The correct option is A 1 : 2
The string on a musical instrument is (almost) fixed at both ends, so any vibration of the string must have nodes at each end. For instance the string with length L could have a standing wave with wavelength twice as long as the string (wavelength λ=2L) as shown in the first sketch in the next series. This gives a node at either end and an antinode in the middle.
Let's work out the relationships among the frequencies of these modes. For a wave, the frequency is the ratio of the speed of the wave to the length of the wave: f=vλ. Compared to the string length L, you can see that these waves have lengths 2L, L, 2L/3, L/2. We could write this as 2L/n, where n is the number of the harmonic.
The fundamental or first mode has frequency f1 = vλ1= v/2L,
The second harmonic has frequency f2 = vλ2 = 2v/2L = 2f1,
The third harmonic has frequency f3 = vλ3 = 3v/2L = 3f1,
The fourth harmonic has frequency f4 = vλ4 = 4v/2L = 4f1, and, to generalise,
The nth harmonic has frequency fn = vλn = nv/2L = nf1.
All waves in a string travel with the same speed, so these waves with different wavelengths have different frequencies as given in the diagrams. The mode with the lowest frequency (f1) is called the fundamental or the principle note. The nth mode has frequency n times that of the fundamental. All of the modes (and the sounds they produce) are called the harmonics of the string. The frequencies f, 2f, 3f, 4f etc are called the harmonic series.
Hence, the frequency ratio of the different modes given in the diagram are in the ratio 1:2:3:4........:n.