestimate needs more information about v than the table gives.