稀客音响招募全国代理商工程商集成商合作伙伴

 找回密码
 注册

扫一扫,访问微社区

搜索
楼主: 廖喇叭

欣赏JBL的1500AL喇叭

  [复制链接]

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:28 | 显示全部楼层
涉及音响灯光机械视频方案从此不求人,秒拿预算!
以下是一篇解绍1500AL喇叭开发过程的文章,以及这款喇叭需要达到的一重要参数是失真。它是从1999年开始立项开发的,大约在2003年完成。而且这款喇叭并不是凭空开发的,它是在1400ND基础上搞的。而1400ND是1989开发的喇叭用在K2-9500上。

请大家重点关注,他们解释的失真的原因以及他们应对的方法。  当然,希望声学楼里的高手,对这些做一个评价。最好能提出你的解决问题的方法,供大家学习。


Development of the 1500AL traces back to the first K2 low frequency driver, the 1400Nd. That driver was originally developed in 1989 for the K2-S9500 by Doug Button, currently Vice President of Research and Development at JBL Professional. The intent was to go “all out” in the design of a linear, low distortion, high output driver. From Doug’s perspective, there was only one way to achieve the lowest possible distortion – an underhung design. Underhung designs use a voice coil that is considerably shorter than the magnetic gap in which it is suspended. Most dynamic loudspeakers use a voice coil that extends well above and below the magnetic gap to make the most use of the magnetic energy. However, there is a price in increased distortion. It has to do with the fact that the coil is not acted upon symmetrically by the permanent field once it is displaced from the rest position.  Conversely, in an underhung design, the full coil is always immersed in a constant strength magnetic field since it never leaves the gap.

Underhung designs are not common in dynamic loudspeakers due to their cost. The fact that the coil height is less than the gap height means that there are always portions of the permanent field that are not in contact with the coil. This is wasted magnetic energy and requires an inordinately strong magnet to ensure reasonable sensitivity. To gain the necessary magnetic flux levels, Doug specified the very first use of neodymium magnets for low frequency transducers. Neodymium magnets have approximately 10 times the magnetic energy by weight as ferrite magnets. Their use resulted in a relatively compact driver that was exceptionally free from distortion, yet had high sensitivity and high output.

The 1400Nd driver, and subsequent K2 systems that employed it, were a stunning success. However, Doug was not completely satisfied. Classic underhung designs have a unique frequency response anomaly that is due to the coil topology. It regards eddy currents set up by the moving coil in the gap. These currents act as the secondary in a transformer to effectively short out the coil circuit leading to a loss in voltage drive. The net result is a “swayback” response curve through the midband with about a 2db drop in output. While this can be dealt with in network compensation, the purist in Doug wanted that energy back. Addressing this would be the starting point for the 1500AL design.

Design work for the K2-S9800 and its transducers began in 1999. The focal point of this system was to be an Alnico magnet woofer with an underhung coil. Alnico had been the magnetic material of choice for JBL from its very inception until the late 1970’s. In 1978, a civil war in Zaire resulted in the temporary embargo of the commercial supply of cobalt that was a primary ingredient in Alnico. Over a one year period, virtually every loudspeaker manufacturer was forced to switch to more readily available ferrite magnets.

Initially, this magnetic material presented problems compared to Alnico. It was less powerful by weight, requiring much more magnetic material than an equivalent Alnico. It was more susceptible to flux modulation caused by voice coil currents and more susceptible to flux loss due to heating. None of these constraints were absolute. Through innovative engineering (eg. SFG, VGC and SVG motors), JBL was able to develop ferrite magnet drivers that exceeded the performance of the previous Alnico versions.

Nonetheless, the ferrite developments led to an interesting question. What would happen if the same level of innovation applied to ferrite designs were applied to Alnico motors? As described above, Alnico starts off with a number of intrinsic advantages compared to other magnetic materials. By leveraging these advantages, it should be possible to achieve new levels of accuracy.

This became the design goal for the 1500AL. The intent was to end up with a bass driver with the lowest distortion possible while retaining the efficiency and dynamic response that were the hallmarks of JBL. However, there was one major disadvantage in Alnico loudspeakers that would have to be addressed – the susceptibility to permanent demagnetization due to overpowering.

This phenomenon is a result of variability in strength of the permanent magnetic field caused by interference from the voice coil’s electromagnetic field. This is referred to as flux modulation and is a leading cause of distortion in any dynamic loudspeaker. The electromagnetic field generated in the coil pushes against the global magnetic field set up by the permanent magnet and return circuit, causing it to “bend”. Under normal operating conditions, Alnico magnets actually resist this bending better than most other magnet materials. However, should this shift become large enough, it will exceed the coercivity of Alnico and cause it to partially demagnetize.

JBL had done extensive work in stabilizing flux modulation during the conversion to ferrite magnet motors. Ferrite is much more susceptible to flux modulation than Alnico. The coercivity is much higher so that extreme modulation will not result in demagnetization. However, under normal operating conditions, this flux modulation will manifest itself as second order harmonic distortion. By installing a copper shorting ring around the base of the pole piece, JBL engineers were able to reduce flux modulation, and therefore distortion levels in ferrite motors, to very low levels.

Doug Button realized that this same technology could be extended to control flux modulation to such a degree that the coercivity in an Alnico magnet would never be exceeded. He specified a huge copper shorting ring that would buck any changes in the global field that was induced by the voice coil signal. The result was that the major drawback of using Alnico for a loudspeaker magnet had been completely eliminated.

Nonetheless, Doug was not done in setting the design parameters for the 1500AL. There remained the previously identified issue of midband loss in output and a more subtle form of flux modulation that was not addressed with the large shorting ring. Doug would devise an ingenious solution that would resolve both of these issues – a lamination of copper and steel rings applied to the outside diameter of the voice coil gap.

Before detailing this solution, it is worthwhile understanding the phenomenon of “local” flux modulation. The variability in the overall strength of the permanent magnetic field is referred to as “global” flux modulation and this was controlled through a massive shorting ring. However local variance in the flux field was determined to exist in the voice coil gap, independent of variance in the global field. It was particularly an issue for an underhung design like the 1500AL which had an inordinately deep gap. The AC field generated by the voice coil would cause variance in the gap strength from top to bottom that dynamically resulted in a teeter tottering effect. Doug realized that another copper shorting ring placed in the gap would address this phenomenon. However, it came to him as an inspiration, that by interspersing steel coils in between a series of copper coils, he could break up the eddy currents that were causing the midband loss. Thus, came the specification for a series of laminated coils of alternating copper and steel construction that would be applied to the outside diameter of the coil gap.

With this final attribute, the conceptual design for the 1500AL was set. However, there was now the formidable task of developing the concept into a production driver. Responsibility for this would fall upon Jerry Moro, Senior Transducer Engineer for JBL Consumer Products. Jerry recognized that for the dynamic range requirement of modern digital sources, the driver would have to accommodate large excursions. A large coil would be required, but to maintain the underhung topology, there would need to be a gap depth of unprecedented proportions. Ultimately, a 0.8” long coil would be suspended in a 1.5” deep gap. This would accommodate 1” of peak to peak excursion. The magnetic energy requirements to provide a reasonable flux density in such a deep gap was enormous. It resulted in an Alnico magnet of massive proportions. An Alnico slug weighing over 5lbs became the core of the motor structure. The overall structure would weigh over 30lbs.

The large excursion requirements presented unique suspension demands. Normally, the surround and spider are designed to act together to provide restoring force and damping for the cone movement. However, with these large excursions, the different construction of the surround and spider would result in non symmetric response to deflections and therefore distortion. Jerry addressed this by designing a mirror imaged pair of spiders that acted symmetrically and thus allowed the surround to be optimized for linearity. Mirror imaging the spiders resulted in any distortion components being cancelled out.

A major focus of Jerry’s design for the 1500AL was to minimize power compression. Power compression regards a reduction in output as power levels increase. It is the biggest factor in restricting dynamic response. Therefore, mitigating it to the maximum degree became a design objective. Heat is by far the major culprit behind dynamic compression. It causes energy losses in the permanent magnetic field and impedance changes in the coil that conspire to reduce output as heat builds up. Jerry designed a series of measures to dissipate heat.

First, the pole piece and magnet have three channels embedded along their outer circumference. Air trapped behind the dustcap is forced past the coil and out these channels to convectively cool the coil. Next, an aluminum motor cap completely surrounds the magnetic return structure. A series of ribs draws heat away from the iron pot to the cap which acts as a large heat sink. Finally, there is an air gap between the cap and the pot structure that is vented in the rear. The motion of the spiders pumps air into this gap to provide further convective cooling.

The net result is a woofer that arguably has lower levels of power compression than any other loudspeaker of its size. It can sustain maximum output levels of 118db with minimal distortion. Testing at a 110db output level revealed midband distortion to be down 50db, or around 0.3%. In summary, the 1500AL sets an unprecedented standard for accuracy, dynamic response and freedom from distortion

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:29 | 显示全部楼层
这是1500AL 的T/S参数:

Fs = 27.3 hz
Qts = 0.27
Qes = 0.28
Qms = 12.84
Vas = 264.55 l
Sd = 880 sq cm
Re = 5.4 ohms
Mms = 139.9g
Bl = 21.64 T*m
Spl = 94.7 dB.

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:36 | 显示全部楼层
为了取得最好的失真,1500AL用了短音圈(underhung)的设计,短音圈的设计的音圈卷幅要比磁隙要短很多。一般的大功率喇叭用的音圈在运动时,都会高出和低于磁隙,这是为了更好的利用磁力的原故,但是其代价就是加大了失真 ,因为线圈的运动不很均匀。相反,沉浮式的设计的音圈永远都不会脱离磁场,因为,它一直是沉浸在磁场内的。但这种设计在一般喇叭中较少用,因为成本高,沉浮式的设计的音圈卷幅要比磁隙要短意为作有一部分磁力是浪费了,为此为了取得合理的灵敏度,就需要一个很强的磁铁。汝铁錋磁铁在这种设计中用的很多。 但是这种经典的沉浮式的设计,由于线圈的结构布局问题造成了频响有一点异常。这是由动圈在隙里面的漩涡流造成的。这种涡流影响了线圈电路并造成了电压降低。表现在频响上就是在中频有2db的衰减。虽然,在做系统时这可以通过分频器来补赏,但是如何能够在设计喇叭时,消除这种情况呢

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:38 | 显示全部楼层
1500AL用的是ALNICO磁铁,同FERRITE相比,在同样重量下它更强劲,需要的磁性材料更少,而且受线圈电流造成的磁通量调制要少,在温度升高时磁通量损失也较少。 在用FERRITE做磁钢时,JBL发明了很多种磁路(如SFG,VGC,SVG等),这些磁路都有效克服了FERRITE的弱点。现在JBL想把这些磁路用在ALNCO上来,情况会如何呢?但是ALNICO磁铁有个重大的不足之处---在大功率时容易消磁,如何解决 这个难题呢?

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:40 | 显示全部楼层
这种消磁现象是由音圈的电磁场干扰了永磁场,从而造成了永磁场的力度发生变异。这有关磁通调制,并且是造成喇叭失真的主要原因。由线圈引起的电磁场冲击有磁钢
和回路引起的总磁场,并使后者“弯曲”。在一般情况下,ALNICO磁铁抗这种“弯曲”的力比其它磁铁要好。但是,当“弯曲”力变得很大超过了它的矫顽力时就会造成消磁

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:41 | 显示全部楼层
在用FERRITE磁钢设计磁路时JBL做了很多设计来平衡磁通调制。FERRITE受磁通调制的影响要比ALNICO要大。但是它的矫顽力要高很多,所以没有消磁现象。但是在一般情况下,磁通调制会引起二次谐波失真。当在柱体底部加以个铜短路环后,FERRITE的这种失真就降到了很低了。

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:41 | 显示全部楼层
这种在FERRITE上结构设计,同样可以用到ALNICO上来控制磁通调制,使其不会超过矫顽力。JBL想到了设计一个大的铜短路环来消除由音圈信号造成的总磁场的各种变动。这样就能克服掉ALNICO做磁钢时的这个重大缺点

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:42 | 显示全部楼层
但是,这个大铜短路环并没有解决先前讲大的中频段的2db损失,也不能解决一些细微的磁通调制。必须要找到一个方法同时解决这些问题。JBL用了一个铜和钢的合金薄环加在音圈隙的外径! 在细讲这个方法之前,先解释一个现象---局部磁通调制。 永磁场里的总的力量的变动称为总磁通调制,这可以由一个大的短路环来控制。但是局部力量变动是发生的音圈隙里的,它是独立于总磁通调制的。这种特别的现象通常是发生在沉浮式的设计中,特别是在象1500AL这样有特别深的隙。由音圈引起的交流场会引发力量在音圈隙的顶部到底部发生如跷跷板式的变化。如果在这个隙里加入一个铜短路环能解决这个问题.

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:43 | 显示全部楼层
但是如果在一系列的铜短路环之间加入钢环,这样就可以分离掉那个在中频造成2db的衰减的涡流

1

主题

63

回帖

4336

积分

金牌会员

积分
4336

专家勋章版主勋章

发表于 2010-5-8 10:44 | 显示全部楼层
由于现有的数字音源动态很大,就需要喇叭要有很大的冲程,就需要大音圈,但由于是采用沉浮式的设计,磁隙的深度要相当深,一个0.8“长的音圈就需要1.5”深的磁隙,从而要求磁铁的力量相当大。在1500AL的ALNICO磁块重五磅,整只喇叭重约30磅! 长冲程需要特殊的支称系统,通常,悬边和弹波会同时提供给振动盆回复力和制动力。但在长冲程的情况下,悬边和弹波的不同结构回造对偏移非对称的反应从而引起失真。为解决这一问题,JBL设计了镜像对称的双弹波结构。
您需要登录后才可以回帖 登录 | 注册

本版积分规则

超薄音响 稀客领航
请用微信扫一扫,关注音响设计网创始人直播

QQ|手机版|Archiver|XYCAD中国音响设计网 ( 京ICP备14030947号 )点击这里与XYCAD官方实时沟通

GMT+8, 2024-12-23 07:02 , Processed in 0.112085 second(s), 23 queries , Gzip On.

Powered by Discuz! X3.5 Licensed

© 2001-2024 Discuz! Team.

快速回复 返回顶部 返回列表