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Applications for wide band rf transformers include = impedance=20 matching, voltage or current transformation, DC isolation, balanced / = unbalanced=20 mixing, matching, power splitting, coupling, and signal inversion. = Custom wide=20 band transformers with special combinations of impedance ratio, = insertion loss,=20 frequency response, and current handling are also = available."
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WIDE BAND RF TRANSFORMERS



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What are wide band rf transformers?

Wideband rf transformers are simply transfomers designed to provide = an=20 impedance transformation over a broad frequency range. In amateur radio=20 applications we wind these transformers on ferrite = toroids. A common impedance transformation is 200 ohms to 50 ohms = using a=20 bi-filar winding. Here is an example from our broad=20 band amplifiers tutorial.

3D"This=20

Figure 1. - wideband rf amplifier with shunt feedback and = emitter=20 degeneration

Transformer T1 is a broadband rf transformer.=20

Designing wide band rf transformers

In the design of these kinds of wide band rf transformers the primary = reactance is usually around 5 times the primary impeda= nce.=20 With a 200 ohms to 50 ohm transformer, we would allow a reactance of = 1,000 ohms=20 at the lowest frequency of interest. Just as an example consider = we were=20 building a broad band amplifier for the amateur bands and going down as = low as=20 1.8 Mhz.=20

For this example we would need bi-filar windings which have a reacta= nce=20 of 1,000 ohms at 1.8 Mhz, this means a required induc= tance=20 of around 88 uH. A look through the Amidon data book tells me that = ferrite=20 toroid FT-50-61 as one example can provide me with an AL factor of 68mH = / 1000=20 turns.=20

This means if 1,000 turns were wound on the toroid it would give us = 68 mH.=20 Yes that IS milli-henries, these are ferrite toroids.=20

Calculating turns for wide band rf transformers

To wind a wide band rf transformer with an inductance of 88 uH (yes = that's=20 micro-henries) which is in fact 0.088 mh we use the following formula:=20

Turns =3D 1,000 X SQRT (L in mH / AL factor) =   =3D   1,000 X=20 SQRT (0.088 / 68)   =3D   36 turns.=20

Our wide band rf transformer needs 36 turns to achieve an inductance = of 88=20 uH.=20

Winding the wide band rf transformer

Because this is a bi-filar winding for our wide band rf transformer, = we need=20 two lengths of wire which we will "twist" together at a "pitch" of 2.5 = turns per=20 inch or 1 turn per 10 mm. If you anchor one end of the two wires = together in a=20 bench vise and fix the other ends securely in a hand drill (a bent nail = or fish=20 hook helps here) you then gently "stretch" the wires first. Then you = slowly turn=20 the hand drill and notice the two wires "twisting" together, as you = proceed you=20 will notice more and more twists appearing. Stop when you have about 2.5 = twists=20 to the inch. Stretch the wires once more.=20

Wind 36 turns through the toroid and that is it! To use in an = application=20 such as figure 1 above you need to pay attention to the "phasing". = Notice the=20 two dots on T1 above? They indicate the start of each wire. Use = an=20 ohmmeter to find the start and finish of one winding, mark it in some = convenient=20 manner e.g. coloured pen. The other winding should then be obvious.=20

Commercially manufactured wide band rf transformers

Coilcraft is one manufacturer of wide band transformers which provide = reliable performance.=20

The transformers are offered in tapped or untapped configurations and = are=20 packaged in a low-profile DIP-style plastic case. All parts are = available in=20 either a surface mount version or a through-hole version that=92s = compatible with=20 standard DIP sockets.=20

Applications include impedance matching, voltage or current = transformation,=20 DC isolation, balanced / unbalanced mixing, matching, power splitting, = coupling,=20 and signal inversion. Custom wide band transformers with special = combinations of=20 impedance ratio, insertion loss, frequency response, and current = handling are=20 also available.=20

Designing wide band rf transformers for different impedances

Alright what if you need something other than a 200 ohm to 50 ohms=20 transformer, how would you go about it?=20

What I tell you here now is applicable from DC to daylight. What that = means=20 is, it is equally applicable to an audio transformer with a bandwidth of = 100 Hz=20 to 3,000 Hz (for an audio=20 transformer) as it is to a broadband transformer designed to operate = at say=20 7.00 to 7.50 Mhz. Read on.=20

Firstly you need to pick either a lower 1 dB or 3 dB bandwidth. = Wozzat???=20 Look at figure 2 below where I present my usual scungy drawing - I'm no = good at=20 this graphic arts caper, not the program, just my lack of artistic = talent.=20

3D"This=20

Figure 2. - band pass filter characteristics

Here I've crudely depicted a range of frequencies being passed by a = filter=20 and indicated the 1 dB and 3 db points. A 1 db point is where the power = output=20 is about 80% of the band pass power or 90% of the voltage level. A 3 db = point is=20 where the power output is about 50% of the band pass power or 70.7% of = the=20 voltage level. If you can't understand decibels then you need to look at = the decibel = page=20

In your broad band transformer you need to determine the lowest point = you can=20 tolerate in frequency. Entirely for discussion purposes I've selected 5 = Mhz for=20 both 1 dB and 3 dB to demonstrate the formulas. Also I'm going to = construct a =20 broad band tranformer to operate between 14.4 ohms and 50 ohms.=20

For the 1 db point to be 5 Mhz, I use the formula Lp =3D R / ( 2 X Pi = X Fo) and=20 for the 3 dB point, I use the formula Lp =3D R / ( 4 X Pi X Fo). The = general=20 formula for any other dB level is a bit difficult to reproduce here but = contact = me and I'll give it to anyone who wants it.=20

The first formula simply gives you an inductance equal the reactance = of R or=20 in our case we're using 14.4 ohms at 5 Mhz. This results in an = inductance of=20 0.458 uH. The second formula simply produces half that inductance or, = 0.229 uH.=20

Back to the result of 0.458 uH, that could easily be achieved with 10 = turns=20 on a T-50-2 toroid. Alright we have a T50-2 toroid with 10 turns on it, = this is=20 supposed to represent 14.4 ohms at 5 Mhz. To match to 50 ohms all we = have to do=20 is work out the turns ratio. Impedance transforms as "the square of the = ratio of=20 turns". Then 50 / 14.4 =3D 3.472' and the square root of this is 1.86 so = we need=20 on the secondary 1.86 times more turns or in our case 19 turns.=20

IF our output were terminated in a genuine 50 ohm load then the = square of [19=20 /10] being the turns ratio would be reflected back giving (if you work = it out) a=20 source of 13.85 ohms.=20

The CRITICAL aspects here are: a) turns ratio AND; b) final=20 termination being a genuine 50 ohm load.=20

What is the upper frequency limit of our wide band rf = transformer?

The high frequency limit is influenced by the leakage inductance Lk = and=20 distributed capacitance of the inductor forming a second order low pass = filter=20 and is influenced by a very wide range of factors. The higher the = inductance,=20 then the lower or flatter the low-frequency end but, this comes at a = price of=20 higher Lk and distributed capacitance limiting high frequency response. = Often a=20 compromise is needed for high ratios of frequencies. Although I have = never=20 tested it, I would imagine at least one octave bandwidth could easily be = accomodated e.g. 2.5 Mhz to 5 Mhz or 5 Mhz to 10 Mhz.=20

 

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Got a question on this topic?

If you are involved in electronics then consider joining our "electronics=20 Questions and Answers" news group to ask your question there as well = as=20 sharing your thorny questions and answers. Help out your colleagues!.=20

The absolute fastest way to get your question answered and yes, I = DO=20 read most posts.=20

This is a mutual help group with a very professional air about it. = I've=20 learn't things. It is an excellent learning resource for lurkers as well = as=20 active contributors. =20

RELATED TOPICS ON WIDE BAND RF TRANSFORMERS

broad=20 band amplifiers

tuned=20 circuit amplifiers

impeda= nce=20

induc= tance=20

reacta= nce=20
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__d("createObjectFrom",[],function(a,b,c,d,e,f){b.__markCompiled&&b.__mar= kCompiled();function g(h,i){var = j=3D{},k=3DES('Array','isArray',false,i);if(typeof = i=3D=3D'undefined')i=3Dtrue;for(var = l=3Dh.length;l--;)j[h[l]]=3Dk?i[l]:i;return j;}e.exports=3Dg;},null);=0A= __d("URISchemes",["createObjectFrom"],function(a,b,c,d,e,f,g){b.__markCom= piled&&b.__markCompiled();var = h=3Dg(['fb','fb-ama','fb-messenger','fbcf','fbconnect','fbrpc','file','ft= p','http','https','mailto','ms-app','itms','itms-apps','itms-services','m= arket','svn+ssh','fbstaging','tel','sms','pebblejs','sftp']),i=3D{isAllow= ed:function(j){if(!j)return true;return = h.hasOwnProperty(j.toLowerCase());}};e.exports=3Di;},null);=0A= __d("copyProperties",[],function(a,b,c,d,e,f){b.__markCompiled&&b.__markC= ompiled();function g(h,i,j,k,l,m,n){h=3Dh||{};var = o=3D[i,j,k,l,m],p=3D0,q;while(o[p]){q=3Do[p++];for(var r in = q)h[r]=3Dq[r];if(q.hasOwnProperty&&q.hasOwnProperty('toString')&&(typeof = 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if(ia.ui_created){j.showLoader(function(){ha._triggerDefault(ia.id);},0);= }else ha.iframe(ia);}else = if(s.nativeApp()&&!ia.ui_created){ia.frame=3Dia.id;n.onready(function(){h= a.setLoadedNode(ia,n.open(ia.url+'#cb=3D'+ia.frameName),'native');});ha._= popupMonitor();}else = if(!ia.ui_created)ha.popup(ia);},async:function(ia){ia.params.redirect_ur= i=3Dlocation.protocol+'//'+location.host+location.pathname;delete = ia.params.access_token;p.remote.showDialog(ia.params,function(ja){var = ka=3Dja.result;if(ka&&ka.e2e){var = la=3Dj.get(ia.id);la.trackEvents(ka.e2e);la.trackEvent('close');delete = ka.e2e;}ia.cb(ka);});},getDefaultSize:function(){return = j.getDefaultSize();},_insertIframe:function(ia){ha._loadedNodes[ia.id]=3D= false;var ja=3Dfunction(ka){if(ia.id in = ha._loadedNodes)ha.setLoadedNode(ia,ka,'iframe');};if(ia.post){aa({url:'a= bout:blank',root:ia.root,className:ia.className,width:ia.size.width,heigh= t:ia.size.height,id:ia.id,onInsert:ja,onload:function(ka){h.submitToTarge= t({url:ia.url,target:ka.name,params:ia.params});}});}else = aa({url:ia.url,root:ia.root,className:ia.className,width:ia.size.width,he= ight:ia.size.height,id:ia.id,name:ia.frameName,onInsert:ja});},_handleRes= izeMessage:function(ia,ja){var = ka=3Dha.getLoadedNode(ia);if(!ka)return;if(ja.height)ka.style.height=3Dja= .height+'px';if(ja.width)ka.style.width=3Dja.width+'px';u.inform('resize.= ack',ja||{},'parent.frames['+ka.name+']');if(!j.isActive(ka))j.show(ka);}= ,_triggerDefault:function(ia){ha._xdRecv({frame:ia},ha._defaultCb[ia]||fu= nction(){});},_popupMonitor:function(){var ia;for(var ja in = ha._loadedNodes)if(ha._loadedNodes.hasOwnProperty(ja)&&ja in = ha._defaultCb){var = ka=3Dha._loadedNodes[ja];if(ka.type!=3D'popup'&&ka.type!=3D'native')conti= nue;var la=3Dka.node;try{if(la.closed){ha._triggerDefault(ja);}else = ia=3Dtrue;}catch(ma){}}if(ia&&!ha._popupInterval){ha._popupInterval=3Dset= Interval(ha._popupMonitor,100);}else = 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__d("legacy:fb.auth",["sdk.Auth","sdk.Cookie","copyProperties","sdk.Event= ","FB","Log","sdk.Runtime","sdk.SignedRequest","sdk.ui"],function(a,b,c,d= ,e,f,g,h,i,j,k,l,m,n,o){b.__markCompiled&&b.__markCompiled();k.provide(''= ,{getLoginStatus:function(){return = g.getLoginStatus.apply(g,arguments);},getAuthResponse:function(){return = g.getAuthResponse();},getAccessToken:function(){return = m.getAccessToken()||null;},getUserID:function(){return = m.getUserID()||m.getCookieUserID();},login:function(p,q){if(q&&q.perms&&!= q.scope){q.scope=3Dq.perms;delete q.perms;l.warn('OAuth2 specification = states that \'perms\' '+'should now be called \'scope\'. 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Applications for wide band rf transformers include = impedance=20 matching, voltage or current transformation, DC isolation, balanced / = unbalanced=20 mixing, matching, power splitting, coupling, and signal inversion. = Custom wide=20 band transformers with special combinations of impedance ratio, = insertion loss,=20 frequency response, and current handling are also = available."
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WIDE BAND RF TRANSFORMERS



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What are wide band rf transformers?

Wideband rf transformers are simply transfomers designed to provide = an=20 impedance transformation over a broad frequency range. In amateur radio=20 applications we wind these transformers on ferrite = toroids. A common impedance transformation is 200 ohms to 50 ohms = using a=20 bi-filar winding. Here is an example from our broad=20 band amplifiers tutorial.

3D"This=20

Figure 1. - wideband rf amplifier with shunt feedback and = emitter=20 degeneration

Transformer T1 is a broadband rf transformer.=20

Designing wide band rf transformers

In the design of these kinds of wide band rf transformers the primary = reactance is usually around 5 times the primary impeda= nce.=20 With a 200 ohms to 50 ohm transformer, we would allow a reactance of = 1,000 ohms=20 at the lowest frequency of interest. Just as an example consider = we were=20 building a broad band amplifier for the amateur bands and going down as = low as=20 1.8 Mhz.=20

For this example we would need bi-filar windings which have a reacta= nce=20 of 1,000 ohms at 1.8 Mhz, this means a required induc= tance=20 of around 88 uH. A look through the Amidon data book tells me that = ferrite=20 toroid FT-50-61 as one example can provide me with an AL factor of 68mH = / 1000=20 turns.=20

This means if 1,000 turns were wound on the toroid it would give us = 68 mH.=20 Yes that IS milli-henries, these are ferrite toroids.=20

Calculating turns for wide band rf transformers

To wind a wide band rf transformer with an inductance of 88 uH (yes = that's=20 micro-henries) which is in fact 0.088 mh we use the following formula:=20

Turns =3D 1,000 X SQRT (L in mH / AL factor) =   =3D   1,000 X=20 SQRT (0.088 / 68)   =3D   36 turns.=20

Our wide band rf transformer needs 36 turns to achieve an inductance = of 88=20 uH.=20

Winding the wide band rf transformer

Because this is a bi-filar winding for our wide band rf transformer, = we need=20 two lengths of wire which we will "twist" together at a "pitch" of 2.5 = turns per=20 inch or 1 turn per 10 mm. If you anchor one end of the two wires = together in a=20 bench vise and fix the other ends securely in a hand drill (a bent nail = or fish=20 hook helps here) you then gently "stretch" the wires first. Then you = slowly turn=20 the hand drill and notice the two wires "twisting" together, as you = proceed you=20 will notice more and more twists appearing. Stop when you have about 2.5 = twists=20 to the inch. Stretch the wires once more.=20

Wind 36 turns through the toroid and that is it! To use in an = application=20 such as figure 1 above you need to pay attention to the "phasing". = Notice the=20 two dots on T1 above? They indicate the start of each wire. Use = an=20 ohmmeter to find the start and finish of one winding, mark it in some = convenient=20 manner e.g. coloured pen. The other winding should then be obvious.=20

Commercially manufactured wide band rf transformers

Coilcraft is one manufacturer of wide band transformers which provide = reliable performance.=20

The transformers are offered in tapped or untapped configurations and = are=20 packaged in a low-profile DIP-style plastic case. All parts are = available in=20 either a surface mount version or a through-hole version that=92s = compatible with=20 standard DIP sockets.=20

Applications include impedance matching, voltage or current = transformation,=20 DC isolation, balanced / unbalanced mixing, matching, power splitting, = coupling,=20 and signal inversion. Custom wide band transformers with special = combinations of=20 impedance ratio, insertion loss, frequency response, and current = handling are=20 also available.=20

Designing wide band rf transformers for different impedances

Alright what if you need something other than a 200 ohm to 50 ohms=20 transformer, how would you go about it?=20

What I tell you here now is applicable from DC to daylight. What that = means=20 is, it is equally applicable to an audio transformer with a bandwidth of = 100 Hz=20 to 3,000 Hz (for an audio=20 transformer) as it is to a broadband transformer designed to operate = at say=20 7.00 to 7.50 Mhz. Read on.=20

Firstly you need to pick either a lower 1 dB or 3 dB bandwidth. = Wozzat???=20 Look at figure 2 below where I present my usual scungy drawing - I'm no = good at=20 this graphic arts caper, not the program, just my lack of artistic = talent.=20

3D"This=20

Figure 2. - band pass filter characteristics

Here I've crudely depicted a range of frequencies being passed by a = filter=20 and indicated the 1 dB and 3 db points. A 1 db point is where the power = output=20 is about 80% of the band pass power or 90% of the voltage level. A 3 db = point is=20 where the power output is about 50% of the band pass power or 70.7% of = the=20 voltage level. If you can't understand decibels then you need to look at = the decibel = page=20

In your broad band transformer you need to determine the lowest point = you can=20 tolerate in frequency. Entirely for discussion purposes I've selected 5 = Mhz for=20 both 1 dB and 3 dB to demonstrate the formulas. Also I'm going to = construct a =20 broad band tranformer to operate between 14.4 ohms and 50 ohms.=20

For the 1 db point to be 5 Mhz, I use the formula Lp =3D R / ( 2 X Pi = X Fo) and=20 for the 3 dB point, I use the formula Lp =3D R / ( 4 X Pi X Fo). The = general=20 formula for any other dB level is a bit difficult to reproduce here but = contact = me and I'll give it to anyone who wants it.=20

The first formula simply gives you an inductance equal the reactance = of R or=20 in our case we're using 14.4 ohms at 5 Mhz. This results in an = inductance of=20 0.458 uH. The second formula simply produces half that inductance or, = 0.229 uH.=20

Back to the result of 0.458 uH, that could easily be achieved with 10 = turns=20 on a T-50-2 toroid. Alright we have a T50-2 toroid with 10 turns on it, = this is=20 supposed to represent 14.4 ohms at 5 Mhz. To match to 50 ohms all we = have to do=20 is work out the turns ratio. Impedance transforms as "the square of the = ratio of=20 turns". Then 50 / 14.4 =3D 3.472' and the square root of this is 1.86 so = we need=20 on the secondary 1.86 times more turns or in our case 19 turns.=20

IF our output were terminated in a genuine 50 ohm load then the = square of [19=20 /10] being the turns ratio would be reflected back giving (if you work = it out) a=20 source of 13.85 ohms.=20

The CRITICAL aspects here are: a) turns ratio AND; b) final=20 termination being a genuine 50 ohm load.=20

What is the upper frequency limit of our wide band rf = transformer?

The high frequency limit is influenced by the leakage inductance Lk = and=20 distributed capacitance of the inductor forming a second order low pass = filter=20 and is influenced by a very wide range of factors. The higher the = inductance,=20 then the lower or flatter the low-frequency end but, this comes at a = price of=20 higher Lk and distributed capacitance limiting high frequency response. = Often a=20 compromise is needed for high ratios of frequencies. Although I have = never=20 tested it, I would imagine at least one octave bandwidth could easily be = accomodated e.g. 2.5 Mhz to 5 Mhz or 5 Mhz to 10 Mhz.=20

 

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Got a question on this topic?

If you are involved in electronics then consider joining our "electronics=20 Questions and Answers" news group to ask your question there as well = as=20 sharing your thorny questions and answers. Help out your colleagues!.=20

The absolute fastest way to get your question answered and yes, I = DO=20 read most posts.=20

This is a mutual help group with a very professional air about it. = I've=20 learn't things. It is an excellent learning resource for lurkers as well = as=20 active contributors. =20

RELATED TOPICS ON WIDE BAND RF TRANSFORMERS

broad=20 band amplifiers

tuned=20 circuit amplifiers

impeda= nce=20

induc= tance=20

reacta= nce=20
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