CSBFB900KJ58-R1 Murata, CSBFB900KJ58-R1 Datasheet - Page 17

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CSBFB900KJ58-R1

Manufacturer Part Number
CSBFB900KJ58-R1
Description
Manufacturer
Murata
Datasheet

Specifications of CSBFB900KJ58-R1

Lead Free Status / RoHS Status
Compliant
Note
• This PDF catalog is downloaded from the website of Murata Manufacturing co., ltd. Therefore, it’s specifications are subject to change or our products in it may be discontinued without advance notice. Please check with our
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sales representatives or product engineers before ordering.
(Note 3)
Fig. 3 shows the equivalent circuit of an emitter
grounding type transistor circuit. In the figure, Ri
stands for input impedance, R
impedance and
rate.
When the oscillation circuit in Fig. 2-6 is expressed
by using the equivalent circuit in Fig. 3, it
becomes like Fig. 4. Z
the table for each Hartley type and Colpitts type
circuit.
The following 3 formulas are obtained based on
Fig. 4.
Fig. 4 4 Hartley/Colpitts Type LC Oscillation Circuits
Notes
Z
Z
Z
Z
(Z
1
2
1
1
R
1
i
1
+Ri) i
0
+Z
i
1
+(R
2
i
2
1
–(Z
R
0
–Z
+Z
Hartley Type
1
2
1
i
2
+Z+Z
stands for current amplification
1 / j C
3
) i
j L
j L
=0
-
+
2
1
2
–Z
R
R
0 1
R
1
1
0
Fig. 3 3
) i
, Z
2
i
3
3
=0
2
=0
and Z are as shown in
-
+
2
0
R
0 1
stands for output
R
0
Z
2
Z
Colpitts Type
3
···················(1)
···················(2)
···················(3)
1 / j C
1 / j C
j L
Z
1
L1
L2
1
As i
oscillation, the following conditional formula can be
performed by solving the formulas of (1), (2) and (3)
on the current.
Then, as Z
the following conditional formula is obtained by
dividing the formula (4) into the real number part
and the imaginary number part.
Formula (5) represents the phase condition and
formula (6) represents the power condition.
Oscillation frequency can be obtained by applying
the elements shown in the aforementioned table to
Z
In either circuit, the term in brackets will be 1 as
long as Ri and R
oscillation frequency can be obtained by the
following formula.
(Hartley Type)
(Colpitts Type)
(Hartley Type)
(Colpitts Type)
1
2
2
osc = (2 fosc.)
osc = (2 fosc.)
Z
1
2
(Imaginary number part)
(Real number part)
R
R
and Z solving it for angular frequency .
0, i
0
0
Z
Z
Z
Z
1
1
R
1
2
Z
Z
2
1
Z
(Z+Z
2
2
, Z
0
2
Z
=(Z
=(Z
Principles of CERALOCK
Z+(Z
0, i
1
2
Z
and Z are all imaginary numbers,
1
1
2
2
fosc. =
)Ri=0
+Ri)Z
+Z+Z
+Z
fosc. =
0
3
2
2
1
is large enough. Therefore
=
=
+Z
1
0 are required for continuous
(Z+Z
L C
(L
2
1
+Z)RiR
2
2
)Ri}(Z
1
C
–{Z
L
2
2
L1
L1
2
2
)R
) C{1+
1
+C
1
·C
(Z
0
(L
2
L2
+
L2
L · C
2
0
+R
1
+Z)+
=0
1
+L
C
0
· {1+
(L
1
)
L1
1
2
L1
1
) C
+C
·C
+ L
L
(C
L2
L2
···················(4)
···················(6)
1
···················(7)
···················(8)
2
· L
L1
) CR R
+C
·············(5)
2
L
L2
·······(9)
·····(10)
) R R
0
}
®
0
}
2
15
P17E.pdf
08.3.28
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