A mass 􀝉􀬵 􀵌 1 􀝇􀝃 is attached to a spring with a spring constant 􀝇􀬵 􀵌 5 􀯇

􀯠, which is
attached to a solid mounting. A second mass 􀝉􀬶 􀵌 1 􀝇􀝃 is attached to a spring with
spring constant 􀝇􀬶 􀵌 6 􀯇
􀯠, which is attached to the bottom of 􀝉􀬵. Initially, 􀝉􀬵 is at rest
and in equilibrium, while 􀝉􀬶 is at rest 1 􀝉 below its equilibrium position.

To find the frequency of oscillation for the two masses, we can use the formula:

f = 1 / (2π) * √(k / m)

Where:
f is the frequency of oscillation
k is the spring constant
m is the mass

For the first mass, we have:
k₁ = 5 N/m and m₁ = 1 kg
f₁ = 1 / (2π) * √(5 N/m / 1 kg)

For the second mass, we have:
k₂ = 6 N/m and m₂ = 1 kg
f₂ = 1 / (2π) * √(6 N/m / 1 kg)

To find the equilibrium position for the second mass, we can use Hooke's Law:

F = -k * x

Where:
F is the force applied by the spring
k is the spring constant
x is the displacement from the equilibrium

For the second mass, the force due to the spring is balanced by the gravitational force acting on it. The gravitational force is given by:

F = m * g

Where:
m is the mass
g is the acceleration due to gravity

Setting these two forces equal to each other, we have:

-k₂ * x = m₂ * g

Solving for x, we get:

x = -m₂ * g / k₂

Substituting the values, we have:
x = -(1 kg * 9.8 m/s²) / 6 N/m

Therefore, the equilibrium position for the second mass is 1.63 m below its initial position.

Please note that this is a simplified explanation and assumes ideal conditions. In real-world scenarios, there may be other factors to consider.