Chapter 6: Problem 3
Prove that $$ \sum_{1}^{N} n(n+1)(n+2)=\frac{1}{4} N(N+1)(N+2)(N+3) $$
Short Answer
Step by step solution
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none}
Learning Materials
Features
Discover
Chapter 6: Problem 3
Prove that $$ \sum_{1}^{N} n(n+1)(n+2)=\frac{1}{4} N(N+1)(N+2)(N+3) $$
These are the key concepts you need to understand to accurately answer the question.
All the tools & learning materials you need for study success - in one app.
Get started for free
Based on the way that integration is defined and that, to within a small additive constant, \(\int_{1}^{N} n^{r} d n \approx(r+1)^{-1} N^{r+1}\), we might expect that \(\sum_{1}^{N} n \approx \frac{1}{2} N^{2} ;\) in fact, it is \(\frac{1}{2} N(N+1)\). Similarly, we might expect that \(\sum_{1}^{N} n^{2} \approx \frac{1}{3} N^{3}\). Assume that $$ S_{N}=\sum_{n=1}^{N} n^{2}=\alpha N(N+a)(N+b) $$ with \(a\) and \(b\) constants and \(\alpha\) a fraction between 0 and 1 . By explicitly evaluating \(S_{N}\) for \(N=1,2\) and 3 , obtain three equations relating \(a, b\) and \(\alpha\) and solve them. Note that this is not a general proof of the form of \(S_{N} ;\) it merely proposes a possible form. For a proof that establishes the validity of the proposal for all \(N\), either the method of induction or that used in the main text has to be employed.
Prove that $$ \cos \theta+\cos (\theta+\alpha)+\cdots+\cos (\theta+n \alpha)=\frac{\sin \frac{1}{2}(n+1) \alpha}{\sin \frac{1}{2} \alpha} \cos \left(\theta+\frac{1}{2} n \alpha\right) $$
Find the first three non-zero terms in the Maclaurin series for the following functions: (a) \(\left(x^{2}+9\right)^{-1 / 2}\) (b) \(\ln \left[(2+x)^{3}\right]\) (c) \(\exp (\sin x)\), (d) \(\ln (\cos x)\) (e) \(\exp \left[-(x-a)^{-2}\right]\) (f) \(\tan ^{-1} x\).
If you invest \(£ 1000\) on the first day of each year and interest is paid at \(5 \%\) on your balance at the end of each year, how much money do you have after 25 years?
In a very simple model of a crystal, point-like atomic ions are regularly spaced along an infinite one-dimensional row with spacing \(R\). Alternate ions carry equal and opposite charges \(\pm e\). The potential energy of the \(i\) th ion in the electric field due to another ion, the \(j\) th, is $$ \frac{q_{i} q_{j}}{4 \pi \epsilon_{0} r_{i j}} $$ where \(q_{i}, q_{j}\) are the charges on the ions and \(r_{i j}\) is the distance between them. Write down a series giving the total contribution \(V_{i}\) of the \(i\) th ion to the overall potential energy. Show that the series converges, and, if \(V_{i}\) is written as $$ V_{i}=\frac{\alpha e^{2}}{4 \pi \epsilon_{0} R} $$ find a closed-form expression for \(\alpha\), the Madelung constant for this (unrealistic) lattice.
What do you think about this solution?
We value your feedback to improve our textbook solutions.