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SingaporeMathsSyllabus dot point

How does a telescoping sum collapse, and how do we exploit it to evaluate a series?

Use the method of differences, including the use of partial fractions, to find the sum of a series whose terms telescope, and deduce the sum to infinity where it exists

A focused answer to the H2 Mathematics outcome on the method of differences. Writing a term as a difference (often via partial fractions), cancelling the telescoping sum, and deducing the sum to infinity.

Generated by Claude Opus 4.810 min answer

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

SEAB wants you to evaluate a series by the method of differences: write each term as the difference of consecutive (or near-consecutive) values of some function f(r)\mathrm{f}(r), so that when you sum, almost everything cancels (telescopes), leaving only the boundary terms. Partial fractions is the usual tool for producing the difference.

The answer

The telescoping idea

If each term can be written ur=f(r)βˆ’f(r+1)u_r = \mathrm{f}(r) - \mathrm{f}(r + 1), then

βˆ‘r=1nur=f(1)βˆ’f(n+1)\sum_{r=1}^{n} u_r = \mathrm{f}(1) - \mathrm{f}(n + 1)

because every interior f(2),f(3),…,f(n)\mathrm{f}(2), \mathrm{f}(3), \ldots, \mathrm{f}(n) appears once positive and once negative and cancels. Only the very first and very last survive.

Producing the difference with partial fractions

A term like 1r(r+1)\dfrac{1}{r(r+1)} does not look like a difference, but partial fractions reveals one:

1r(r+1)=1rβˆ’1r+1\frac{1}{r(r+1)} = \frac{1}{r} - \frac{1}{r+1}

This is the standard route: factor the denominator, split into partial fractions, and recognise the difference of a function at consecutive arguments.

Wider gaps

If the difference is f(r)βˆ’f(r+2)\mathrm{f}(r) - \mathrm{f}(r + 2) (a gap of two), then two terms survive at each end: f(1)+f(2)\mathrm{f}(1) + \mathrm{f}(2) at the start and βˆ’f(n+1)βˆ’f(n+2)-\mathrm{f}(n+1) - \mathrm{f}(n+2) at the end. Always write out the first few and last few terms to see exactly what remains.

Sum to infinity

Once you have the closed form, let nβ†’βˆžn \to \infty. If the surviving nn-dependent terms tend to zero, the sum to infinity is just the constant boundary part.

Examples in context

Example 1. A converging resistance ladder. A series βˆ‘1r(r+1)=1βˆ’1n+1\sum \dfrac{1}{r(r+1)} = 1 - \dfrac{1}{n+1} models cumulative contributions that approach a finite total of 11, a clean physical analogue of a quantity saturating as more stages are added.

Example 2. Checking a closed form. Having found βˆ‘r=1n1(2rβˆ’1)(2r+1)=n2n+1\sum_{r=1}^{n} \dfrac{1}{(2r-1)(2r+1)} = \dfrac{n}{2n+1}, substituting n=1n = 1 gives 13\dfrac{1}{3}, which matches the single term 11Γ—3\dfrac{1}{1 \times 3}, a quick verification of the algebra.

Try this

Q1. Given 1rβˆ’1r+1=1r(r+1)\dfrac{1}{r} - \dfrac{1}{r+1} = \dfrac{1}{r(r+1)}, find βˆ‘r=1n1r(r+1)\displaystyle\sum_{r=1}^{n} \dfrac{1}{r(r+1)}. [3 marks]

  • Cue. Telescopes to 1βˆ’1n+1=nn+11 - \dfrac{1}{n+1} = \dfrac{n}{n+1}.

Q2. State what is meant by a telescoping sum and why it simplifies. [2 marks]

  • Cue. Each term is a difference of consecutive values, so interior terms cancel in pairs, leaving only the boundary terms.

Q3. Deduce the sum to infinity of βˆ‘r=1∞1r(r+1)\displaystyle\sum_{r=1}^{\infty} \dfrac{1}{r(r+1)}. [2 marks]

  • Cue. nn+1β†’1\dfrac{n}{n+1} \to 1 as nβ†’βˆžn \to \infty, so the sum to infinity is 11.

Exam-style practice questions

Practice questions written in the style of SEAB exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Original6 marksExpress 1r(r+1)\dfrac{1}{r(r+1)} in partial fractions and hence find βˆ‘r=1n1r(r+1)\displaystyle\sum_{r=1}^{n} \dfrac{1}{r(r+1)}. Deduce the sum to infinity.
Show worked answer β†’

Partial fractions: 1r(r+1)=1rβˆ’1r+1\dfrac{1}{r(r+1)} = \dfrac{1}{r} - \dfrac{1}{r+1}.

The sum telescopes:
βˆ‘r=1n(1rβˆ’1r+1)=(1βˆ’12)+(12βˆ’13)+β‹―+(1nβˆ’1n+1)\sum_{r=1}^{n}\left(\dfrac{1}{r} - \dfrac{1}{r+1}\right) = \left(1 - \tfrac{1}{2}\right) + \left(\tfrac{1}{2} - \tfrac{1}{3}\right) + \cdots + \left(\tfrac{1}{n} - \tfrac{1}{n+1}\right).

All interior terms cancel, leaving 1βˆ’1n+1=nn+11 - \dfrac{1}{n+1} = \dfrac{n}{n+1}.

As nβ†’βˆžn \to \infty, 1n+1β†’0\dfrac{1}{n+1} \to 0, so the sum to infinity is 11.

Markers reward the partial fractions, showing the cancellation explicitly, the closed form nn+1\dfrac{n}{n+1}, and the limit.

Original5 marksGiven that 1rβˆ’1r+2=2r(r+2)\dfrac{1}{r} - \dfrac{1}{r+2} = \dfrac{2}{r(r+2)}, find βˆ‘r=1n1r(r+2)\displaystyle\sum_{r=1}^{n} \dfrac{1}{r(r+2)}.
Show worked answer β†’

From the identity, 1r(r+2)=12(1rβˆ’1r+2)\dfrac{1}{r(r+2)} = \dfrac{1}{2}\left(\dfrac{1}{r} - \dfrac{1}{r+2}\right).

The sum is 12βˆ‘r=1n(1rβˆ’1r+2)\dfrac{1}{2}\sum_{r=1}^{n}\left(\dfrac{1}{r} - \dfrac{1}{r+2}\right). Because the gap is 22, two terms survive at each end:

=12[(1+12)βˆ’(1n+1+1n+2)]=12[32βˆ’1n+1βˆ’1n+2]= \dfrac{1}{2}\left[\left(1 + \tfrac{1}{2}\right) - \left(\tfrac{1}{n+1} + \tfrac{1}{n+2}\right)\right] = \dfrac{1}{2}\left[\dfrac{3}{2} - \dfrac{1}{n+1} - \dfrac{1}{n+2}\right].

So the sum is 34βˆ’12(n+1)βˆ’12(n+2)\dfrac{3}{4} - \dfrac{1}{2(n+1)} - \dfrac{1}{2(n+2)}.

Markers reward the factor 12\frac{1}{2}, correctly identifying that two terms survive at each end (gap of two), and the closed form.

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