Murata Manufacturing RF Transformers 12

Reset All
Part RoHS Manufacturer Transformer Type Mounting Feature Manufacturer Series Approvals (V) Terminal Finish Impedance (Primary) Power Rating Impedance (Secondary) No. of Winding (Primary) Isolation Voltage Insertion Loss Inductance (Primary) Packing Method Output Current-1 Maximum DC Unbalance Current No. of Winding (Secondary) Sub-Category Dimensions Maximum Operating Temperature Application Minimum Cutoff Frequency Minimum Operating Temperature Height Width Diameter Nominal Input Voltage (V) Load Resistance Additional Features JESD-609 Code Maximum Cutoff Frequency Minimum Operating Frequency Length Turns Ratio (Np:Ns) Maximum Operating Frequency

LDB212G4010C-001

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

Tin (Sn)

1 dB

L2.0XB1.25XH0.95 (mm)

85 Cel

2300 GHz

-40 Cel

.95 mm

1.25 mm

e3

2500 MHz

2 mm

DXW21BN7511TL

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

1 dB

TR, 7 INCH

L2.0XB1.2XH1.2 (mm)

85 Cel

50 GHz

-40 Cel

1.2 mm

1.2 mm

20

1200 MHz

2 mm

DXW21BN7511SL

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

1.4 dB

TR, EMBOSSED, 7 INCH

L2.0XB1.2XH1.2 (mm)

85 Cel

1000 GHz

-40 Cel

1.2 mm

1.2 mm

20

1500 MHz

2 mm

#458PT-1720=P3

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

B5F

L6.9XB3.8XH4.4 (mm)

4.4 mm

3.8 mm

6.9 mm

#617PT-2038=P3

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

4.5 dB

TR, PLASTIC, 13 INCH

85 Cel

5 GHz

-40 Cel

3.2 mm

2.7 mm

200 MHz

4.4 mm

1:1:2

LDB212G4020C-001

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

Tin (Sn)

50 OHMS

100 OHMS

1.05 dB

TAPE & REEL

Other Transformers

L2.0XB1.25XH0.95 (mm)

85 Cel

SIGNAL

2300 GHz

-40 Cel

.95 mm

1.25 mm

e3

2500 MHz

2300000 KHz

2 mm

2500000 KHz

LDB21924M05C-001

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

Tin (Sn)

1.4 dB

L2.0XB1.25XH0.95 (mm)

85 Cel

889 GHz

-40 Cel

.95 mm

1.25 mm

e3

960 MHz

2 mm

#458PT-2002=P3

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

B5F

L6.9XB3.8XH4.4 (mm)

4.4 mm

3.8 mm

6.9 mm

LDB182G5010G-120

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

Tin (Sn)

50 OHMS

100 OHMS

1.2 dB

TAPE & REEL

Other Transformers

L1.6XB0.8XH0.6 (mm)

85 Cel

SIGNAL

2300 GHz

-40 Cel

.6 mm

.8 mm

e3

2700 MHz

2300000 KHz

1.6 mm

2700000 KHz

LDB212G4005C-001

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

Tin (Sn)

.9 dB

L2.0XB1.25XH0.95 (mm)

85 Cel

2300 GHz

-40 Cel

.95 mm

1.25 mm

e3

2500 MHz

2 mm

LDB31900M20C-416

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

TIN

50 OHMS

200 OHMS

.9 dB

TAPE & REEL

L1.6XB0.8XH0.6 (mm)

85 Cel

SIGNAL

800 GHz

-40 Cel

.6 mm

.8 mm

e3

1000 MHz

800000 KHz

1.6 mm

1000000 KHz

DXW21BN2511NL

Murata Manufacturing

RF TRANSFORMER

SURFACE MOUNT

1 dB

TR, EMBOSSED, 7 INCH

85 Cel

13.56 GHz

-40 Cel

1.2 mm

1.2 mm

20

2 mm

RF Transformers

RF transformers are a type of transformer used in radio frequency (RF) applications to match impedances and transform signal levels between different stages of a circuit. They are commonly used in RF amplifiers, filters, and mixers.

The primary function of an RF transformer is to match the impedance of the input and output stages of an RF circuit. Impedance matching is critical in RF applications to ensure maximum power transfer and signal integrity. RF transformers also help to transform the signal levels between stages of an RF circuit, such as between a high-impedance antenna and a low-impedance amplifier.

RF transformers are typically designed to operate at high frequencies, ranging from a few kHz to several GHz, depending on the specific application. They are also designed to handle high power levels and have low losses. The design of an RF transformer is usually optimized for a specific frequency range and bandwidth.

RF transformers are typically constructed with a magnetic core made of ferrite, powdered iron, or other high-permeability materials, and one or more coils wound around the core. The coils are usually made of copper wire with a thin insulating layer. The number of turns and the size of the wire are determined by the required impedance transformation and the frequency range of the circuit.