Path: utzoo!utgpu!news-server.csri.toronto.edu!cs.utexas.edu!hellgate.utah.edu!dog.ee.lbl.gov!ucbvax!pasteur!galileo.berkeley.edu!jbuck From: jbuck@galileo.berkeley.edu (Joe Buck) Newsgroups: sci.electronics Subject: Re: A question about the Nyquist theorm Keywords: Nyquist Theorem Message-ID: <11577@pasteur.Berkeley.EDU> Date: 1 Mar 91 20:29:16 GMT References: <20408@shlump.nac.dec.com> <625@ctycal.UUCP> <11515@pasteur.Berkeley.EDU> <1347@cameron.egr.duke.edu> Sender: news@pasteur.Berkeley.EDU Reply-To: jbuck@galileo.berkeley.edu (Joe Buck) Lines: 22 In article <1347@cameron.egr.duke.edu>, rea@egr.duke.edu (Rana E. Ahmed) writes: |> Suppose we sample a pure sine wave of frequency 'f' at the Nyquist rate, |> i.e., at 2f samples/sec (exact), such that we start sampling the sine wave |> at the time of its zero crossing. Thus, if we assume uniform sampling, |> then all subsequent samples will have values equal to zero, i.e., x[m]=0 for |> all m (Assuming instantaneous sampling, i.e., no Hold Time for samples). |> Intutively, if we pass these samples (each of zero voltage (say)) through an |> ideal low-pass filter, then we should expect to get zero voltage at the output |> of filter. In other words, reconstructed signal voltage =0 for all t. |> (see also the formula for x(t) above ). |> How can we recover the pure sine in this sampling strategy? |> Am I missing something ?? Yes. The theorem has a "<" and you're assuming "<=". Sampling produces aliasing. If the Nyquist frequency is f, then a sine wave at frequency q looks exactly like a sine wave at frequency q+mf, where m is any integer. So if you want to recover your sine wave at frequency f, sampling at 2f isn't enough: you need 2f + delta (for an arbitrarily small delta). -- Joe Buck jbuck@galileo.berkeley.edu {uunet,ucbvax}!galileo.berkeley.edu!jbuck