CSTCR6M00G53-R0 Murata, CSTCR6M00G53-R0 Datasheet - Page 13

Resonators 6.00MHz 0.5%

CSTCR6M00G53-R0

Manufacturer Part Number
CSTCR6M00G53-R0
Description
Resonators 6.00MHz 0.5%
Manufacturer
Murata
Series
CSTCR-Gr

Specifications of CSTCR6M00G53-R0

Tolerance
0.5 %
Termination Style
SMD/SMT
Operating Temperature Range
- 20 C to + 80 C
Dimensions
2 mm W x 4.5 mm L x 1.5 mm H
Frequency Stability
0.2 %
Frequency
6 MHz
Lead Free Status / RoHS Status
Lead free / RoHS Compliant

Available stocks

Company
Part Number
Manufacturer
Quantity
Price
Part Number:
CSTCR6M00G53-R0
Manufacturer:
MURATA
Quantity:
9 000
Part Number:
CSTCR6M00G53-R0
Manufacturer:
MURATA
Quantity:
8 000
Note
(Note 3)
Fig.Ⅲ shows the equivalent circuit of an emitter
grounding type transistor circuit. In the figure, Ri
stands for input impedance, R
impedance and ß stands for current amplification
rate.
When the oscillation circuit in Fig.2-6 is expressed
by using the equivalent circuit in Fig.Ⅲ, it becomes
like Fig. Ⅳ. Z
for each Hartley type and Colpitts type circuit.
The following 3 formulas are obtained based on
Fig.Ⅳ.
• Please read rating and
• This catalog has only typical specifications because there is no space for detailed specifications. Therefore, please review our product specifications or consult the approval sheet for product specifications before ordering.
Notes
Fig.
Z
Z
β R
Z
Z
(Z
1
2
1
1
1
i
1
+Ri) i
0
+Z
Hartley/Colpitts Type LC Oscillation Circuits
i
1
+(R
2
i
2
1
1
–(Z
R
–Z
0
CAUTION (for storage, operating, rating, soldering, mounting and handling) in this catalog to prevent smoking and/or burning, etc.
, Z
+Z
Hartley Type
1
1
2
2
+Z+Z
i
2
1 / jωC
3
and Z are as shown in the table
) i
jωL
jωL
=0
-
+
2
1
2
R
–Z
R
R
0 1
1
0
Fig.
) i
2
…………………………… (3)
i
3
3
=0 …………………… (1)
=0 …………………… (2)
+
-
2
0
R
0 1
R
stands for output
0
Z
2
Z
Colpitts Type
3
1 / jωC
1 / jωC
jωL
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
(Hartley Type)
(Colpitts Type)
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)
1
,Z
1
βR
2
(Imaginary number part)
(Real number part)
                  …… (9)
                  … (10)
                ………… (7)
                ………… (8)
≠ 0, i
R
and Z solving it for angular frequency ω .
0
0
Z
βR
Z
Z
Z
1
1
1
2
Z
2
Z
1
Z
(Z+Z
, Z
2
0
≠ 0, i
2
2
=(Z
Principles of CERALOCK
Z
=(Z
Z+(Z
1
2
Z
and Z are all imaginary numbers,
1
2
1
2
fosc. =
)Ri=0     ………………… (6)
+Z+Z
0
fosc. =
3
+Ri)Z
+Z
1
is large enough. Therefore
≠ 0 are required for continuous
+Z
1
(Z+Z
(L
L C
2
1
+Z)RiR
2
1
2
)Ri}(Z
C
L
–{Z
L1
L1
2
2
) C{1+
)R
1
+C
·C
1
(Z
0
2
L2
L2
+
0
+R
2
1
=0    ………… (5)
+Z)+
C
C
(L
· {1+
0
1
)    ………… (4)
L1
1
L1
1
· C
+C
+ L
L
(C
L2
1
L2
2
· L
L1
) CR R
+C
2
L
L2
) R R
0
}
®
0
}
2
11
P17E.pdf
SEP.16,
2011
2

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