JPH0434633Y2 - - Google Patents

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Publication number
JPH0434633Y2
JPH0434633Y2 JP6692682U JP6692682U JPH0434633Y2 JP H0434633 Y2 JPH0434633 Y2 JP H0434633Y2 JP 6692682 U JP6692682 U JP 6692682U JP 6692682 U JP6692682 U JP 6692682U JP H0434633 Y2 JPH0434633 Y2 JP H0434633Y2
Authority
JP
Japan
Prior art keywords
cabinet
ellipse
dome
diffraction
section
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.)
Expired
Application number
JP6692682U
Other languages
Japanese (ja)
Other versions
JPS58169787U (en
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 filed Critical
Priority to JP6692682U priority Critical patent/JPS58169787U/en
Publication of JPS58169787U publication Critical patent/JPS58169787U/en
Application granted granted Critical
Publication of JPH0434633Y2 publication Critical patent/JPH0434633Y2/ja
Granted legal-status Critical Current

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  • Details Of Audible-Bandwidth Transducers (AREA)

Description

【考案の詳細な説明】 本考案は、回折(diffraction)による影響を除
去したスピーカ・キヤビネツトに関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a speaker cabinet that eliminates the effects of diffraction.

一般にスピーカ・ユニツトから放射される音波
はキヤビネツトの形状によつて回折の影響を受け
る。この回折による音圧周波数特性上の攪乱を除
去するには、キヤビネツトの形状を球体のような
滑らかな曲線とするのが望ましい。しかし、そう
すると、音圧を前面に押し出すバツフル効果が減
退し能率が低下する。したがつて、バツフル効果
による感度上昇の点からは、逆に直方体のキヤビ
ネツトの方がよい。この考えに基いて、キヤビネ
ツトの形状に楕円のような曲線を取り入れたキヤ
ビネツトが考案されている。
Generally, sound waves emitted from a speaker unit are affected by diffraction depending on the shape of the cabinet. In order to eliminate disturbances in the sound pressure frequency characteristics due to this diffraction, it is desirable that the shape of the cabinet be a smooth curve like a sphere. However, in this case, the buffling effect that pushes the sound pressure to the front is diminished, resulting in a decrease in efficiency. Therefore, from the viewpoint of increasing sensitivity due to the buffling effect, a rectangular parallelepiped cabinet is better. Based on this idea, a cabinet has been devised that incorporates an elliptical curve into the shape of the cabinet.

第1図及び第2図は、かかる従来キヤビネツト
の例を示す略図である。第1図Aは第1例の側面
図、第1図Bはその断面図、第2図Aは第2例の
側面図、第2図Bはその断面図である。第1例に
おいては、断面が楕円に似た形状で横方向には滑
らかであるが上部及び接地面に角(かど)があ
り、この部分で回折(矢印で示す。)が起こる。
第2例は、回転楕円体のキヤビネツトであるが、
接地面でやはり回折が起こるほか、各スピーカの
取付け部周辺が異形となり各スピーカからの音波
に位相差が生じる欠点がある。
1 and 2 are schematic diagrams showing examples of such conventional cabinets. FIG. 1A is a side view of the first example, FIG. 1B is a sectional view thereof, FIG. 2A is a side view of the second example, and FIG. 2B is a sectional view thereof. In the first example, the cross section is shaped like an ellipse and is smooth in the lateral direction, but there are corners at the top and the ground plane, and diffraction (indicated by arrows) occurs at these parts.
The second example is a spheroidal cabinet,
In addition to diffraction occurring on the ground plane, the area around the mounting portion of each speaker is irregularly shaped, resulting in a phase difference between the sound waves from each speaker.

本考案は、これらの欠点を改良するため、キヤ
ビネツトを超楕円体としたものである。以下、図
面により本考案を具体的に説明する。
In the present invention, in order to improve these drawbacks, the cabinet is made into a superellipsoid. Hereinafter, the present invention will be explained in detail with reference to the drawings.

第3図は、超(スーパー)楕円の例を示す図で
ある。超楕円については、例えば昭和51年8月発
行の「科学朝日」に新しい形として紹介されてい
て公知である。普通の楕円は、一般に次の式で表
わされる。
FIG. 3 is a diagram showing an example of a super ellipse. The hyperellipse is well known, for example, as it was introduced as a new shape in ``Science Asahi'' published in August 1976. An ordinary ellipse is generally expressed by the following formula.

(x/a)2+(y/b)2=1 ここに、2aは長径、2bは短径である。 (x/a) 2 +(y/b) 2 =1 where 2a is the major axis and 2b is the minor axis.

この楕円の式を拡張して (x/a)n+(y/b)n=1 なる式を考えた場合、n=2のときは楕円であ
るがn>2になると楕円の縁がふくらみ始め、n
=∞ではこの変形楕円に外接する長方形となる
(第3図参照)。このn>2で普通の楕円より少し
外に張り出した形の楕円を超楕円という。すなわ
ち、超楕円は、楕円と長方形の中間に位置し、長
方形と接する部分が楕円よりカーブが小さく殆ど
直線になるという特徴を有する。本考案は、この
超楕円の特徴を有効に利用したものである。
If we extend this ellipse formula and consider the formula (x/a) n + (y/b) n = 1, when n = 2, it is an ellipse, but when n>2, the edges of the ellipse swell. beginning, n
At =∞, it becomes a rectangle circumscribing this deformed ellipse (see Figure 3). An ellipse with n>2 that extends slightly outward from a normal ellipse is called a superellipse. That is, a superellipse is located between an ellipse and a rectangle, and has a characteristic that the portion that touches the rectangle has a smaller curve than the ellipse and is almost a straight line. The present invention effectively utilizes the characteristics of this superellipse.

第4図は本考案の好適な実施例を示す斜視図、
第5図はその側面図である。図において、1は超
楕円体のキヤビネツトを全体として示し、11
上部ドーム、12は胴部、13は下部ドームであ
る。2はキヤビネツト1を支持する脚、3は大口
径スピーカ・ユニツト、4は中口径スピーカ・ユ
ニツト、5は小口径スピーカ・ユニツトを示す。
上部ドーム11は上部の回折を除去するための超
楕円体ドーム、下部ドーム13は下部及び接地面
における回折及び反射を除去するための超楕円体
ドームである。これらの超楕円体ドームは、第6
図A,Bに示す様に全ての横断面及び頂点を基準
とした縦断面図が部分的に超楕円曲線を持つよう
に構成されている。即ち、胴部12は横断面が超
楕円形である筒状体であり、その両端の輪郭ない
し射影は略直線状である。更に上下ドーム11
び13は第6図Bにその横断面図(x−y平面)
が示されている様に胴部12と同様にどの断面に
おいても超楕円形状であり、頂点14を基準とし
た縦断面図(o−z平面)では第6図Aに示す様
に超楕円形状をx軸に平行な面(例えばx面)で
切断した形状と成されている。尚第6図Aの一点
鎖線で示される超楕円形状は第6図Bの一点鎖線
における断面を示している。ただし、超楕円キヤ
ビネツト1を上部ドーム11、胴部12及び下部ド
ーム13に分けたのは製作上の便宜からであつて、
これらを一体出来に構成してもよい。したがつ
て、超楕円キヤビネツト1は、表面がすべて連続
で滑らかであり回折を起こす部分は全くない。よ
つて、回折効果の除去に極めて有効である。ま
た、各スピーカ・ユニツト3,4,5を取り付け
る部分が横から見てほぼ直線状であり縦(上)か
ら見ても殆ど直線的であるから、第2図の例のよ
うに位相差を生ぜず定位感があり、また回折効果
除去とバツフル効果の利用が同時にできる利点が
ある。
FIG. 4 is a perspective view showing a preferred embodiment of the present invention;
FIG. 5 is a side view thereof. In the figure, 1 indicates a superellipsoidal cabinet as a whole, 1 1 is an upper dome, 1 2 is a body, and 1 3 is a lower dome. 2 is a leg supporting the cabinet 1; 3 is a large-diameter speaker unit; 4 is a medium-diameter speaker unit; and 5 is a small-diameter speaker unit.
The upper dome 11 is a superellipsoidal dome for removing diffraction at the upper part, and the lower dome 13 is a superellipsoidal dome for removing diffraction and reflection at the lower part and the ground plane. These hyperellipsoidal domes are the sixth
As shown in Figures A and B, all cross sections and vertical cross sections based on the apex are constructed so as to partially have hyperelliptic curves. That is, the body 1 2 is a cylindrical body having a super elliptical cross section, and the contours or projections of both ends thereof are approximately linear. Furthermore, the cross-sectional view (x-y plane) of the upper and lower domes 1 1 and 1 3 is shown in Figure 6B.
As shown in FIG . The shape is obtained by cutting an elliptical shape along a plane parallel to the x-axis (for example, the x-plane). The super elliptical shape indicated by the dashed-dotted line in FIG. 6A shows a cross section taken along the dashed-dotted line in FIG. 6B. However, the reason why the superelliptic cabinet 1 is divided into an upper dome 1 1 , a body 1 2 , and a lower dome 1 3 is for manufacturing convenience.
These may be constructed as one unit. Therefore, the entire surface of the superelliptic cabinet 1 is continuous and smooth, and there are no parts that cause diffraction. Therefore, it is extremely effective in removing diffraction effects. In addition, since the parts to which each speaker unit 3, 4, and 5 are attached are almost linear when viewed from the side and almost straight when viewed from the vertical (top), the phase difference can be adjusted as shown in the example in Figure 2. It has the advantage of being able to eliminate diffraction effects and utilize the buffling effect at the same time.

第7図は、上下ドーム11,13及び胴部12
断面の超楕円形をn=2.7としたときの周波数特
性を示す曲線図である。図において、実線の曲線
はスピーカ・ユニツトを上記の超楕円キヤビネツ
トに入れて測定したもの、点線の曲線は同じスピ
ーカ・ユニツトをJIS箱に入れて測定したものを
示す。図からみると、本考案によれはピークやデ
イツプの低域効果が著しいことが分かる。
FIG. 7 is a curve diagram showing frequency characteristics when the superelliptical cross sections of the upper and lower domes 1 1 , 1 3 and the body 1 2 are set to n=2.7. In the figure, the solid line curve shows the measurement taken with the speaker unit placed in the above-mentioned hyperelliptical cabinet, and the dotted line curve shows the measurement made with the same speaker unit placed in the JIS box. From the figure, it can be seen that the present invention has a remarkable low-frequency effect of peaks and dips.

なお、上述の実施例では、上下に超楕円体ドー
ムを付けたが、上部ドームのみ設けた場合でも同
様の効果が得られる。また、単一のスピーカ・ユ
ニツトのみの場合やバツフル孔を設けた場合でも
効果があることは、勿論である。
In the above-described embodiment, superellipsoidal domes are provided at the top and bottom, but the same effect can be obtained even if only the upper dome is provided. Furthermore, it goes without saying that the effect can be obtained even when only a single speaker unit is used or when a buffle hole is provided.

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

第1図及び第2図は従来例を示す略図、第3図
は超楕円の例を示す図、第4図及び第5図は本考
案の好適な実施例を示す図、第6図は本考案の上
下ドームの超楕円を示す図、第7図は本考案の効
果を示す周波数特性曲線図である。 11……上部超楕円体ドーム、12……横断面が
超楕円形の胴部、13……下部超楕円体ドーム。
FIGS. 1 and 2 are schematic diagrams showing a conventional example, FIG. 3 is a diagram showing an example of a superellipse, FIGS. 4 and 5 are diagrams showing a preferred embodiment of the present invention, and FIG. 6 is a diagram showing the present invention. FIG. 7 is a diagram showing the superellipses of the upper and lower domes of the invention, and is a frequency characteristic curve diagram showing the effects of the invention. 1 1 ... Upper hyperellipsoidal dome, 1 2 ... Body with superellipsoidal cross section, 1 3 ... Lower hyperellipsoidal dome.

Claims (1)

【実用新案登録請求の範囲】 1 横断面がすべて超楕円形であり且つ少なくと
も上部においては頂点を基準とした縦断面が部
分的に超楕円曲線を持つように構成されたスピ
ーカ・キヤビネツト。 2 下部においても頂点を基準とした縦断面が部
分的に超楕円曲線を持つように構成された実用
新案登録請求の範囲第1項記載のスピーカ・キ
ヤビネツト。
[Claims for Utility Model Registration] 1. A speaker cabinet whose cross section is entirely superelliptical, and at least in the upper part, the longitudinal section with the apex as a reference partially has a superelliptic curve. 2. The speaker cabinet according to claim 1 of the utility model registration, wherein the vertical cross section with respect to the apex also partially has a hyperelliptic curve even in the lower part.
JP6692682U 1982-05-08 1982-05-08 speaker cabinet Granted JPS58169787U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6692682U JPS58169787U (en) 1982-05-08 1982-05-08 speaker cabinet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6692682U JPS58169787U (en) 1982-05-08 1982-05-08 speaker cabinet

Publications (2)

Publication Number Publication Date
JPS58169787U JPS58169787U (en) 1983-11-12
JPH0434633Y2 true JPH0434633Y2 (en) 1992-08-18

Family

ID=30076770

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6692682U Granted JPS58169787U (en) 1982-05-08 1982-05-08 speaker cabinet

Country Status (1)

Country Link
JP (1) JPS58169787U (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002544603A (en) * 1999-05-10 2002-12-24 ギエリス ヨウハン Pattern synthesis method and apparatus
WO2009038084A1 (en) * 2007-09-21 2009-03-26 Sanyo Electric Co., Ltd. Diaphragm and speaker including same

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0537595Y2 (en) * 1986-10-31 1993-09-22

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002544603A (en) * 1999-05-10 2002-12-24 ギエリス ヨウハン Pattern synthesis method and apparatus
JP4753474B2 (en) * 1999-05-10 2011-08-24 ギエリス ヨウハン Pattern synthesis method and apparatus
WO2009038084A1 (en) * 2007-09-21 2009-03-26 Sanyo Electric Co., Ltd. Diaphragm and speaker including same
JP2009077300A (en) * 2007-09-21 2009-04-09 Sanyo Electric Co Ltd Diaphragm and speaker equipped with the same

Also Published As

Publication number Publication date
JPS58169787U (en) 1983-11-12

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