Find's Treasure Forums

Welcome to Find's Treasure Forums, Guests!

You are viewing this forums as a guest which limits you to read only status.

Only registered members may post stories, questions, classifieds, reply to other posts, contact other members using built in messaging and use many other features found on these forums.

Why not register and join us today? It's free! (We don't share your email addresses with anyone.) We keep email addresses of our users to protect them and others from bad people posting things they shouldn't.

Click here to register!



Need Support Help?

Cannot log in?, click here to have new password emailed to you

Changed email? Forgot to update your account with new email address? Need assistance with something else?, click here to go to Find's Support Form and fill out the form.

depths on various metals

A

Anonymous

Guest
Hi Eric,
I was reading the specs on the Deepstar and noticed the ranges: US Nickel: 14 inches US Quarter: 13 inches
This seems strange, since a quarter is much bigger than a nickel, it would seem to have a much larger cross section and seemingly should be able to be detected much deeper than the nickel, not to mention it being clad and higher conductivity seems like that should help too.
Is it because the deepstar is tuned to smaller, low conductivity items, or is there something about the quarter or deepstar to behave this way?
Thanks,
-jeff
 
Hi Jeff,
It is the characteristics of both the object and the detector that gives this strange result. Dealing with the object first. One of the fundamental laws of electromagnetics is that any change in equilibrium is resisted. If you change a magnetic field, as happens at the end of the TX pulse, then eddy currents will flow to try and maintain the field at its original value. In the absence of a metal object, the coil will produce a very high voltage in an attempt to jump between the ends of the coil and maintain the field. Hence the back emf. If there is a metal object, then a small portion of the field is coupled to the object and on field removal, currents are set up in the object to try and maintain this local field. For a metal with a relatively high resistance (nickel) the emf necessary to set up the current to maintain the field is higher than for a lower resistance metal (quarter). This results in a higher signal initially for the nickel, but which decays quicker due to the resistive losses. For the quarter, the initial signal amplitude is lower but due to the lower resistance, carries on for longer. It
 
Top