Newton's third law of motion gives meaning to the first two laws by restricting what type of fundamental forces act between particles. This restriction gives meaning to the "force" described in the first two laws.
Taken by themselves (by which I mean without any reference to any explicit form for the fundamental forces acting between particles), the third law is what gives the first two laws any predictive power. This is what Mr. Kleppner is referring to when he says that Newton's third law is "an important logical element in making sense of the first two laws."
For example, suppose you are watching two balls float in outer space; ball A and ball B. You see ball A accelerate towards ball B. Using Newton's first law you know there is a force acting on ball A from ball B. Using Newton's second law you know that the force is along a vector connecting the two balls. Finally, using Newton's third law you can predict that ball B should also be accelerating towards ball A. And you can test that prediction. So, the third law is what gives the first two laws any predictive power.
I would argue that instead of Newton's third law it is the explicit form of the fundamental forces which "really" give the first two laws their meaning. In this case, Newton's third law of motion is just a restriction on what form those fundamental forces can take.
To illustrate this idea, suppose we want to use Newton's laws to do some science.
Newton's first law states:
A body in motion will stay in motion unless acted upon by an external
force.
Since we don't know what a force is yet, it could be anything and this statement can be rephrased as:
A body in motion will stay in motion unless it doesn't.
You can see why this is not useful.
Newton's second law of motion states:
The acceleration of a body is parallel and proportional to the force exerted on the body and inversely proportional to the mass of the body.
Again, without a definition of force, this statement is useless.
Now, suppose we have a definition for a force, such as gravity.
$F_{gravity} = G \frac{m_{1} m_{2}}{r^2}$
Now, the first two laws have meaning. We can use our definition of force to predict the motion of a particle due to the gravitational attraction of some other body and then go out and test it!
Newton's third law of motion states:
Any force exerted by body A on body B implies an equal and opposite force on body B by body A.
Given a description of all the fundamental forces acting between particles, we don't need Newton's third law. Instead, Newton's third law is telling us how these forces act, namely symmetric with respect to both particles. You can see this reflected in the mathematical formula for the force of gravity; switching $m_1$ and $m_2$ you get the same force.