Newton's 3rd law - Whenever an object exerts a force on another object, the other object exerts an equal an opposite force on the initial object. In some cases, the opposing force is a reaction force due to acceleration of the other object.
Bernoulli - In the ideal case where there is no work done on a gas or fluid, the total energy remains constant, and if there is a "work free" transition that causes a change in kinetic energy, then an equal an opposite transition occurs in the pressure energy. (Temperature energy is also a component of total energy, but it's ignored in the "classic" Bernoulli case).
Newton's 3rd law and lift - Wings produce lift by appying a downwards force to the air, which which responds with an equal and opposite lift force. Since the air is free to move, the result of the force applied to the air is a downwards acceleration of the air, and it's the reactive response to this acceleration that results in the reactive lift force from the air.
Bernoulli and lift - If a wing were 100% efficient, no work would be required, and all of the increase in kinetic energy of the air would correspond to an equal and opposite decrease in pressure energy.
Wings are not 100% efficient. When a wing passes through a volume of air, the result is a downwards and slightly forwards acceleration of air. The forwards component corresponds to drag. Newtons 3rd law still applies in this case, the only difference is the direction and magnitude of the force; the wing applies a downwards and somewhat forwards force on the air, and the air reacts with an equal and opposing upwards and somewhat backwards force. The Bernoulli relationship is impacted by efficiency; the increase in kinetic energy of the air is more than the decrease in pressure energy, and this work related component is a "non-Bernoulli" aspect of a wings interaction of the air. In addition, there is some change in air temperature, especially at higher air speeds, which also affects Bernoulli, but not Newton's 3rd law.
Wings work via a combination of forward speed and effective angle of attack (zero effective angle of attack means zero lift), which is how a wing applies a downwards (and forwards) force to the air. As mentioned before, the bottom of a wing accelerates air downwards through mechanical interaction, and above a wing, "Coanda like" effects (friction, viscosity, void effects), cause the air to tend to follow the upper surface of a wing, which also accelerates air downwards.
Getting back to your original post, the lift on a wing can be approximated by integrating the sum of pressures across the chord of the wing, using the speed at each point near the surface of a wing to calculate pressures via the Bernoulli relationship. However this process needs to be modified to compensate for work done on the air ("non-Bernoulli" like transitions in pressure, kinetic, and temperature energy), and take into account that the air stream is somewhat detached from the surface of a wing (there's a shear boundary layer than transitions from zero relative speed to the speed of the air). Except for about the leading 1/3rd of the wing chord, the flow is turbulent, small horizontal eddies, so an effective "average" speed has to be used to account for these eddies (or the turbulent flow is ignored and treated as "semi-laminar"). Although this approach might be good for approximating lift mathematically, it's not a good method for explaining lift, since lift is a reaction force to downwards acceleration of a very large volume of air per unit of time, not just the air streams near the surface of a wing.