I believe Action potential is the brief wave of positive charge that sweeps down the axon. Axon is part of the neuron that conducts impulses from the dendrites towards the cell body along the neuron. The action potential is brief since the sodium channels can only stay open for a very brief amount of time. As it travels along the neuron there is a change in polarity across the membrane of the axon .
        
             
        
        
        
Answer:
The final charges of each sphere are:   q_A = 3/8 Q
, q_B = 3/8 Q
,               q_C = 3/4 Q
Explanation:
This problem asks for the final charge of each sphere, for this we must use that the charge is distributed evenly over a metal surface.
 Let's start Sphere A makes contact with sphere B, whereby each one ends with half of the initial charge, at this point
                 q_A = Q / 2
                 q_B = Q / 2
Now sphere A touches sphere C, ending with half the charge
                 q_A = ½ (Q / 2) = ¼ Q
                 q_B = ¼ Q
Now the sphere A that has Q / 4 of the initial charge is put in contact with the sphere B that has Q / 2 of the initial charge, the total charge is the sum of the charge
                   q = Q / 4 + Q / 2 = ¾ Q
This is the charge distributed between the two spheres, sphere A is 3/8 Q and sphere B is 3/8 Q
                   q_A = 3/8 Q
                   q_B = 3/8 Q
The final charges of each sphere are:
                 q_A = 3/8 Q
                 q_B = 3/8 Q
                 q_C = 3/4 Q
 
        
             
        
        
        
Answer:
  I_weight = M L²
 this value is much larger and with it it is easier to restore balance.I
Explanation:
When man walks a tightrope, he carries a linear velocity, this velocity is related to the angular velocity by
             v = w r
For man to maintain equilibrium needs the total moment to be zero
              ∑τ = I α
               S  τ = 0
 The forces on the home are the weight of the masses, the weight of the man and the support on the rope, the latter two are zero taque the distance to the center of rotation is zero.
 Therefore the moment of the masses and the open is the one that must be zero.
If the man carries only the bar, we could approximate it by two open one on each side of the axis of rotation formed by the free of the rope
               I = ⅓ m L² / 4
As the length of half the length of the bar and the mass of the bar is small, this moment is small, therefore at the moment if there is some imbalance it is difficult to recover.
If, in addition to the opening, each of them carries a specific weight, the moment of inertia of this weight is
              I_weight = M L²
 this value is much larger and with it it is easier to restore balance.