JP2016129141A - モーダル解析 - Google Patents
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Abstract
Description
によって与えられる。別の例として、エネルギ印加区域がa×a×aの寸法を有する立方体の場合、最大共振波長は、
によって与えられる。さらに別の例では、図2Bに示すように、エネルギ印加区域が半径a、長さdの円筒であり得る。この場合、最大共振波長は、2a>dが成立する場合
によって与えられ、2a<dが成立する場合は
によって与えられる。別の例では、エネルギ印加区域が半径aの球体の場合、最大共振波長は、
によって与えられる。
として表すことができる。別の例として、a×a×aの寸法を有する立方体空洞では、モーダル条件は、
として表すことができる。別の例として、半径aの球体空洞では、モーダル条件は、
として表すことができる。空洞の寸法とともに「モーダル条件」を満たす波長で動作する装置を本明細書では「モーダル装置」と呼び、その空洞を本明細書では「モーダル空洞」と呼ぶ。一部の実施形態では、モーダル装置は、その空洞のモーダル条件を満たす波長の範囲内でしか動作しないように構成される。一部の実施形態では、この装置は、モーダル条件を満たす波長およびその条件を満たさない波長の両方で動作するように構成することができる。そのような装置をモーダル装置と呼ぶか非モーダル装置と呼ぶかは、その装置が運転される波長によって決まる。
ε”=εd”+εσ”=εd”+σ’/(ωε0) (1)
によって示すことができ、下付き文字dおよびσは、双極子回転およびイオン伝導それぞれの寄与率を表し、σ’は導電率であり、ωは角周波数であり、ε0は自由空間または真空の誘電率である。以下、略記として総損失を「σ」によって示す場合がある。ただし本明細書で使用するとき、用語「損失」は、あらゆる種類の吸収率の寄与を包含するよう広く使用する。
[(f1,A1),(f1,A2)
(f2,A1),(f2,A2)]
[I11,I21,I31,...,INd1;
I12,I22,I32,...,INd2;
...
I1Nm,I2Nm,I3Nm,...,INdNm]
I行列と呼ぶこの行列は、MSEおよび離散化を決定した後で求めてもよい。
1/2(σ1I1j+σ2I2j+...+σNdINdj)=Pj (2)
1/2σI=P (3)
σ=2PI−1 (4)
Ej=a1Ij1+a2Ij2+...aKIjK (5)
によって与えることができ、Kは使用可能なMSEの数である。
によって与えられる。最大共振波長ならびに対応する最低共振波長は、様々な周波数の波で空洞を掃引し、空洞内の吸収を検出することにより実験的に見出すこともできる。第1の吸収ピーク(または反射ディープ(reflection deep))は、最低共振周波数および空洞によってサポートされる最も長い共振波長に対応することができる。
を超える波長でのみエネルギを加えるように供給源を構成することができる。そのような波長は、約4.3GHzより小さい周波数に対応する。実施形態にもよるが、先に説明したように、1つまたは複数の所定の周波数で交流波形を発生させるために、特定の磁電管または半導体発振器を使用することができる。一部の実施形態では、ステップ904Xは省略してもよい。例えば一部の実施形態では、モーダル条件を満たしても満たさなくてもよい既知の周波数でエネルギを加えるように電磁エネルギ源を構成することができ、ステップ904Xは省略することができる。一部の実施形態では、エネルギ印加区域の寸法を、例えば空洞の壁を移動することによって制御するようにプロセッサを構成することができ、これらの寸法が変わるたびにステップ904Xを実行することができる。
Claims (13)
- 複数の放射素子を介して空洞内の対象物に1MHzから100GHzの周波数範囲内の複数の周波数で電磁エネルギを加えるための装置であって、
エネルギ印加区域内の第1の領域および第2の領域に、第1および第2の量のRFエネルギがそれぞれ第1および第2の領域に加えられるよう関連付け、ここで前記第1の量のエネルギは前記第2の量のエネルギと異なっており、
複数の組の値を選択することであって、各組が前記エネルギ印加領域内に1のフィールドパターンを及ぼす少なくとも1のパラメータの値を含み、前記組のうちの2つは周波数の値および位相の値のうちの1以上において互いに異なっており、前記複数の組は前記第1および第2の領域にエネルギを印加する目的をもって選択され、
前記選択された複数の組の値で前記エネルギ印加領域に電磁エネルギをかけることにより、前記第1の量のRFエネルギを前記エネルギ印加領域の第1の領域に印加し、前記第2の量のRFエネルギを前記エネルギ印加領域の第2の領域に印加するために、供給源を調整する、
ように構成される少なくとも1個のプロセッサ
を含むことを特徴とする装置。 - 請求項1に記載の装置において、前記少なくとも1個のプロセッサは、前記第1の領域と第2の領域の位置を区別するように構成されることを特徴とする装置。
- 請求項1または請求項2に記載の装置において、前記少なくとも1個のプロセッサが、前記複数の組の値を逐次的に選択するように構成されることを特徴とする装置。
- 請求項1乃至3の何れか1項に記載の装置において、前記少なくとも1個のプロセッサが、各領域内で散逸される前記エネルギについての指示に基づいて、前記第1の領域および前記第2の領域にエネルギを加えるように構成されることを特徴とする装置。
- 請求項1乃至4の何れか1項に記載の装置において、前記供給源が、複数の放射素子により電磁エネルギを供給するように構成され、前記少なくとも1個のプロセッサが、異なる振幅のエネルギを少なくとも2つの放射素子に同時に供給するために、前記供給源を調整するように構成されることを特徴とする装置。
- 請求項1乃至5の何れか1項に記載の装置において、前記少なくとも1個のプロセッサが、前記第1の領域に加えられるエネルギ量が前記第2の領域に加えられるエネルギ量と異なり、前記第1の領域内で吸収されるエネルギが、前記第2の領域内で吸収される前記エネルギと実質的に同じとなるよう、前記供給源を制御するように構成されることを特徴とする装置。
- 請求項1乃至6の何れか1項に記載の装置において、前記少なくとも1個のプロセッサが、
前記エネルギ印加区域内の前記対象物の空間的位置を示す情報を特定し、
第1の選択された組の値でのRFエネルギの印加が、前記対象物の前記空間的位置の第1のエリアに対応する第1の高強度領域を有するフィールドパターンの励起を生じさせ、第2の選択された組の値でのRFエネルギの印加が、前記対象物の前記空間的位置の第2のエリアに対応する第2の高強度領域を有するフィールドパターンの励起を生じさせるように、前記複数の組の値を選択する
ように構成されることを特徴とする装置。 - プロセッサにより調整される電磁エネルギの供給源を用いて空洞内の対象物に1MHzから100GHzの周波数範囲の複数の周波数で電磁エネルギを供給する方法であって、
前記プロセッサにより、第1の領域にかけられる第1の量のエネルギと、第2の領域にかけられる第2の量のエネルギとを割り当てるステップと、
前記プロセッサによって、各組がエネルギ印加領域内で1のフィールドパターンを及ぼす少なくとも1のパラメータの値を含む複数の組の値を選択するステップであって、これらの組は前記d会い1および第2の領域にエネルギを印加する目的をもって選択されるステップと、
前記選択された複数の組の値で前記エネルギ印加領域に電磁エネルギをかけることにより、前記第1の量のRFエネルギを前記第1の領域に印加し、前記第2の量のRFエネルギを前記第2の領域に印加するために、供給源を調整するステップであって、前記第1の量のエネルギは前記第2の量のエネルギと異なっているステップと、
を含むことを特徴とする方法。 - 請求項8に記載の方法において、前記第1および第2の量のエネルギが前記プロセッサにより決定されることを特徴とする方法。
- 請求項8または9に記載の方法において、当該方法が、
前記エネルギ印加領域内の前記対象物の空間的位置を示す情報を特定するステップと、
第1の選択された組の値でのRFエネルギの印加が、前記対象物の前記空間的位置の第1のエリアに対応する第1の高強度領域を有するフィールドパターンの励起を生じさせ、第2の選択された組の値でのRFエネルギの印加が、前記対象物の前記空間的位置の第2のエリアに対応する第2の高強度領域を有するフィールドパターンの励起を生じさせるように、前記複数の組の値を選択するステップと、を含むことを特徴とする方法。 - 請求項10に記載の方法において、さらに、前記エネルギ印加区域内の前記第1の領域および前記第2の領域の位置を、前記第1のエリアおよび前記第2のエリアに従って決定するステップを含むことを特徴とする方法。
- 請求項10に記載の方法において、さらに、前記第1のエリアに吸収されるエネルギが、前記第2のエリアに吸収されるエネルギとほぼ等しくなるように前記供給源を制御するステップを含むことを特徴とする方法。
- 請求項8乃至10のいずれか1項に記載の方法において、さらに、前記第1の領域に吸収されるエネルギが、前記第2の領域に吸収されるエネルギとほぼ等しくなるように前記供給源を制御するステップを含むことを特徴とする方法。
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