Bidirectional power transfer system, method of operating the same, and wireless power system
US-12021391-B2 · Jun 25, 2024 · US
US9450543B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9450543-B2 |
| Application number | US-201214367098-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 12, 2012 |
| Priority date | Dec 29, 2011 |
| Publication date | Sep 20, 2016 |
| Grant date | Sep 20, 2016 |
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The present invention provides a new structure of Doherty power amplifier. The present invention reduces use of ¼ wavelength lines and lowers the Q point of the Doherty power amplifier. The present method extends the DPA bandwidth with a simpler and more convenient design and facilitates the design of a narrowed size.
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What is claimed is: 1. A Doherty power amplifier, comprising an input power divider into which an input signal of the Doherty power amplifier is inputted, one output of the input power divider being connected to a carrier amplifier, the other output of the divider being connected to a first ¼ wavelength line, the other end of the first ¼ wavelength line being connected to a peaking amplifier, one end of the carrier amplifier being connected to a second ¼ wavelength line, the other end of the second ¼ wavelength line being connected to the peaking amplifier; a junction point between the second ¼ wavelength line and the peaking amplifier being a signal output point of the Doherty power amplifier, wherein a characteristic impedance Z 01 of the second ¼ wavelength line is determined by the following equation: Z 01 =50*√{square root over ((1+γ))}, where, γ is a power ratio. 2. A Doherty power amplifier, comprising an input power divider into which an input signal of the Doherty power amplifier is inputted, one output of the input power divider being connected to a carrier amplifier, the other output of the divider being connected to a first ¼ wavelength line, the other end of the first ¼ wavelength line being connected to a peaking amplifier, one end of the carrier amplifier being connected to a second ¼ wavelength line, the other end of the second ¼ wavelength line being connected to the peaking amplifier; a junction point between the second ¼ wavelength line and the peaking amplifier being a signal output point of the Doherty power amplifier, wherein a load impedance Z 02 of the peaking amplifier is determined by the following equation: Z 02 = 50 * ( 1 + γ ) γ , where, γ is a power ratio. 3. A Doherty power amplifier, comprising an input power divider into which an input signal of the Doherty power amplifier is inputted, one output of the input power divider being connected to a carrier amplifier, the other output of the divider being connected to a first ¼ wavelength line, the other end of the first ¼ wavelength line being connected to a peaking amplifier, one end of the carrier amplifier being connected to a second ¼ wavelength line, the other end of the second ¼ wavelength line being connected to the peaking amplifier; a junction point between the second ¼ wavelength line and the peaking amplifier being a signal output point of the Doherty power amplifier, wherein when the input signal is small, the peaking amplifier is closed, and the carrier amplifier works in a high-impedance state, the impedance of the carrier amplifier being determined by the following equation: Z high _ impedance =50* (1+γ), where, γ is a power ratio.
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