Answers

 

1. 

EP(S)=5p;

EP(H)=2p+2(1-p)=2;

= 5p2+2(1-p)=5p2+2-2p.

Hence,

D(p)=p(-5p2+7p-2).

So, the fixed points are p=0, p=1, p=2/5, which is globally stable.  As soon as any small variation around 0 or 1 occurs, the system will evolve towards p=2/5.  The graph is not to scale and rough. 

 

2.

We could do the same as in (1).  However, let us follow a different procedure that will make life easier.  First, we rewrite the matrix, listing only the payoffs for the row player:

 

 

A

B

A

3

1

B

4

0

 

What we have now is a matrix such that the replicator dynamics does not change if we add a constant to any column. (We shall not prove this but be thankful to the mathematician who did!).  This allows us to obtain a matrix in which the bottom row is all zeros, which will simplify calculations; all we need to do is to add -4 to the first column, as the bottom of the second column is already zero.  So, we obtain:

 

A

B

A

-1

1

B

0

0

 

Now,

EP(A)= -p+1-p=1-2p;

EP(B)=0

= -2p2+p

Hence,

D(p)=p(2p2-3p+1).

The fixed points are p=0, p=1/2, p=1. 

 

Since for p=1/3, the rate of change is positive and for p=2/3 it is negative, p=1/2 is globally stable.  The graph is not to scale and rough.

 

3.  After simplifying the matrix as per exercise 9, we have:

 

S

C

S

-5

10

C

0

0

 

Hence, if Pr(S)=p, we obtain:

EP(S)= -5p+10 (1-p) = -15p + 10;

EP(C)=0;

= -15p2+10p.

Hence,

D(p)=p(15p2 -25p +10).

The fixed points are p=0, p=2/3, p=1.    The graph is:

 

p=2/3 is globally stable; the system will end up with 2/3 of the players swerving. 

 

4.

The game is dominance solvable, the equilibrium being (H,H).  Since no strongly dominated strategy survives replicator dynamics, only H will remain.  So, Pr(H)=1 is globally stable and H will become fixated.

We can verify this the long way.  First, let’s simplify the matrix, thus obtaining

 

 

A

B

A

-2

-1

B

0

0

 

Then, if Pr(A)=p,

EP(A)= -2p-1(1-p)=-1-p

EP(B)=0

= p(-1-p) = -p-p2

Hence,

D(p)=p(-1-p+p+ p2)=p(p+1)(p-1).

The solutions are p=0, p=1, and p= -1.  However, no probability is negative and consequently p = -1 must be disregarded.  The only question left is whether D(p) is positive or negative between 0 and 1.  By substituting, say p=1/2, we see that it’s negative.  So, the graph looks, more or less, like this:

 

Consequently, 0 is globally stable; at the end, A will disappear and B will become fixated, as we discovered above.

 

 

5.

After simplification, we obtain

 

 

A

B

A

1

-2

B

0

0

 

Setting Pr(A)=p,

EP(A)= 3p -2

EP(B)=0

=  3p2 -2p

Hence,

D(p)= p(- 3p2 +5p– 2) = .

The solutions are p=0, p=1, and p=2/3.  By substituting, say, 1/2 for p, we note that the D(p) is negative between 0 and 2/3.  The graph is (more or less)

 

 

So, 2/3, the interior point, is unstable; A or B will eventually go to fixation.

 

6.

a. For ρA > 1/N to obtain, in replicator dynamics the interior point p* must be less than 1/3.  Hence, 

p*= (d-b)/(a-c+d-b)<1/3, that is,

3(d-b)< a-c+d-b, or

2(d-b)<a-c.

b. For ρA > ρB to obtain, it must be that p*<1/2.  Proceeding as before, we get d-b<a-c.

 

7.

p*=1/2, and therefore the relation does not obtain.  The fixation probabilities of S and H are the same.