Consider an elemental segment in the string as shown in the Figure (a).
(a) Transverse waves in a stretched string.
(b) Elemental segment in a stretched string is zoomed and the pulse seen from an observer frame who moves with velocity v.
Let A and B be two points on the string at an instant of time. Let dl and dm be the length and mass of the elemental string, respectively. By definition, linear mass density, `mu` is
`mu=(dm)/(dl) " "...(1)`
`dm=mu dl" "...(2)`
The elemental string AB has a curvature which looks like an arc of a circle with centre at O, radius R and the arc subtending an angle `theta` at the origin O as shown in Figure (b). The angle `theta` can be written in terms of arc lengh and radius as `theta=(dl)/(R)`. The centripetal acceleration supplied by the tension in the string is
`a_(cp)=(v^(2))/(R)" "...(3)`
Then, centripetal force can be obtained when mass of the string (dm) is included in equation (3)
`F_(cp)=((dm)v^(2))/(R)" " ...(4)`
The centripetal force experienced by elemental string can be calculated by substituting equation (2) in equation (4) we get
`((dm)v^(2))/(R)=(mu v^(2).dl)/(R)" "...(5)`
The tension T acts along the tangent of the elemental segment of the string at A and B. Since the arc length is very small, variation in the tension force can be ignored. T is resolved into horizontal component
`T cos ((theta)/(2))` and vertical component `T sin((theta)/(2))`.
The horizontal components at A and B are equal in magnitude but opposite in direction, therefore, they cancel each other. Since the elemental arc length AB is taken to be very small, the vertical components at A and B apears to acts vertical towards the centre of the arc and hence, they add up. the net radial force `F_(r)` is
`F_(r)=2T sin((theta)/(2))" " ....(6)`
Since the amplitude of the wave is very small when it is compared with the length of the string, the sine of small angle is approximated as `sin((theta)/(2))~~(theta)/(2)`. Hence equation (6) can be written as
`F_(r)=2Txx(theta)/(2)=T theta" "...(7)`
But `theta=(dl)/(R)`, therefore substituting in equation (7), we get
`F_(r)=T(dl)/(R)" " ...(8)`
Applying Newton's second law to the elemental string in the radial direction, under equilibrium, the radial component of the force is equal to the centripetal force. Hence equating equation (5) and equation (8), we have
`T(dl)/(R)=mu v^(2)(dl)/(R)`
`v=sqrt((T)/(mu))" measured in ms"^(-1)" "...(9) `
