Whenever cos(theta) = 1,
we get sin(theta) = +-sqrt(1-cos^2theta) = 0
and cos(theta)-sin(theta) = 1 - 0 = 1.
cos(theta) = 1 for theta = 2npi for all n in ZZ.
Whenever sin(theta) = -1,
we get cos(theta) = +-sqrt(1-sin^2theta) = 0
and cos(theta)-sin(theta) = 0 - (-1) = 1.
sin(theta) = -1 for theta = -pi/2+2npi for all n in ZZ.
Putting two cases together, we have solutions when:
theta = 2npi for all n in ZZ
and when
theta = -pi/2 + 2npi for all n in ZZ
To make sure that these are the only solutions:
Starting with cos(theta)-sin(theta)=1, first add sin(theta) to both sides:
cos(theta)=sin(theta)+1
Then square both sides:
cos^2(theta)=sin^2(theta)+2sin(theta)+1
Then use cos^2(theta)=1-sin^2(theta) to get:
1-sin^2(theta)=sin^2(theta)+2sin(theta)+1
Add sin^2(theta)-1 to both sides to get:
0=2sin^2(theta)+2sin(theta)=2sin(theta)(sin(theta)+1)
So either sin(theta) = 0 or sin(theta) = -1
We have already accounted for sin(theta) = -1 in our solutions.
What about sin(theta) = 0?
If this is so, then
cos^2(theta) = 1 - sin^2(theta) = 1 - 0 = 1
So cos(theta) = +-sqrt(1) = +-1
Only the case cos(theta) = 1 satisfies cos(theta)-sin(theta) = 1 and we have accounted for that case already too.
So we have found all the solutions.