Hello Ankit, When you terminate your TL by a short (in EM theory they call it "perfectly electric conductor"- PEC), your tangential electric field has to be zero. The only way for that to happen is if your incident wave has a value of, say, +a, your reflected wave has to have -a (the tangential component). That way, at your short (PEC) you have a minimum (zero). That is not true for the magnetic component. As a matter of fact, the short is where you magnetic field (tangential) is maximum. Hence, they have to be completely out of phase. The same argument is true if you terminate your TL with a (perfect) open, but this time you flip who is zero and who is max. If you want, you can also see this from a circuit point of view: if you terminate with a short, you can not have any voltage, right? That is electric field. But the current will be very large (maximum, in fact). That is magnetic field. And if it is open, there is no current (zero magnetic field) but large voltage (electric field). If you want more info, any undergrad level EM book should have this (Ramo, Shadiku, Pozar, etc.). I hope it helps. Regards, Davi ________________________________ From: Ankit wangoo <ankit.wangoo@xxxxxxxxx> To: si-list@xxxxxxxxxxxxx Sent: Sunday, March 3, 2013 8:16 PM Subject: [SI-LIST] TEM wave propagation and standing waves Hi We all know in transmission line structures such as co-axial cables, strip-line and micro strip-lines(partially ,if we assume field lines remains inside the dielectric) , electromagnetic energy flows in TEM mode, that is electric and magnetic field are always perpendicular to each other. We also know that characteristics of TEM waves guided by transmission lines are same as those for uniform plan wave propagating in an unbound dielectric medium. When we solve Helmholtz equation we find that Electric field can have one of solution as E=a*e^j(wt-kz) + b*e^j(wt+kz). where first term is a forward travelling wave and send is backward travelling wave. From Ampere circuital law in point form , we can find that H, jw*mu**H*Þl cross *E* . Then H some out to be in phase with E field .That means that at a particular position and at particular time when electric field is maximum , magnetic field will also be maximum. however , when we study standing wave in transmission line which is terminated by short.We find that current (magnetic field ) and Voltage (electric field) are actually completely out of phase. when current is max, voltage is zero and vice-versa What can explain this difference in analysis ? I was thinking more about this,,, standing waves are formed by two waves and each of them electric field and magnetic field are in phase.however in standing wave , because of reflection one of them get polarized in different direction such that some points electric field gets cancelled and some point magnetic field get cancelled. however ,i am not completely convinced.Can somebody shed some light on this or refer me to some appropriate reading material? Thanks for your help Ankit wangoo ------------------------------------------------------------------ To unsubscribe from si-list: si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field or to administer your membership from a web page, go to: //www.freelists.org/webpage/si-list For help: si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field List forum is accessible at: http://tech.groups.yahoo.com/group/si-list List archives are viewable at: //www.freelists.org/archives/si-list Old (prior to June 6, 2001) list archives are viewable at: http://www.qsl.net/wb6tpu ------------------------------------------------------------------ To unsubscribe from si-list: si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field or to administer your membership from a web page, go to: //www.freelists.org/webpage/si-list For help: si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field List forum is accessible at: http://tech.groups.yahoo.com/group/si-list List archives are viewable at: //www.freelists.org/archives/si-list Old (prior to June 6, 2001) list archives are viewable at: http://www.qsl.net/wb6tpu