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#1
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![]() "Ron Baker, Pluralitas!" wrote in message ... "Hein ten Horn" wrote in message ... Ron Baker, Pluralitas! wrote: "Hein ten Horn" wrote: Ron Baker, Pluralitas! wrote: Hein ten Horn wrote: Ron Baker, Pluralitas! wrote: Hein ten Horn wrote: As a matter of fact the resulting force (the resultant) is fully determining the change of the velocity (vector) of the element. The resulting force on our element is changing at the frequency of 222 Hz, so the matter is vibrating at the one and only 222 Hz. Your idea of frequency is informal and leaves out essential aspects of how physical systems work. Nonsense. Mechanical oscillations are fully determined by forces acting on the vibrating mass. Both mass and resulting force determine the frequency. It's just a matter of applying the laws of physics. You don't know the laws of physics or how to apply them. I'm not understood. So, back to basics. Take a simple harmonic oscillation of a mass m, then x(t) = A*sin(2*pi*f*t) v(t) = d(x(t))/dt = 2*pi*f*A*cos(2*pi*f*t) a(t) = d(v(t))/dt = -(2*pi*f)^2*A*sin(2*pi*f*t) hence a(t) = -(2*pi*f)^2*x(t) Only for a single sinusoid. and, applying Newton's second law, Fres(t) = -m*(2*pi*f)^2*x(t) or f = ( -Fres(t) / m / x(t) )^0.5 / (2pi). Only for a single sinusoid. What if x(t) = sin(2pi f1 t) + sin(2pi f2 t) In the following passage I wrote "a relatively slow varying amplitude", which relates to the 4 Hz beat in the case under discussion (f1 = 220 Hz and f2 = 224 Hz) where your expression evaluates to x(t) = 2 * cos(2pi 2 t) * sin(2pi 222 t), indicating the matter is vibrating at 222 Hz. So where did you apply the laws of physics? You said, "It's just a matter of applying the laws of physics." Then you did that for the single sine case. Where is your physics calculation for the two sine case? Where is the expression for 'f' as in your first example? Put x(t) = 2 * cos(2pi 2 t) * sin(2pi 222 t) in your calculations and tell me what you get for 'f'. And how do you get 222 Hz out of cos(2pi 2 t) * sin(2pi 222 t) Why don't you say it is 2 Hz? What is your law of physics here? Always pick the bigger number? Always pick the frequency of the second term? Always pick the frequency of the sine? What is "the frequency" of cos(2pi 410 t) * cos(2pi 400 t) What is "the frequency" of cos(2pi 200 t) + cos(2pi 210 t) + cos(2pi 1200 t) + cos(2pi 1207 t) So my statements above, in which we have a relatively slow varying amplitude (4 Hz), How do you determine amplitude? What's the math (or physics) to derive amplitude? are fundamentally spoken valid. Calling someone an idiot is a weak scientific argument. Yes. And so is "Nonsense." And so is your idea of "the frequency". Note the piquant difference: nonsense points to content and we're not discussing idiots (despite a passing by of some very strange postings. ![]() Hard words break no bones, yet deflate creditability. gr, Hein Well, I think I've had it. A 'never' ending story. Too much to straighten out. Too much comment needed. Questions moving away from the subject. No more indistinguishable close frequencies. No audible beat, no slow changing envelopes. Take a plot, use a high speed camera or whatever else and see for yourself the particle is vibrating at a period in accordance with 222 Hz. In my view I've sufficiently underpinned the 222 Hz frequency. If you disagree, then do the job. Show your frequencies and elucidate them. (No hint needed, I guess.) gr, Hein |
#2
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![]() "Hein ten Horn" wrote in message ... "Ron Baker, Pluralitas!" wrote in message ... "Hein ten Horn" wrote in message ... Ron Baker, Pluralitas! wrote: "Hein ten Horn" wrote: Ron Baker, Pluralitas! wrote: Hein ten Horn wrote: Ron Baker, Pluralitas! wrote: Hein ten Horn wrote: As a matter of fact the resulting force (the resultant) is fully determining the change of the velocity (vector) of the element. The resulting force on our element is changing at the frequency of 222 Hz, so the matter is vibrating at the one and only 222 Hz. Your idea of frequency is informal and leaves out essential aspects of how physical systems work. Nonsense. Mechanical oscillations are fully determined by forces acting on the vibrating mass. Both mass and resulting force determine the frequency. It's just a matter of applying the laws of physics. You don't know the laws of physics or how to apply them. I'm not understood. So, back to basics. Take a simple harmonic oscillation of a mass m, then x(t) = A*sin(2*pi*f*t) v(t) = d(x(t))/dt = 2*pi*f*A*cos(2*pi*f*t) a(t) = d(v(t))/dt = -(2*pi*f)^2*A*sin(2*pi*f*t) hence a(t) = -(2*pi*f)^2*x(t) Only for a single sinusoid. and, applying Newton's second law, Fres(t) = -m*(2*pi*f)^2*x(t) or f = ( -Fres(t) / m / x(t) )^0.5 / (2pi). Only for a single sinusoid. What if x(t) = sin(2pi f1 t) + sin(2pi f2 t) In the following passage I wrote "a relatively slow varying amplitude", which relates to the 4 Hz beat in the case under discussion (f1 = 220 Hz and f2 = 224 Hz) where your expression evaluates to x(t) = 2 * cos(2pi 2 t) * sin(2pi 222 t), indicating the matter is vibrating at 222 Hz. So where did you apply the laws of physics? You said, "It's just a matter of applying the laws of physics." Then you did that for the single sine case. Where is your physics calculation for the two sine case? Where is the expression for 'f' as in your first example? Put x(t) = 2 * cos(2pi 2 t) * sin(2pi 222 t) in your calculations and tell me what you get for 'f'. And how do you get 222 Hz out of cos(2pi 2 t) * sin(2pi 222 t) Why don't you say it is 2 Hz? What is your law of physics here? Always pick the bigger number? Always pick the frequency of the second term? Always pick the frequency of the sine? What is "the frequency" of cos(2pi 410 t) * cos(2pi 400 t) What is "the frequency" of cos(2pi 200 t) + cos(2pi 210 t) + cos(2pi 1200 t) + cos(2pi 1207 t) So my statements above, in which we have a relatively slow varying amplitude (4 Hz), How do you determine amplitude? What's the math (or physics) to derive amplitude? are fundamentally spoken valid. Calling someone an idiot is a weak scientific argument. Yes. And so is "Nonsense." And so is your idea of "the frequency". Note the piquant difference: nonsense points to content and we're not discussing idiots (despite a passing by of some very strange postings. ![]() Hard words break no bones, yet deflate creditability. gr, Hein Well, I think I've had it. A 'never' ending story. Too much to straighten out. Too much comment needed. Questions moving away from the subject. No more indistinguishable close frequencies. No audible beat, no slow changing envelopes. Take a plot, use a high speed camera or whatever else and see for yourself the particle is vibrating at a period in accordance with 222 Hz. In my view I've sufficiently underpinned the 222 Hz frequency. If you disagree, then do the job. Show your frequencies and elucidate them. (No hint needed, I guess.) gr, Hein Bravo. Well done. What an impressive display of applying the laws of physics. Newton, Euler, Gauss, and Fourier have nothing on you. |
#3
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![]() "Ron Baker, Pluralitas!" wrote in message news:469db833$0$20583 "Hein ten Horn" wrote in message "Ron Baker, Pluralitas!" wrote in message "Hein ten Horn" wrote in message Ron Baker, Pluralitas! wrote: "Hein ten Horn" wrote: Ron Baker, Pluralitas! wrote: Hein ten Horn wrote: Ron Baker, Pluralitas! wrote: Hein ten Horn wrote: As a matter of fact the resulting force (the resultant) is fully determining the change of the velocity (vector) of the element. The resulting force on our element is changing at the frequency of 222 Hz, so the matter is vibrating at the one and only 222 Hz. Your idea of frequency is informal and leaves out essential aspects of how physical systems work. Nonsense. Mechanical oscillations are fully determined by forces acting on the vibrating mass. Both mass and resulting force determine the frequency. It's just a matter of applying the laws of physics. You don't know the laws of physics or how to apply them. I'm not understood. So, back to basics. Take a simple harmonic oscillation of a mass m, then x(t) = A*sin(2*pi*f*t) v(t) = d(x(t))/dt = 2*pi*f*A*cos(2*pi*f*t) a(t) = d(v(t))/dt = -(2*pi*f)^2*A*sin(2*pi*f*t) hence a(t) = -(2*pi*f)^2*x(t) Only for a single sinusoid. and, applying Newton's second law, Fres(t) = -m*(2*pi*f)^2*x(t) or f = ( -Fres(t) / m / x(t) )^0.5 / (2pi). Only for a single sinusoid. What if x(t) = sin(2pi f1 t) + sin(2pi f2 t) In the following passage I wrote "a relatively slow varying amplitude", which relates to the 4 Hz beat in the case under discussion (f1 = 220 Hz and f2 = 224 Hz) where your expression evaluates to x(t) = 2 * cos(2pi 2 t) * sin(2pi 222 t), indicating the matter is vibrating at 222 Hz. So where did you apply the laws of physics? You said, "It's just a matter of applying the laws of physics." Then you did that for the single sine case. Where is your physics calculation for the two sine case? Where is the expression for 'f' as in your first example? Put x(t) = 2 * cos(2pi 2 t) * sin(2pi 222 t) in your calculations and tell me what you get for 'f'. And how do you get 222 Hz out of cos(2pi 2 t) * sin(2pi 222 t) Why don't you say it is 2 Hz? What is your law of physics here? Always pick the bigger number? Always pick the frequency of the second term? Always pick the frequency of the sine? What is "the frequency" of cos(2pi 410 t) * cos(2pi 400 t) What is "the frequency" of cos(2pi 200 t) + cos(2pi 210 t) + cos(2pi 1200 t) + cos(2pi 1207 t) So my statements above, in which we have a relatively slow varying amplitude (4 Hz), How do you determine amplitude? What's the math (or physics) to derive amplitude? are fundamentally spoken valid. Calling someone an idiot is a weak scientific argument. Yes. And so is "Nonsense." And so is your idea of "the frequency". Note the piquant difference: nonsense points to content and we're not discussing idiots (despite a passing by of some very strange postings. ![]() Hard words break no bones, yet deflate creditability. Well, I think I've had it. A 'never' ending story. Too much to straighten out. Too much comment needed. Questions moving away from the subject. No more indistinguishable close frequencies. No audible beat, no slow changing envelopes. Take a plot, use a high speed camera or whatever else and see for yourself the particle is vibrating at a period in accordance with 222 Hz. In my view I've sufficiently underpinned the 222 Hz frequency. If you disagree, then do the job. Show your frequencies and elucidate them. (No hint needed, I guess.) Bravo. Well done. What an impressive display of applying the laws of physics. Newton, Euler, Gauss, and Fourier have nothing on you. Thanks for your constructive contributions. gr, Hein |
#4
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![]() How do you determine amplitude? What's the math (or physics) to derive amplitude? The fundamental formular Acos(B) + C is all you need to describe angular modulation. Changing the value of A over time determines the amplitude of an AM modulated carrier. Changing the value of B over time determines the amplitude of an FM modulated carrier. The rate of change of A or B changes the modulation frequency respectively. C is DC, Y axis offset and has not been discussed here. r, Bob F. |
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