It is always directed back toward the equilibrium position of the system.

Now consider Fig. 15 which illustrates a full employment equilibrium position.

As a result, it accelerates and starts going back to the equilibrium position.

Therefore, the mass continues past the equilibrium position, compressing the spring.

Where is the angle measured from the inverted equilibrium position.

In a perfect economy, any market should be able to move to the equilibrium position instantly without travelling along the curve.

The system oscillates about the equilibrium position under the influence of loads.

Therefore, oscillating material does not move far from its initial equilibrium position.

But where will the electrons find their equilibrium positions?

It will again overshoot its equilibrium position and continue downward some distance.

Plucking the string moves it away from this equilibrium position.

When the Arm is hanging down in the stable equilibrium position .

When the mass moves closer to the equilibrium position, the restoring force decreases.

Seesaws also work as a simple example of a mechanical system with two equilibrium positions.

The neo-classical analysis can be justified only if the new equilibrium positions are reached quickly.

Once put into motion the block will oscillate back and forth around the equilibrium position.

Once the mass is displaced from its equilibrium position, it experiences a net restoring force.

On each bounce, the system is "trying" to return to its equilibrium position, but overshoots it.

The economies' previous equilibrium positions differ from this new position in at least two major aspects.

Eventually, when the supply of labour catches up with the demand for it, the economy breaks into a new equilibrium position.

The upper graph shows the economy's initial general equilibrium position in the real and monetary sectors.

The error in ignoring higher order terms remains small if remains close to the equilibrium position.

Consider a fluid particle that is displaced upwards, say, from its equilibrium position.

This produces a righting moment which returns the toy to the equilibrium position.

Its unstable equilibrium position is obtained by rotating the figure 180 about a horizontal axis.