Tuesday, June 17, 2014
BUJJI YAMP
Good Morning,
Here we comes with BUJJI YAMP. It is assembled with only six components for each amplifier. 1 LM386, 2 Resistors and 4 Capacitors.
The amplifier circuit is taken from the data sheet of LM386 with a gain of 20. The normal mobile charger or PC/LAPTOP USB can be used to power up the device. The audio is feed through stereo cable into the pin no 3 of LM386. It is meant to listen the music through your phone hands free.
Here we comes with BUJJI YAMP. It is assembled with only six components for each amplifier. 1 LM386, 2 Resistors and 4 Capacitors.
The amplifier circuit is taken from the data sheet of LM386 with a gain of 20. The normal mobile charger or PC/LAPTOP USB can be used to power up the device. The audio is feed through stereo cable into the pin no 3 of LM386. It is meant to listen the music through your phone hands free.
Saturday, June 7, 2014
Designing of Single section Band Pass Filter
Dear all,
Today we present a simple method for designing a single section band pass filter.
Today we present a simple method for designing a single section band pass filter.
The Impedance of the coil is 75 Ohms = 2πFL.
Impedance of capacitance = 1/2πFC
Let us calculate value of L & C for F of 17.820 MHz and R = 75 Ohms.
Capacitance value calculation:
R
= 1/2πFC
Where F = 17.820 MHz
R
= 75 Ω
C
= 1/2πRF
C
= 120 pF
Inductor Value calculation :
R
= 2πFL
Where F
= 17.820 MHz
R
= 75 Ω
L
= R/2πF
L
= (75)/(2*π*17.82*10^6)
L
= 0.7µH
Approx Expected Q of the copper coil is between 200 and 300.
Bandwidth of the circuit is =
F/Q
Loaded Q is decided as 20 to take care of low insertion loss.
The loaded Q is around 20 => Bandwidth
is 891 KHz
Impedance of the coil is 75 Ω
For Q = 20 the impedance of the tank circuit is 75 * 20 =
1500 Ω
![]() |
| Loaded Q is 20 |
Rin = Rout = 50Ω ( input impedance is 50 Ohms )
Equivalent circuit with double loading.
![]() |
| Equivalent circuit with double loaded |
Impedance of the coil is 75 Ω
For Q = 20 the impedance of the tank circuit is 75 * 20 =
1500 Ω
(Here we are neglecting the coil's finite Q)
(Here we are neglecting the coil's finite Q)
Series and parallel equivalent of loading circuit
![]() |
| Series and parallel equivalent of loading circuit |
![]() |
| parallel to series and series to parallel conversion |
Parallel to series and series to parallel impedance conversion equations.
Rp = Rs{1+ (Xs/Rs)^2}
Xp = (Rp*Rs)/Xs
Rs = Rp/{1+(Rp/Xp)}
Xs = (Rs*Rp)/Xp
These equation are from MOTOROLA application note
Now let us calculate Xp and Xs, we know Rp = 1500 and Rs = 25 Ohms
Rp = Rs{1+K^2}
Where K = Xs/Rs
1 + K^2 = Rp/Rs
1 + K^2 = 1500/25
1 + k^2 = 60
K = 7.6
Xs/Rs = 7.5
Xs = 7/5 * Rs
Xs = 190
Xs = 1/2πFC
C = 1/2πXsF
Where F = 17.820 MHz
Xs = 190
C = 47pF
Series equivalent circuit:
![]() |
| Series equivalent circuit |
Input/output circuit:
![]() |
| Input/Output circuit |
Xs = Rs*Rp/Xp
Xp = Rs*Rp/Xs
Where Rs = 25
Rp = 1500
Xp = 197
This means for loaded Q of 20 and above Xs and Xp are almost
same
Now tuning capacitance Ct = Total capacitance required –
coupling capacitor (Xp)
= 120 – 47 pF
= 73 pF
Final circuit is
![]() |
| Final Circuit |
The insertion loss of the circuit is 20Log(D/D-1)
Where D = Unloaded Q/desired Q
In our case unloaded Q in between 200 - 300 and the loaded Q is 20.
In our case insertion loss is 1db
There is no circuit which will give zero loss due to finite unloaded Q
If somebody claims he has designed a zero loss band pass filter then Prof A.ZVEREV Russian scientist would be unhappy man. As he is the designer of insertion loss equation.
Thursday, June 5, 2014
IF SDR
Dear all,
Here we comes with shortwave radio with IF 1.8432 MHz with a few modifications in the SDR circuit.
Crystal Frequency, which we changed from 28.224 MHz to 7.3728 MHz.
Band pass Filter, where the capacitor and inductor values are changed. The modified and original circuit is shown below.
Here we comes with shortwave radio with IF 1.8432 MHz with a few modifications in the SDR circuit.
![]() |
| IF SDR |
Crystal Frequency, which we changed from 28.224 MHz to 7.3728 MHz.
Band pass Filter, where the capacitor and inductor values are changed. The modified and original circuit is shown below.
![]() |
| Modified Band pass Filter |
![]() |
| Original Band pass filter |
Monday, June 2, 2014
Friday, May 30, 2014
Thursday, May 29, 2014
Tuesday, May 27, 2014
Wednesday, May 21, 2014
Tuesday, May 20, 2014
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