- 53 Views
- Uploaded on
- Presentation posted in: General

Model 2: Strings on the violin and guitar.

Model 2: Strings on the violin and guitar

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

The motion of vibrating structures such as the guitar or violin string commonly consists of a linear combination of motion of individual modes. We have sketched the first 3 transverse modes of the bias spring. Each mode has an associated shape and natural frequency. For instance, when we draw back a string on a guitar and release it we hear the fundamental tone of the string along with several overtones. If we know the initial shape of the string and its initial velocity it is possible to describe the subsequent total vibration after its release by summing the contribution from each mode.

2003/ 1

A musical string can be modelled as an elastic string. We will use the same equation:

(5)

The 1 dimensional wave equation

This has also already been done. We use equation 8:

(8)

L

The boundary conditions are the same as before for the spring:

At x=0 u(0,t) = 0

Thus B= 0

At x=Lu(L,t) = 0

So sin(L) = 0

L = nπwhere n= 1,2,3,….

u3(x,t)

u2(x,t)

u1(x,t)

(9)

n= 1,2,3,….

and the rest.

(9)

n= 1,2,3,….

The resultant motion on the string is the sum of modes described by eqn. 9:

(10)

L/2

X=0

X=L

0

1

At t=0 u(x,0) only contains terms multiplied by bn:

(11)

(10)

Differentiate wrt t

t=0

(12)

(11)

Initial displacement

Initial velocity

(12)

We can use a property of the sine function:

if n=m

if n ≠ m(13)

The trick is to multiply both sides of equations 11 and 12 by sin (mπx) and then integrate between the limits 0 and L. All terms are equal to zero except those where n =m.

We can do this to eqn. 11:

(14)

Rearrange to find the value of the m’th term:

(15)

(12)

(16)

L/2

0.5L

X=0

X=L

Initial conditions:

for x=0 to L/2 (17)

for x=L/2 to L (18)

for x=0 to L (19)

0

(16)

The velocity is zero at t=0 and we can see from eqn. 16 that all an = 0 too.

Plucked string at t=0 (left) and the first 3 non-zero modes that sum to produce the total motion.

String capture

Release

Capture

String capture

Release

The rocking action forces the body to vibrate and sound is radiated.

Consider the E and A strings:

Fundamental of A is tuned to 440 Hz

E string fundamental is around but not exactly 660Hz.

Beat frequency between fundamentals would be approximately 660-440= 220 Hz. Yet we hear beating of the order of a 1 to 10 Hz as we adjust the E string. This beat frequency reduces to zero as we improve the tuning.