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propagation constant

 1. (¼ÛÀü¼±·Î Äڷγª¹æÀü ¹× ¹«¼±ÀâÀ½) ÁÖ¾îÁø ÁÖÆļö¿¡¼­ ÁøÇàÆÄÀÇ ÀüÆÄ»ó¼ö´Â º¹¼Ò·®À¸·Î¼­, ½Ç¼öºÎ´Â ´ÜÀ§ ±æÀÌ ´ç ³×ÆÛ(neper)·Î °¨¼è»ó¼öÀ̸ç, Çã¼öºÎ´Â ´ÜÀ§ ±æÀÌ ´ç ¶óµð¾È(radian)À¸·Î À§»ó»ó¼öÀÌ´Ù.
 2. (ÀüÆÄ º¹»ç) ±ÕÀÏ ¸ÅÁú¿¡ ÀÖ´Â ÁøÇàÆÄÀÇ ÀüÆÄ»ó¼ö´Â ÀüÆĸ¦ Ç¥ÇöÇÏ´Â ÆäÀÌÀú ·®ÀÇ ÀüÆÄ ¹æÇ⠰Ÿ®¿¡ ´ëÇÑ ´ë¼öÀû ÆíµµÇÔ¼öÀÇ À½ÀÌ´Ù. ÁÖ : ¿øÅëÇü ¶Ç´Â ±¸Çü ÁøÇàÆÄÀÇ °æ¿ì¿¡ À־, ÁøÆøÀÎÀÚ °ú 1/r Àº °¢°¢ ÆäÀÌÀú ·®¿¡ Æ÷ÇÔµÇÁö ¾Ê´Â´Ù.
 3. (µµÆÄ°ü) ÁÖÆļö¿Í ¸ðµå°¡ ÁÖ¾îÁø ÁøÇàÆÄ¿¡¼­, ½Ç¼öºÎ°¡ Neper/m ´ÜÀ§ÀÇ °¨¼è»ó¼öÀÌ°í Çã¼öºÎ°¡ radian/m ´ÜÀ§ÀÇ À§»ó»ó¼öÀÎ º¹¼Ò·®.
 4. (Àü¼Û¼±·Î ¹× Æ®·£½ºµà¼­) A) (±ÕÀÏ ¼±·ÎÀÇ ´ÜÀ§±æÀÌ´ç) ¼±·ÎÀÇ ±æÀÌ°¡ ¹«ÇÑÇϰųª ¼±·ÎÀÇ Æ¯¼ºÀÓÇÇ´ø½º·Î Á¾´ÜµÉ ¶§, ¼±·ÎÀÇ ÇÑ ÁöÁ¡¿¡¼­ÀÇ ÆäÀÌÀúÀü·ù¿Í ¼±·ÎÀÇ Àü¼Û¹æÇâÀ» µû¶ó óÀ½ ÁöÁ¡À¸·ÎºÎÅÍ ´ÜÀ§ °Å¸®¸¸Å­ ¶³¾îÁø µÎ ¹ø° ÁöÁ¡¿¡¼­ ÆäÀÌÀúÀü·ù¿ÍÀÇ ÀÚ¿¬´ë¼öºñ. B) (Áֱ⼺ ¼±·ÎÀÇ ´Ü¸é´ç) Áֱ⼺ ¼±·ÎÀÇ ±æÀÌ°¡ ¹«ÇÑÇϰųª ±× ¹Ýº¹ÀÓÇÇ´ø½º·Î Á¾´ÜµÉ ¶§, ÀÓÀÇÀÇ ´Ü¸éÀ¸·Î µé¾î°¡´Â ÆäÀÌÀú Àü·ù¿Í °°Àº ´Ü¸éÀ¸·ÎºÎÅÍ ³ª¿À´Â ÆäÀÌÀú Àü·ù¿ÍÀÇ ÀÚ¿¬´ë¼öºñÀÌ´Ù. C) (Àü±â º¯È¯±â) º¯È¯±â°¡ ±×°ÍÀÇ ¹Ýº¹ ÀÓÇÇ´ø½º·Î Á¾´ÜµÉ ¶§ º¯È¯±â·Î µé¾î°¡´Â ÆäÀÌÀú  Àü·ù¿Í º¯È¯±â·ÎºÎÅÍ ³ª¿À´Â ÆäÀÌÀú Àü·ù¿ÍÀÇ ÀÚ¿¬´ë¼öºñÀÌ´Ù.
 5. ÁÖ¾îÁø ÁÖÆļö¿¡¼­ ½Ãº¯ Á¤Çö ÀüÀÚÆĸðµå¿¡¼­, ÁÖ¾îÁø ¹æÇâÀÇ °Å¸®¿¡ µû¸¥ ÀüÀÚ±âÀå ¼ººÐ º¹¼ÒÁøÆøÀÇ ´ë¼öÀû º¯È­À². ÁÖ : ÀüÆÄ»ó¼ö ¥ë ´Â ¥ë=  ¥á+i¥â ·Î ÁÖ¾îÁö´Â º¹¼Ò·®À̸ç, ¿©±â¼­ ½Ç¼öºÎ ¥á ´Â °¨¼è»ó¼ö, Çã¼öºÎ ¥â ´Â À§»ó»ó¼öÀÌ´Ù.
 1.(overhead-power-line corona and radio noise) The propagation constant of a traveling plane wave at a given frequency is the complex quantity whose real part is the attenuation constant in nepers per unit length and whose imaginary part is the phase constant in radians per unit length. IEEE Std. 539-1972.
 2. (radio wave propagation). Of a traveling wave in a homogeneous medium, the negative of the partial logarithmic derivative, with respect to distance in the direction of the wave, of the phasor quantity describing the wave. Note: In the case of cylindrical or spherical traveling waves, the amplitude factors and 1/r, respectively, are not to be included in the phasor quantity. IEEE Std. 211-1973.
 3. (waveguide) Of a traveling wave at a given frequency and for a given mode, the complex quantity whose real part  is the attenuation constant in nepers per unit length and whose imaginary part is the phase constant in radians per unit length. IEEE Std. 146-1984.
 4. (transmission lines and transducers) (A) (per unit length of a uniform line) The natural logarithm of the ratio of the phasor current at a point of the line, to the phasor current at a second point, at  unit distance from the first point along the line in  the direction of transmission, when  the line is   infinite in length or is terminated in its characteristic impedance. (B) (per section of a periodic line). The natural logarithm of the ratio of the phasor current entering a section, to the phasor current leaving the same section, when the periodic line is infinite in length or is terminated in its iterative impedance. (C) (of an electric transducer). The natural logarithm of the ratio of  the phasor current entering the transducer, to the phasor current leaving the transducer, when the transducer is terminated in its iterative impedance.  IEEE Std. 270-1966
 5. For an electromagnetic field mode varying sinusoidally with time at a given frequency, the logarithmic rate of change, with respect to distance in a given direction, of the complex amplitude of any field component. Note: The propagation constant, ¥ë, is a complex quantity given by  ¥ë=  ¥á+i¥â, where ¥á, the real part, is the attenuation constant and ¥â, the imaginary part, is the phase constant.
http://www.its.bldrdoc.gov/fs-1037/