Solution

1. Speed of a transverse wave on a string

It is known that the propagation speed $v$ of transverse waves along a stretched string depends on its tension force $F$ and linear density $\mu$ (mass per unit length) according to the formula:
$$v = \sqrt{\frac{F}{\mu}}$$

2. Condition for the formation of a standing wave

Since the guitar string is rigidly fixed at both ends, nodes of the standing wave must form at these ends. At the first harmonic (fundamental tone), exactly one antinode, which is half a wavelength $\lambda$, fits along the entire length of the string $l$:
$$l = \frac{\lambda}{2} \implies \lambda = 2l$$

3. Relationship between frequency, wavelength, and speed

By definition, the wave propagation speed is related to its wavelength and frequency by the formula:
$$v = \lambda \nu$$
Substituting the expression for the wavelength here, we obtain the wave speed at the first harmonic:
$$v = 2l\nu$$

4. Derivation of the final formula

Let's equate the two expressions for the wave speed:
$$2l\nu = \sqrt{\frac{F}{\mu}}$$
From here, we express the required tension force $F$. Squaring both sides of the equation:
$$4l^2\nu^2 = \frac{F}{\mu}$$
$$F = 4\mu l^2\nu^2$$

5. Calculation

Let's convert all values to the SI system:

$l = 60 \text{ cm} = 0.6 \text{ m}$

$\mu = 0.1 \text{ g/cm} = \frac{0.1 \cdot 10^{-3} \text{ kg}}{10^{-2} \text{ m}} = 0.01 \text{ kg/m}$

$\nu = 100 \text{ Hz}$

Substituting the values into our formula:
$$F = 4 \cdot 0.01 \cdot (0.6)^2 \cdot 100^2 = 4 \cdot 0.01 \cdot 0.36 \cdot 10000 = 144 \text{ N}$$