JPS60199246A - Reception power measurement device - Google Patents

Reception power measurement device

Info

Publication number
JPS60199246A
JPS60199246A JP59055790A JP5579084A JPS60199246A JP S60199246 A JPS60199246 A JP S60199246A JP 59055790 A JP59055790 A JP 59055790A JP 5579084 A JP5579084 A JP 5579084A JP S60199246 A JPS60199246 A JP S60199246A
Authority
JP
Japan
Prior art keywords
wave
received
output
level
channel
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP59055790A
Other languages
Japanese (ja)
Inventor
Isao Shimizu
功 清水
Takeshi Hattori
武 服部
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP59055790A priority Critical patent/JPS60199246A/en
Publication of JPS60199246A publication Critical patent/JPS60199246A/en
Pending legal-status Critical Current

Links

Landscapes

  • Monitoring And Testing Of Transmission In General (AREA)

Abstract

PURPOSE:To prevent mis-decision by providing a memory storing the relation among reception wave levels of a desired reception channel and adjacent channel, the output of an out-band noise measuring section and the output of an envelope detector in advance and referencing the memory to decide whether the received wave is on the desired channel or the adjacent channel. CONSTITUTION:A computer 12 obtains a received wave level Bd when the received wave is a desired channel wave and the received wave level Bu when the wave is the adjacent channel wave from the level of an out-band noise output 6 and obtains the received wavelevel Dd when the wave is the desired channel wave and the received wave level Du when the wave is the adjacent channel wave from the received envelope level of the received envelope output 9. Then the Bd and the Dd, and the Bu and the Du are compared respectively, and when Bd=Dd, it is decided that the input wave is the desired channel wave and when Bu=Du, it is decided that the received wave is the adjacent channel wave. The result of decision is outputted to the decision output terminal 14. Then the received wave level is outputted to a received electric field level output terminal 15 at the same time.

Description

【発明の詳細な説明】 発明の属する技術分野 本発明は、移動通信における希望チャネルおよび隣接チ
ャネルに対する受信波の電界強度を測定するための受信
電力測定装置に関する。
TECHNICAL FIELD The present invention relates to a received power measuring device for measuring the electric field strength of received waves for a desired channel and an adjacent channel in mobile communication.

従来技術 第1図は、従来のこの種受信電力測定装置の一例を示す
ブロック図である。すなわち、受信波を中間周波数帯域
の信号(IF信号)に変換してIF信号入力端子lに入
力させ、該IF信号をIF増幅器2で増幅し、ディスク
リミネータ3で検波復調された信号を音声信号除去用の
バイパスフィルタ4を通して包結線検波器5に入力させ
る。バイパスフィルタ4の出力は、入力電界強度に応じ
て抑圧された帯域外雑音であり、これを包結線検波器5
を通して平滑された信号を帯域外雑音出力6として出力
し、帯域外雑音出力6のレベルによって受信波の電界強
度を測定する。m域外雑音出力6のレベルと受信波の電
界強度との関係は、受信波が希望チャネルであるか、ま
たは隣接チャネルであるかによって異なり、第2図に曲
線■で希望波に対する受信波電界強度と雑音出力との関
係を示し、曲線■で隣接チャネルに対する受電波の電界
強度と雑音出力との関係を示す、同図の横軸は、受信波
の電界強度(diIL)を示し、縦軸は、帯域外雑音出
力6のレベル(dBs+)を示す。
BACKGROUND ART FIG. 1 is a block diagram showing an example of a conventional received power measuring device of this type. That is, the received wave is converted into an intermediate frequency band signal (IF signal) and inputted to the IF signal input terminal l, the IF signal is amplified by the IF amplifier 2, and the signal detected and demodulated by the discriminator 3 is output as an audio signal. The signal is input to the envelope detector 5 through a bypass filter 4 for signal removal. The output of the bypass filter 4 is out-of-band noise suppressed according to the input electric field strength, which is sent to the envelope detector 5.
The smoothed signal is output as an out-of-band noise output 6, and the electric field strength of the received wave is measured based on the level of the out-of-band noise output 6. The relationship between the level of the m-band noise output 6 and the electric field strength of the received wave varies depending on whether the received wave is the desired channel or the adjacent channel. The curve ■ shows the relationship between the electric field strength of the received wave for the adjacent channel and the noise output. The horizontal axis of the figure shows the electric field strength of the received wave (diIL), and the vertical axis , shows the level (dBs+) of the out-of-band noise output 6.

第2図により、例えば雑音出力が一38dBmのときは
、曲線ψ上の点Aにより、希望チャネルの受信波レベル
はOdB#Lであると判定する。しかし、希望チャネル
の受信波が到来していない場合でも、隣接チャネルの受
信波レベルが高い場合は、曲線ψで示した特性に従って
雑音レベルが抑圧される0例えば隣接チャネルの受信波
が?1dB鉢程度であれば、曲線ψ上の点Bにより雑音
出力は−38dB腸となる。これは、受信器の局部発振
に使用されているシンセサイザの雑音が、隣接チャネル
波によって中間周波数に変換されて、復調雑音を抑圧す
るためである。従って、上述の従来装置は、受信波が希
望チャネル波であるのか又は隣接チャネル波であるのか
を判定できない場合がある。
According to FIG. 2, for example, when the noise output is -38 dBm, the received wave level of the desired channel is determined to be O dB#L from point A on the curve ψ. However, even when the received wave of the desired channel has not arrived, if the received wave level of the adjacent channel is high, the noise level is suppressed according to the characteristic shown by the curve ψ.For example, if the received wave of the adjacent channel is? If it is about 1 dB, the noise output will be -38 dB at point B on the curve ψ. This is because the noise of the synthesizer used for local oscillation of the receiver is converted to an intermediate frequency by the adjacent channel wave, thereby suppressing demodulation noise. Therefore, the conventional device described above may not be able to determine whether the received wave is a desired channel wave or an adjacent channel wave.

第3図に示すような電界測定器も一般に使用されている
。この場合は、受信波は中間周波に変換されてIF信号
入力端子lから対数増幅器7に入力され、対数増幅器7
で搬送波の包絡線が対数圧縮される。そして、包結線検
波器8によって対数増幅器7の出力の包結線を検出し、
受信包結線出力9として出力する。受信包絡線出力9の
レベルは当然受信波レベルに対応している。第4図は。
An electric field measuring device as shown in FIG. 3 is also commonly used. In this case, the received wave is converted to an intermediate frequency and inputted to the logarithmic amplifier 7 from the IF signal input terminal l,
The envelope of the carrier wave is logarithmically compressed. Then, the envelope detector 8 detects the envelope of the output of the logarithmic amplifier 7,
It is output as a reception envelope connection output 9. The level of the received envelope output 9 naturally corresponds to the received wave level. Figure 4 is.

受信波の電界強度と受信包結線出力9のレベル関係を示
す図であり、横軸に受信波の電界強度(di#L)をと
り、縦軸に受信包絡線出力9の包絡線出力レベル(V)
を示す、同図の曲線■は希望波の受信電界強度と包結線
出力との関係を示し、曲線[株]は隣接チャネルに対す
る受信波電界強度と包結線出力の関係を示す、同図から
、例えば、包絡線出力が1.3 Vのときの受信波レベ
ルは曲線■上の0点ではOdB、であり1曲線[株]上
のD点では72dBILとなるから、受信入力が希望波
であるか、隣接波であるかを分離することができない、
これも前述と同様に、中間周波に変換されたシンセサイ
ザ雑音を包結線検波してしまうためである。
It is a diagram showing the level relationship between the electric field strength of the received wave and the received envelope output 9, where the horizontal axis represents the electric field strength (di#L) of the received wave, and the vertical axis represents the envelope output level (di#L) of the received envelope output 9. V)
The curve ■ in the same figure shows the relationship between the received signal field strength of the desired wave and the envelope line output, and the curve [share] shows the relationship between the received wave electric field strength and the envelope line output for the adjacent channel.From the same figure, For example, when the envelope output is 1.3 V, the received wave level is OdB at point 0 on curve ■, and 72 dBIL at point D on curve 1, so the received input is the desired wave. It is not possible to separate whether it is a wave or an adjacent wave,
This is also because, as described above, the synthesizer noise converted to the intermediate frequency is subjected to envelope detection.

移動通信では、多数の無線チャネルを異なる地域で繰り
返し利用しており、移動機がゾーンを移行する際には、
無線チャネルを移行先の無線チャネルに切換えるいわゆ
るチャネル!1lJfiFが行なわれる。このようなチ
ャネル切替または通話開始に際しては、希望チャネルの
電界レベルを測定して、そのチャネルに電波が存在せず
、使用可能であることを判定する必要がある。このため
、′希望チャネル波の受信レベル測定を行うが、上述の
従来装置では、局留チャネル波と隣接チャネル波を分離
して受信レベルを測定することができないため、受信電
力の測定精度が悪いという欠点がある0例えば、前述の
例では、隣接チャネル波が高レベルのとき、aWチャネ
ル波が存在しなくても使用不可能と誤判定してしまう。
In mobile communications, many radio channels are repeatedly used in different regions, and when a mobile device changes zones,
The so-called channel that switches the wireless channel to the destination wireless channel! 1lJfiF is performed. When switching channels or starting a call, it is necessary to measure the electric field level of the desired channel and determine that there is no radio wave in that channel and that it can be used. For this reason, the reception level of the desired channel wave is measured, but with the conventional device described above, it is not possible to separate the local channel wave and the adjacent channel wave and measure the reception level, so the measurement accuracy of the reception power is poor. For example, in the above-mentioned example, when the adjacent channel wave is at a high level, it is incorrectly determined that the aW channel wave is unusable even if it does not exist.

発[Jjの目的 本発明の目的は、上述の従来の欠点を解決し、希望チャ
ネル波と隣接チャネル波とを分離して、受信電力を正確
に測定することが可能な受信電力測定装置を提供するこ
とにある。
An object of the present invention is to solve the above-mentioned conventional drawbacks, and to provide a received power measuring device that can accurately measure received power by separating desired channel waves and adjacent channel waves. It's about doing.

発明の構成 本発明の受信電力測定装置は、受@信号を復調するディ
スクリミネータと、該ディスクリミネータの出力の高域
側帯域外雑音を測定する帯域外雑音測定部と、受信波の
電力レベルを測定するための包結線検波器と、希望受信
チャネルの受信波レベルと前記帯域外雑音測定部の出力
および前記包結線検波器の出力との関係および隣接チャ
ネルに対する受信波レベルと前記帯域外雑音測定部の出
力および前記包結線検波器の出力との関係をあらかじめ
記憶したメモリとを備えて、前記包結線検波器と帯域外
雑音測定部の出力から上記メモリを参照して、受信波が
希望チャネルであるか又は隣接チャネルであるかを判定
することを特徴とする。
Structure of the Invention The received power measuring device of the present invention includes a discriminator that demodulates a received signal, an out-of-band noise measuring section that measures high-frequency out-of-band noise of the output of the discriminator, and a received power measuring device that demodulates a received signal. An envelope detector for measuring the level, a relationship between the received wave level of the desired reception channel, the output of the out-of-band noise measurement unit, and the output of the envelope detector, and the relationship between the received wave level of the adjacent channel and the out-of-band A memory is provided in which the relationship between the output of the noise measuring section and the output of the envelope detector is stored in advance, and the received wave is determined by referring to the memory from the output of the envelope detector and the out-of-band noise measuring section. It is characterized by determining whether it is a desired channel or an adjacent channel.

発明の実施例 次に、本発明について、図面を参照して詳細に説明する
Embodiments of the Invention Next, the present invention will be described in detail with reference to the drawings.

第5図は1本発明の一実施例を示すブロック図である。FIG. 5 is a block diagram showing an embodiment of the present invention.

すなわち、IF信号入力端子lから入力した中間周波数
帯域の信号(IF信号)をIF増幅器2で増幅し、IF
増幅器2の出力をディスクリミネータ3によって検波復
調し、ディスクリミネータ3の出力をバイパスフィルタ
4(カットオ)周波数20kHz)によって帯域外の高
周波雑音を抽出し、包結線検波器5によってバイパスフ
ィルタ4の出力を包結線検波した雑音出力を帯域外雑音
出力6として出力する0本実施例では、バイパスフィル
タ4と包結線検波機5とで、“高域側帯域外雑音を測定
する帯域外雑音測定部”を構成している。一方、IF信
号入力端子lのIF倍信号対数増幅器7を通して包結線
検波器8に入力させ、包結線検波器8によって包結線検
波し、受信包絡線出力9として出力する。帯域外雑音出
力6は、アナログ−ディジタル変換器lOによってディ
ジタル信号に変換されてコンピュータ12に入力され、
受信包結線出力9はアナログ−ディジタル変換器IIに
よってディジタル信号に変換してコンピュータ12に入
力させる。コンピュータ12には、メモリ13が接続さ
れており、メモリ13には、希望チャネル波と隣接チャ
ネル波に対する受信電界レベルと雑音出力および受信波
包結線出力の関係があらかじめ測定され、例えばテーブ
ル形式で格納されている。そして、コンピュータ12は
アナログ−ディジタル変換器lOから入力される雑音出
力レベルと、アナログ−ディジタル変換器11から入力
される受信波包結線出力レベルから、メモリ13を参照
して当該受信波が希望チャネルであるが、または隣接チ
ャネルであるかを判定し、希望チャネル波または隣接チ
ャネル波の受信電界強度をめ、判定出力14および受信
電界レヘル出カ15として出力する。
That is, the intermediate frequency band signal (IF signal) input from the IF signal input terminal l is amplified by the IF amplifier 2, and the IF
The output of the amplifier 2 is detected and demodulated by a discriminator 3, the output of the discriminator 3 is extracted by a bypass filter 4 (cutoff frequency: 20 kHz), high frequency noise outside the band is extracted, and the envelope detector 5 extracts high frequency noise from the bypass filter 4. In this embodiment, the bypass filter 4 and the envelope detector 5 constitute an "out-of-band noise measurement unit that measures high-frequency out-of-band noise". ”. On the other hand, the IF multiplied signal of the IF signal input terminal 1 is inputted to the envelope detector 8 through the logarithmic amplifier 7, the envelope detector 8 performs envelope detection, and the signal is output as a reception envelope output 9. The out-of-band noise output 6 is converted into a digital signal by an analog-to-digital converter lO and input to the computer 12;
The reception envelope output 9 is converted into a digital signal by an analog-to-digital converter II and input to the computer 12. A memory 13 is connected to the computer 12, and in the memory 13, the relationship between the received electric field level, noise output, and received wave envelope output for the desired channel wave and the adjacent channel wave is measured in advance and stored in a table format, for example. has been done. Then, the computer 12 refers to the memory 13 based on the noise output level input from the analog-to-digital converter IO and the received wave envelope output level input from the analog-to-digital converter 11, and determines whether the received wave is the desired channel. However, it determines whether it is a desired channel wave or an adjacent channel wave, and outputs the received electric field strength of the desired channel wave or the adjacent channel wave as a determination output 14 and a received electric field level output 15.

第6図は、受信波の電界強度と帯域外雑音出方レベルお
よび受信包結線出力レベルの関係を示す特性図で、横軸
は受信波の電界強度(dB#L)を示し、左端部に記載
した縦軸には帯域外雑音出方レベル(dB■)を、右端
部に記載した縦軸には受信包結線出力レベル(V)を対
応させている。同図に実線で示した曲線■および■は、
それぞれ希望チャネルおよび隣接チャネルに対する受信
波と雑音出力のレベル関係を示し、第2図で示した特性
と同じである。また、一点鎖線で示した曲線■および[
株]は、それぞれ受信波レベルと受信包絡線出力レベル
の関係を示し、第4図に示した特性と同じである。前記
メモリ13には、希望チャネル波および隣接チャネル波
の受信電界レベルにそれぞれ対応する雑音出力および受
信包結線出力のレベルがテーブル形式で格納されている
Figure 6 is a characteristic diagram showing the relationship between the electric field strength of the received wave, the out-of-band noise output level, and the reception envelope output level.The horizontal axis shows the electric field strength (dB#L) of the received wave, and the left end The vertical axis shown corresponds to the out-of-band noise output level (dB), and the vertical axis shown at the right end corresponds to the receiving envelope output level (V). The curves ■ and ■ shown by solid lines in the same figure are
This shows the level relationship between the received wave and noise output for the desired channel and the adjacent channel, respectively, and the characteristics are the same as those shown in FIG. In addition, the curves ■ and [
4 shows the relationship between the received wave level and the received envelope output level, respectively, and has the same characteristics as shown in FIG. The memory 13 stores in a table format the levels of the noise output and reception envelope output corresponding to the reception electric field levels of the desired channel wave and the adjacent channel wave, respectively.

次に、本実施例の動作について第6図を参照して説明す
る。今、例えば、帯域外雑音出力6のレベルが−44,
5dBm(点Eで示す)であり、受信包結線出力9のレ
ベルが点Hで示す1.53Vであったとする。コンピュ
ータ12は、先ずこの受信波が、希望チャネル波である
ものとして、メモリ13を参照して受信電界をめる。第
6図の曲線■からめた受信電界は1点Fで示す8dBp
であり1曲線■からめた受信電界も点Fで示す8dBp
となり、矛盾はない0次に、受信波が隣接チャネルであ
るものとしてメモリ13から受信電界をめると1曲線■
からは、点Gに示す93dB ILとなり、曲−〇から
は、点Iで示す79.5dJtが得られ、矛盾した結果
となる。従って、コンピュータ12は受信波が希望チャ
ネルであると判定し、判定結果を示す信号を判定出力端
子14に出力し、また受信波レベルを8dBpとして受
信電界レベル出力端子15に出力する。
Next, the operation of this embodiment will be explained with reference to FIG. Now, for example, the level of out-of-band noise output 6 is -44,
5 dBm (indicated by point E), and the level of the reception envelope output 9 is 1.53 V, indicated by point H. First, the computer 12 assumes that the received wave is a desired channel wave and calculates the received electric field by referring to the memory 13. The received electric field combined with the curve ■ in Figure 6 is 8 dBp, which is indicated by one point F.
The received electric field from one curve ■ is also 8 dBp, which is shown by point F.
Therefore, there is no contradiction. If we assume that the received wave is an adjacent channel and the received electric field from the memory 13 is added to the 0th order, we get a curve ■
From the point G, 93 dB IL is obtained, and from the song -0, 79.5 dJt, shown at the point I, is obtained, giving contradictory results. Therefore, the computer 12 determines that the received wave is the desired channel, outputs a signal indicating the determination result to the determination output terminal 14, and outputs the received wave level to the received electric field level output terminal 15 as 8 dBp.

一般的には、コンピュータ12は帯域外雑音出力6のレ
ベルから、受信波が希望チャネル波であるとした場合の
受信波レベルBdと隣接チャネル妓であるとした場合の
受信波レベルBuをめ、受信包絡線出力9の受信包絡線
レベルから、希望チャネル波であるとしたときの受信波
レベルDdと隣接チャネル波であるとした場合の受信波
レベルDuとをめ、次に、上記BdとDdおよびBuと
Duとをそれぞれ比較して、Bd=Ddであれば入力波
は希望チャネル波であり、Bu=Duであれば受信波は
隣接チャネル波であると判定する0判定結果は判定出力
端子14に出力する。同時に、受信波レベルを受信電界
レベル出力端子15に出力する。
Generally, the computer 12 calculates the received wave level Bd when the received wave is the desired channel wave and the received wave level Bu when the received wave is the adjacent channel wave from the level of the out-of-band noise output 6, From the reception envelope level of the reception envelope output 9, determine the reception wave level Dd when it is a desired channel wave and the reception wave level Du when it is an adjacent channel wave, and then calculate the above Bd and Dd. Compare Bu and Du respectively, and if Bd=Dd, it is determined that the input wave is the desired channel wave, and if Bu=Du, it is determined that the received wave is the adjacent channel wave.The 0 determination result is the determination output terminal. Output to 14. At the same time, the received wave level is output to the received electric field level output terminal 15.

ただし、入力波に対する雑音出力および包結線出力が希
望チャネル波と隣接チャネル波に対して同等の特性を持
つようになると、判定精度が低下し、受信入力を測定で
きるダイナミックレンジが狭くなる。
However, if the noise output and envelope output for the input wave have similar characteristics for the desired channel wave and the adjacent channel wave, the determination accuracy decreases and the dynamic range in which the received input can be measured becomes narrower.

第7図は、この点を改良した本発明の他の実施例の特性
を示す図である。これは、第5図に示したバイパスフィ
ルタ4のカットオフ周波数を音声帯域の信号が除去でき
る程度の低い周波数(例えば6kHz程度)としたもの
である、この場合は、希望チャネル波に対する受信波レ
ベルと帯域外維音出力6のレベルの関係は同図に■で示
すようになり、隣接チャネル波に対する雑音出力特性は
、同図に曲線■で示すようになる。前述の実施例では、
バイパスフィルタ4のカットオフが20kH2と高いた
めに、隣接チャネル波の入力レベルが高いときの雑音抑
圧量が大きかったのに比して。
FIG. 7 is a diagram showing the characteristics of another embodiment of the present invention that improves this point. This is because the cutoff frequency of the bypass filter 4 shown in Fig. 5 is set to a low frequency (for example, about 6 kHz) that can remove signals in the audio band.In this case, the received wave level for the desired channel wave is set to The relationship between the level and the level of the out-of-band fiber sound output 6 is shown by a curve ``■'' in the same figure, and the noise output characteristic for adjacent channel waves is shown by a curve ``black'' in the same figure. In the above embodiment,
Since the cutoff of the bypass filter 4 is as high as 20kHz, the amount of noise suppression is large when the input level of the adjacent channel wave is high.

バイパスフィルタ4のカットオフを下げることによって
隣接チャネル波のレベルが高い場合でも雑音抑圧量が少
なくなったためである。入力波が希望チャネル波の場合
は、バイパスフィルタ4のカットオフ周波数を下げた影
響はあまりない、また、受信電界レベルと受信包結線出
力レベルの関係は、希望チャネル波および隣接チャネル
波に対して、それぞれ同図に曲線■および[株]に示す
ようになり、これは、第6図に曲線■および叩で示した
特性とほぼ同じである。
This is because by lowering the cutoff of the bypass filter 4, the amount of noise suppression is reduced even when the level of adjacent channel waves is high. When the input wave is the desired channel wave, lowering the cutoff frequency of the bypass filter 4 has little effect, and the relationship between the received electric field level and the received envelope output level is similar to the desired channel wave and the adjacent channel wave. , respectively, as shown by curves ■ and [stock] in the same figure, which are almost the same as the characteristics shown by curves ■ and curves in FIG. 6.

今、雑音出力が第7図に点りで示す一39dB■で、包
結線出力が点Mで示す1.28Vであるものとすると、
受信入力が隣接チャネル波であると仮定した場合の受信
電界レベルは、曲線[株]からは点Nで示す72dBp
となり1曲線■からは受信電界レベルをめることができ
ない、従って、上記仮定は棄却される。そして、入力波
は希望チャネル波であると判定され、曲線りりおよび■
から、受信電界が0dBILであることがめられる。す
なわち、受信波が希望チャネル波であるか隣接チャネル
波であるかを判定する精度が向上する利点がある。また
、受信波が希望チャネル波である場合と隣接チャネル波
である場合とでは、雑音抑圧量が大きく異なり、雑音出
力がP以下の範囲では、雑音出力から一意的に受信電界
レベルが決定される利点がある。上述の特性例では、受
信電界が一10dBx以上であれば、雑音出力から一意
的に高精度で受信電界レベルをめることが可能である。
Now, suppose that the noise output is -39 dB as shown by the dot in Fig. 7, and the envelope output is 1.28 V as shown by the point M.
Assuming that the received input is an adjacent channel wave, the received electric field level is 72 dBp as indicated by point N from the curve.
The received electric field level cannot be estimated from the curve 1, so the above assumption is rejected. Then, the input wave is determined to be the desired channel wave, and the curve and ■
From this, it can be seen that the received electric field is 0 dBIL. That is, there is an advantage that the accuracy of determining whether a received wave is a desired channel wave or an adjacent channel wave is improved. Furthermore, the amount of noise suppression differs greatly depending on whether the received wave is a desired channel wave or an adjacent channel wave, and in the range where the noise output is below P, the received electric field level is uniquely determined from the noise output. There are advantages. In the above characteristic example, if the received electric field is 110 dBx or more, it is possible to uniquely and accurately determine the received electric field level from the noise output.

これは。this is.

実用上十分な範囲をカバーしている。Covers a sufficient range for practical use.

発11の効果 以上のように、本発明においては、希望チャネル波と隣
接チャネル波に対して、それぞれ受信電界と雑音出力お
よび受信包絡線出力のレベル関係をめてメモリに格納し
ておき、受信波に対する雑音出力レベルおよび受信包絡
線出力レベルを測定し、上記2つの測定値から前記メモ
リを参照して希望チャネル波または隣接チャネル波とし
ての受信電界レベルをめるように構成したから、入力波
が希望チャネル波であるか隣接チャネル波であるかを適
確に判定し、高精度で受信電界レベルを測定することが
できるという効果がある。
As described above, in the present invention, the level relationship between the received electric field, noise output, and received envelope output for the desired channel wave and the adjacent channel wave is stored in memory, and the received The noise output level and reception envelope output level for the wave are measured, and the received electric field level as the desired channel wave or adjacent channel wave is calculated by referring to the memory from the above two measured values. This has the advantage that it is possible to accurately determine whether a wave is a desired channel wave or an adjacent channel wave, and to measure the received electric field level with high accuracy.

本発明を移動通信に適用し、移動機がゾーンを移行する
際に移行先の無線チャネルに切換えるいわゆるチャネル
切換え時に、希望チャネルが空であることを確認するた
めの受信電界測定に利用すれば、隣接チャネルからの干
渉の影響を除去することができ、同一チャネル干渉(同
じ周波数を使用する他のゾーンの無線チャネルからの干
渉)に対する許容量と、隣接チャネル干渉に対する許容
量とを別個に設定することができるという利点もある。
If the present invention is applied to mobile communications and used to measure the received electric field to confirm that the desired channel is empty during so-called channel switching, when a mobile device switches to a new wireless channel when changing zones, The effects of interference from adjacent channels can be removed, and the tolerance for co-channel interference (interference from radio channels in other zones that use the same frequency) and the tolerance for adjacent channel interference are set separately. There is also the advantage of being able to

また、従来のように、希望チャネルが使用されていない
場合に、高レベルの隣接チャネルの受信波によって希望
チャネルが使用中であると誤判定することを防止できる
という効果がある。
Furthermore, unlike in the prior art, when a desired channel is not in use, it is possible to prevent an erroneous determination that the desired channel is in use due to a received wave of a high-level adjacent channel.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の受信電界測定装置の一例を示すブロック
図、第2図は上記従来例の雑音出力特性を示す図、第3
図は従来の電界測定器の一例を示すブロック図、第4図
は上記従来例の包結線出力特性を示す図、第5図は本発
明の一実施例を示すブロック図、第6図は、上記実施例
の雑音出力特性および受信包結線出力特性を示す図、第
7図は本発明の他の実施例における雑音出力特性゛およ
び受信包絡線出力特性を示す図である。 図において、l:IF信号入力端子、2:IF増幅器、
3:ディスクリミネータ、4:バイパスフィルタ、5:
包結線検波器、6:帯域外雑音出力、7:対数増幅器、
8:包結線検波器、9:受信包絡線出力、10,11:
アナログ−ディジタル変換器、12:コンピュータ、1
3:メモIハ14=判定出力端子、15:受信電界レベ
ル出力端子。 出願人 日本電信電話公社 代理人 弁理士 住田俊宗
Fig. 1 is a block diagram showing an example of a conventional received electric field measuring device, Fig. 2 is a diagram showing the noise output characteristics of the above conventional example, and Fig. 3 is a block diagram showing an example of a conventional received electric field measuring device.
FIG. 4 is a block diagram showing an example of a conventional electric field measuring device, FIG. 4 is a diagram showing envelope line output characteristics of the conventional example, FIG. 5 is a block diagram showing an embodiment of the present invention, and FIG. 6 is a block diagram showing an example of the conventional electric field measuring device. FIG. 7 is a diagram showing the noise output characteristic and reception envelope output characteristic of the above embodiment, and FIG. 7 is a diagram showing the noise output characteristic and reception envelope output characteristic in another embodiment of the present invention. In the figure, l: IF signal input terminal, 2: IF amplifier,
3: Discriminator, 4: Bypass filter, 5:
Enveloping line detector, 6: Out-of-band noise output, 7: Logarithmic amplifier,
8: Envelope detector, 9: Reception envelope output, 10, 11:
Analog-digital converter, 12: Computer, 1
3: Memo Ic 14=judgment output terminal, 15: Received electric field level output terminal. Applicant: Nippon Telegraph and Telephone Public Corporation Agent: Patent Attorney: Toshimune Sumita

Claims (1)

【特許請求の範囲】[Claims] 受信信号を復調するディスクリミネータと、該ディスク
リミネータの出力の高域側帯域外雑音を測定する帯域外
雑音測定部と、受信波の電力レベルを測定するための包
絡線検波器と、希望受信チャネルの受信波レベルと前記
帯域外雑音測定部の出力および前記包結線検波器の出力
との関係および隣接チャネルに対する受信波レベルと前
記帯域外雑音測定部の出力および前記包結線検波器の出
力との関係をあらかじめ記憶したメモリとを備えて、前
記包結線検波器と帯域外雑音測定部の出力から上記メモ
リを参照して、受信波が希望チャネルであるか又は隣接
チャネルであるかを判定することを特徴とする受信電力
測定装置。
a discriminator that demodulates a received signal, an out-of-band noise measurement unit that measures high-frequency out-of-band noise of the output of the discriminator, an envelope detector that measures the power level of the received wave, and The relationship between the received wave level of a receiving channel, the output of the out-of-band noise measurement unit, and the output of the envelope detector; and the relationship between the received wave level of an adjacent channel, the output of the out-of-band noise measurement unit, and the output of the envelope detector. and a memory in which the relationship between the signals and the signals is stored in advance, and determines whether the received wave is a desired channel or an adjacent channel by referring to the memory from the outputs of the envelope detector and the out-of-band noise measuring section. A received power measuring device characterized by:
JP59055790A 1984-03-23 1984-03-23 Reception power measurement device Pending JPS60199246A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59055790A JPS60199246A (en) 1984-03-23 1984-03-23 Reception power measurement device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59055790A JPS60199246A (en) 1984-03-23 1984-03-23 Reception power measurement device

Publications (1)

Publication Number Publication Date
JPS60199246A true JPS60199246A (en) 1985-10-08

Family

ID=13008704

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59055790A Pending JPS60199246A (en) 1984-03-23 1984-03-23 Reception power measurement device

Country Status (1)

Country Link
JP (1) JPS60199246A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0738513A (en) * 1993-07-21 1995-02-07 Nec Corp Radio receiver

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0738513A (en) * 1993-07-21 1995-02-07 Nec Corp Radio receiver

Similar Documents

Publication Publication Date Title
US5067171A (en) Method and apparatus for hand-off of call in progress
US5129098A (en) Radio telephone using received signal strength in controlling transmission power
US5010584A (en) Mobile communication transceiver
WO2001048933A1 (en) Receiver and gain control method
US5918184A (en) Method and apparatus for detecting a supervisory audio tone
CN1938958A (en) Am reception circuit
KR0168790B1 (en) Apparatus for extending dynamic range of rssi
JPH11298343A (en) Portable communication equipment
WO1993020622A1 (en) Squelch detector
JPS60199246A (en) Reception power measurement device
US5983080A (en) Apparatus and method for generating voice signals at a wireless communications station
US6415139B1 (en) Detection circuit of tone signal
JP3505790B2 (en) Digital radio receiver
JP4742859B2 (en) Radio, control method and program
JP2000031723A (en) Broad band digital receiver
JP2751667B2 (en) Cellular receiver
JPH0314841Y2 (en)
JP3002240B2 (en) Radio receiver
JP2004180156A (en) Apparatus for detecting interference wave, receiving apparatus, and communication apparatus
JP2000174643A (en) Digital radio receiver
JPS63215121A (en) Interference detector
JPH03171832A (en) Mobile radio reception method
JPH01122216A (en) Reception equipment
JPH1188205A (en) Digital radio receiver
JPH0317254B2 (en)