Skip to content
회로도전자부품
2014.01.11 08:06

종이 스피커

조회 수 14735 추천 수 0 댓글 0
?

단축키

Prev이전 문서

Next다음 문서

크게 작게 위로 아래로 댓글로 가기 인쇄
?

단축키

Prev이전 문서

Next다음 문서

크게 작게 위로 아래로 댓글로 가기 인쇄

종이 스피커

Paper Speaker 또는 Foil Speaker 로 불리는 스피커 실험 동영상.

 

얇은 종이에 구리호일(은박지도 될까? ^^)

 

한번 만들어보고 싶네.

 

 

 

 

 

 참고 : http://web.media.mit.edu/~plusea/?p=265

 

 

 

 

Flat spiral coil inductor calculator

Formula used in this calculation is based on the Harold A. Wheeler approximations.

L (uH) = r^2 * A^2 / (30*A -11 *Di)
A= (Di+N*(w+s))/2

...where:

Di =inner diameter in inches.
s =distance between windings in inches.
w =wire diameter in inches.
N = number of turns.
Do =outer diameter.
1 inch = 0,0254m=2,54cm = 25,4mm.

This formula applies at 'low' frequencies (<30MHz) ) using enameled copper wire. Some people call it "magnet wire".

Flat spiral coil
image
Flat spiral inductor
Coil inner diameter (Di):
Number of turns (N):
Wire Diameter (w):
Spacing between turns (s):
Inductance (L):
Outer diameter (Dout):
Wire lenght (Wl):
image

More about flat spiral air core inductors
A flat spiral coil is a type of an air core inductor usually incorporated in the primary of a tesla generator, RFID tag, and proximity detectors. In the same category as the flat spiral coils we have planar spiral coils, planar square spiral coils, planar rectangular spiral coils, planar hexagonal spiral coils and octagonal spiral coil. Planar coils are mostly used in high frequency applications and designed as tracks on a circuit board. Take a look at our planar coil calculator here.

What is an air core inductor?
An "air core inductor" is an inductor that does not depend upon a ferromagnetic material to achieve its specified inductance. Some inductors are wound without a bobbin and just air as the core. Some others are wound on a bobbin made of bakelite, platsic, ceramic etc.


Advantages of an air core coil:
Its inductance is unaffected by the current it carries.
This contrasts with the situation with coils using ferromagnetic cores whose inductance tends to reach a peak at moderate field strengths before dropping towards zero as saturation approaches. Sometimes non-linearity in the magnetization curve can be tolerated; for example in switching power supplies and in some switching topologies this is an advantage.
In circuits such as audio cross over filters in hi-fi speaker systems you must avoid distortion; then an air coil is a good choice. Most radio transmitters rely on air coils to prevent the production of harmonics.
Air coils are also free of the "iron losses" which a problem with ferromagnetic cores. As frequency is increased this advantage becomes progressively more important. You obtain better Q-factor, greater efficiency, greater power handling, and less distortion.
Lastly, air coils can be designed to perform at frequencies as high as 1 Ghz. Most ferromagnetic cores tend to be rather lossy above 100 MHz.

And the "downside":
Without a high permeability core you must have more and/or larger turns to achieve a given inductance value. More turns means larger coils, lower self-resonance dur to higher interwinding capacitance and higher copper loss. At higher frequencies you generally don't need high inductance, so this is then less of a problem.
Greater stray field radiation and pickup:
With the closed magnetic paths used in cored inductors radiation is much less serious. As the diameter increases towards a wavelength (lambda = c / f), loss due to electromagnetic radiation will become significant. You may be able to reduce this problem by enclosing the coil in a screen, or by mounting it at right angles to other coils it may be coupling with.
You may be using an air cored coil not because you require a circuit element with a specific inductance per se but because your coil is used as a proximity sensor, loop antenna, induction heater, Tesla coil, electromagnet, magnetometer head or deflection yoke etc. Then an external radiated field may be what you want.

 

로그인 후 댓글쓰기가 가능합니다.

?

List of Articles
번호 분류 제목 날짜 조회 수
153 회로도전자부품 AM FM one transistor am transmitter & Reciver 1 2014.03.04 8962
152 회로도전자부품 KSP13 TRANSISTOR를 이용한 1석 오디오 회로 file 2014.03.04 6318
151 회로도전자부품 One transistor capacitance multiplier(발진기,바이브레이터) 2014.02.17 15960
150 회로도전자부품 Simplest Ever DC-DC Boost 12v to 73v(IC 없이 승압회로) file 2014.02.13 9142
149 회로도전자부품 Pspice 따라하기 file 2014.02.12 11895
148 회로도전자부품 트랜지스터 file 2014.02.11 12319
147 회로도전자부품 CDS회로(LED 켜기) file 2014.02.10 8201
146 회로도전자부품 2석 오디오(트랜지스터 오디오) file 2014.02.07 9829
145 회로도전자부품 지식채널ⓔ 못 배운 과학자 마이클 페러데이 2014.02.07 6613
144 회로도전자부품 평활회로 2014.02.06 8821
143 회로도전자부품 갤럭시S 배터리 개조. file 2014.02.05 8273
142 회로도전자부품 Voltage Detector 2014.02.04 7054
141 회로도전자부품 삼성 DVD-writer 16X 분해(레이저 다이오드, 볼록렌즈, 네오디뮴, 각종모터) file 2014.01.30 7588
140 회로도전자부품 버추얼 브레드보드 프로그램(시뮬레이션 가능) file 2014.01.29 8395
139 회로도전자부품 [재미있는 과학실험] 연필을 이용한 검전기 만들기 2014.01.23 5691
138 회로도전자부품 DC to DC Boost(The Voltage Doubler) file 2014.01.22 5789
137 회로도전자부품 No IC & DC to DC converter 2014.01.22 5963
136 회로도전자부품 다이오드(Diode) 2014.01.22 6230
135 회로도전자부품 RC 회로 2014.01.22 5860
134 회로도전자부품 저항(resistor) 2014.01.22 5782
Board Pagination Prev 1 ... 4 5 6 7 8 ... 13 Next
/ 13

http://urin79.com

우린친구블로그

sketchbook5, 스케치북5

sketchbook5, 스케치북5

나눔글꼴 설치 안내


이 PC에는 나눔글꼴이 설치되어 있지 않습니다.

이 사이트를 나눔글꼴로 보기 위해서는
나눔글꼴을 설치해야 합니다.

설치 취소