The Wave Equation

The wave equation for a plane wave traveling in the x direction is

where v is the phase velocity of the wave and y represents the variable which is changing as the wave passes. This is the form of the wave equation which applies to a stretched string or a plane electromagnetic wave. The mathematical description of a wave makes use of partial derivatives.

In two dimensions, the wave equation takes the form

which could describe a wave on a stretched membrane.

Waves in Ideal String

The wave equation for a wave in an ideal string can be obtained by applying Newton's 2nd Law to an infinitesmal segment of a string.

If a constant horizontal tension T is maintained in the string, then 如果在弦中保持恒定的水平拉力 T，那么 Newton's 2nd law becomes 牛顿第二定律变为 Combination of these two expressions for small angles gives 将这两个表达式结合在一起，对于小角度来说得到 Show details 显示详细信息 Solutions to wave equation 波动方程的解

String Wave Equation Development

Analysis of the forces on a segment of stretched string gives two relationships: 分析拉伸弦上一段的力得到两个关系式：

Combining gives and relating this to the slopes at the segment ends gives 并将其与段端的斜率联系起来 In the limit Δx→ 0 this becomes 在 Δx→0 的极限情况下，这变为 Wave equation 波动方程 组合得到

Ideal String Constraints

In order for the wave equation to apply to the waves in a string, it must meet certain constraints. For an ideal string, it is assumed that

1. The string is perfectly uniform with a constant mass per unit length, and is perfectly elastic with no resistance to bending.

2. The string tension is presumed to be large enough so that gravity can be neglected.

3. Small segments of the string are presumed to move transversely in a plane perpendicular to the string, and that the displacements and slopes of segments of the string are small.

Though stringent, these idealizations permit the development of a wave equation which describes well the vibrations of thin real strings.