|
|||||||
| Home | Forums | Rules | Articles | Store | Gallery | Blogs | Register | Donations | FAQ | Calendar | Search | Today's Posts | Mark Forums Read | Search |
| Solid State Talk all about solid state amplification. |
|
Please consider donating to help us continue to serve you.
Ads on/off / Custom Title / More PMs / More album space / Advanced printing & mass image saving |
|
|
|
Thread Tools | Search this Thread |
|
|
#31 | |
|
diyAudio Member
Join Date: Jun 2004
Location: Warsaw
|
Quote:
QED047 I meant a buck regulator of audio bandwidth tracking output signal and thus keeping the Vds at constant low value. Yes, that's nearly a class D amp, but why are you afraid of doing something that you seem to be more then competent to do? |
|
|
|
|
|
#32 | |
|
diyAudio Member
Join Date: May 2009
|
Quote:
Also, as I said before, all the Class D designs I have encountered depend on negative feedback to account for non-linearities in conversion and variations in load. I seem to be particularly sensitive to IM distortion so I try to avoid feedback although I won't pretend to understand what's going on in this department. |
|
|
|
|
|
#33 | |
|
diyAudio Member
Join Date: Aug 2004
Location: Behind you
|
Quote:
__________________
http://mrevil.pwp.blueyonder.co.uk/ |
|
|
|
|
|
#34 |
|
diyAudio Member
Join Date: Feb 2005
Location: Copenhagen
|
QED047 : thanks for the extended explanation, wich also clarifies the oscillator question, and thanks to Darkfenriz for supporting that.
But what I still don't get is: Where do the power go? It pulls 2A, but only dissipate 1W so the DC point at the followers source is ½volt or ...? The coil must take some of the heat also.
__________________
STOP - Hammertime! |
|
|
|
|
#35 | |
|
diyAudio Member
Join Date: Oct 2008
|
Quote:
|
|
|
|
|
|
#36 | |
|
diyAudio Member
Join Date: May 2009
|
Quote:
When stinius replies "Yes of course" it is of course true that a real inductor (as opposed to a theoretical, resistance free device) will dissipate some power as heat - but this is a small percentage (part of the 10% losses) of that which is usually lost in a convenional current sink. This is the point I think you may be missing:- while the follower "sees" what appears to be a resistive element "inside" the Constant Current circuit - the power is actually going into charging up a magnetic field. When the transistor connecting the inductor to ground opens, the magnetic field collapses - generating a potential (at the switch/inductor junction) that is conducted back into the supply reservoir via the diode. Hence the unwanted power that would have otherwise gone out as heat in a linear CC circuit is restored back to the supply and reused (well, around 90% of it anyway). I think you may be unused to considering power "stored" in a magnetic field. If you look at the junction between the inductor and the transistor to ground with a scope you will see the node alternating between ground and the supply rail in a rigid square wave. If the diode was disconnected the voltage at this node would go way up (until it reached the breakdown voltage of the transistor!) - but the diode dumps it all into the supply - which keeps the lid on the voltage raise. This last point presents a slight design challenge (easily overcome) as any inductance between where the diode dumps its potential and the resevoir caps may "pump up" the supply rail locally - but by returning the diode cathode to the reservoir directly, and having plenty of low ESR caps there (and maybe a little resistive/inductive filtering to allow the volts out into the amplifier in a more orderly fashion) we can easily get around this. If you play around with a buck voltage regulator instead of a linear regulator, you get used to watching the current from your bench supply go down as you wind up the output voltage - hence the power (V x I) stays put. With a linear regulator the current stays put as you wind up the voltage (you hope!) so the power dissipated goes up. I guess you need to watch these things first-hand to get the feel for it. I remember scratching my head a bit when I first met switching topologies
|
|
|
|
|
|
#37 |
|
diyAudio Member
Join Date: Jun 2004
Location: Warsaw
|
Hi QED047
Sorry if you find me pestering, but I have a question, that came to mind: How does it behave at negative side overdrive? To my understanding the switching frequency should go down with output voltage because of less steep current ramp. Isn't there a point at which the switching frequency falls into audio range? |
|
|
|
|
#38 | |
|
diyAudio Member
Join Date: Dec 2005
Location: Belgium
|
Quote:
|
|
|
|
|
|
#39 | ||
|
diyAudio Member
Join Date: Oct 2008
|
Quote:
Quote:
|
||
|
|
|
|
#40 | |
|
diyAudio Member
|
Quote:
__________________
"The test of the machine is the satisfaction it gives you. There isn't any other test. If the machine produces tranquility it's right. If it disturbs you it's wrong until either the machine or your mind is changed." Robert M Pirsig. |
|
|
|
| Currently Active Users Viewing This Thread: 1 (0 members and 1 guests) | |
| Thread Tools | Search this Thread |
|
|
|
|
||||
| Thread | Thread Starter | Forum | Replies | Last Post |
| New class A biasing (with non-switching class AB overflow) | Steven | Solid State | 34 | 24th March 2007 07:40 PM |
| Quick question - possible to build high-power current-source Class D amp? | 454Casull | Class D | 2 | 24th November 2006 11:48 PM |
| Aleph-type current source, but source follower this time | tschrama | Pass Labs | 4 | 29th July 2005 01:55 PM |
| switching regulator as a current source | SS | Parts | 13 | 10th February 2004 02:58 PM |
| Source follower electret mike -> use with current source? | capslock | Solid State | 1 | 28th February 2003 01:54 PM |
| New To Site? | Need Help? |
| Page generated in 0.15708 seconds (80.90% PHP - 19.10% MySQL) with 11 queries |