Difference between revisions of "Doppler effect"
From Encyclopedia of Mathematics
(Importing text file) |
Ulf Rehmann (talk | contribs) m (tex encoded by computer) |
||
| Line 1: | Line 1: | ||
| + | <!-- | ||
| + | d0338501.png | ||
| + | $#A+1 = 16 n = 0 | ||
| + | $#C+1 = 16 : ~/encyclopedia/old_files/data/D033/D.0303850 Doppler effect | ||
| + | Automatically converted into TeX, above some diagnostics. | ||
| + | Please remove this comment and the {{TEX|auto}} line below, | ||
| + | if TeX found to be correct. | ||
| + | --> | ||
| + | |||
| + | {{TEX|auto}} | ||
| + | {{TEX|done}} | ||
| + | |||
The change in the received frequency of vibration with the speed of motion of the source of the vibration with respect to the observer or vice versa. If the distance between the source and the observer decreases, the frequency increases; if it increases, the frequency decreases. All types of waves give the Doppler effect: sound waves, elastic waves and electromagnetic waves. | The change in the received frequency of vibration with the speed of motion of the source of the vibration with respect to the observer or vice versa. If the distance between the source and the observer decreases, the frequency increases; if it increases, the frequency decreases. All types of waves give the Doppler effect: sound waves, elastic waves and electromagnetic waves. | ||
| − | Let | + | Let $ x ^ {j} $ |
| + | and $ {\overline{x}\; } {} ^ {j} $, | ||
| + | where $ j = 0 , 1 , 2 , 3 , $ | ||
| + | and $ x ^ {0} = t $, | ||
| + | $ {\overline{x}\; } {} ^ {0} = \overline{t}\; $ | ||
| + | are the time, be the inertial reference systems of the source of an electromagnetic wave and of the observer. Further, let the phase multiplier of the plane wave have the form $ \mathop{\rm exp} ( i \omega _ {j} x ^ {j} ) $ | ||
| + | and $ \mathop{\rm exp} ( i {\overline \omega \; } _ {j} {\overline{x}\; } {} ^ {j} ) $ | ||
| + | in the first and second reference frame, respectively. The Doppler effect is then expressed by a formula relating the time components (frequencies) $ \omega _ {0} $ | ||
| + | and $ {\overline \omega \; } _ {0} $ | ||
| + | of the four-dimensional wave vectors $ \{ \omega _ {j} \} $ | ||
| + | and $ \{ {\overline \omega \; } _ {j} \} $: | ||
| − | + | $$ | |
| + | {\overline \omega \; } _ {0} = \omega _ {0} | ||
| + | \frac{\sqrt {1 - v ^ {2} / c ^ {2} } }{1 - ( v / c) \cos \phi } | ||
| + | . | ||
| + | $$ | ||
| − | Here | + | Here $ v $ |
| + | is the relative velocity between the source and the observer, $ \phi $ | ||
| + | is the angle between the velocity $ v $ | ||
| + | and the line of observation measured in the system of the observer, and $ c $ | ||
| + | is the velocity of light in vacuum. | ||
The effect was named after Ch. Doppler who was the first to predict it theoretically (1842). | The effect was named after Ch. Doppler who was the first to predict it theoretically (1842). | ||
| Line 11: | Line 41: | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> L.D. Landau, E.M. Lifshitz, "The classical theory of fields" , Addison-Wesley (1951) pp. Chapt. 6 (Translated from Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> S.E. Frish, A.V. Timoreva, "A course in general physics" , '''1''' , Moscow (1962) pp. Chapt. 12 (In Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> L.D. Landau, E.M. Lifshitz, "The classical theory of fields" , Addison-Wesley (1951) pp. Chapt. 6 (Translated from Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> S.E. Frish, A.V. Timoreva, "A course in general physics" , '''1''' , Moscow (1962) pp. Chapt. 12 (In Russian)</TD></TR></table> | ||
| − | |||
| − | |||
====Comments==== | ====Comments==== | ||
| − | |||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> E.T. Whittaker, "A history of the theories of aether and electricity" , '''I Chapt. XII, p. 368; Vol. II Chapt. II, p. 40–42 & Chapt. III, p. 92''' , Harper Torchbooks (1960)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> J.W.S. Rayleigh, "The theory of sound" , '''II''' , Dover, reprint (1945) pp. 154–156</TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> E.T. Whittaker, "A history of the theories of aether and electricity" , '''I Chapt. XII, p. 368; Vol. II Chapt. II, p. 40–42 & Chapt. III, p. 92''' , Harper Torchbooks (1960)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> J.W.S. Rayleigh, "The theory of sound" , '''II''' , Dover, reprint (1945) pp. 154–156</TD></TR></table> | ||
Latest revision as of 19:36, 5 June 2020
The change in the received frequency of vibration with the speed of motion of the source of the vibration with respect to the observer or vice versa. If the distance between the source and the observer decreases, the frequency increases; if it increases, the frequency decreases. All types of waves give the Doppler effect: sound waves, elastic waves and electromagnetic waves.
Let $ x ^ {j} $ and $ {\overline{x}\; } {} ^ {j} $, where $ j = 0 , 1 , 2 , 3 , $ and $ x ^ {0} = t $, $ {\overline{x}\; } {} ^ {0} = \overline{t}\; $ are the time, be the inertial reference systems of the source of an electromagnetic wave and of the observer. Further, let the phase multiplier of the plane wave have the form $ \mathop{\rm exp} ( i \omega _ {j} x ^ {j} ) $ and $ \mathop{\rm exp} ( i {\overline \omega \; } _ {j} {\overline{x}\; } {} ^ {j} ) $ in the first and second reference frame, respectively. The Doppler effect is then expressed by a formula relating the time components (frequencies) $ \omega _ {0} $ and $ {\overline \omega \; } _ {0} $ of the four-dimensional wave vectors $ \{ \omega _ {j} \} $ and $ \{ {\overline \omega \; } _ {j} \} $:
$$ {\overline \omega \; } _ {0} = \omega _ {0} \frac{\sqrt {1 - v ^ {2} / c ^ {2} } }{1 - ( v / c) \cos \phi } . $$
Here $ v $ is the relative velocity between the source and the observer, $ \phi $ is the angle between the velocity $ v $ and the line of observation measured in the system of the observer, and $ c $ is the velocity of light in vacuum.
The effect was named after Ch. Doppler who was the first to predict it theoretically (1842).
References
| [1] | L.D. Landau, E.M. Lifshitz, "The classical theory of fields" , Addison-Wesley (1951) pp. Chapt. 6 (Translated from Russian) |
| [2] | S.E. Frish, A.V. Timoreva, "A course in general physics" , 1 , Moscow (1962) pp. Chapt. 12 (In Russian) |
Comments
References
| [a1] | E.T. Whittaker, "A history of the theories of aether and electricity" , I Chapt. XII, p. 368; Vol. II Chapt. II, p. 40–42 & Chapt. III, p. 92 , Harper Torchbooks (1960) |
| [a2] | J.W.S. Rayleigh, "The theory of sound" , II , Dover, reprint (1945) pp. 154–156 |
How to Cite This Entry:
Doppler effect. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Doppler_effect&oldid=46765
Doppler effect. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Doppler_effect&oldid=46765
This article was adapted from an original article by V.M. BabichM.M. Popov (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article