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The composition of two translations is simply another translation.
Suppose that the point has position vector . We can let be any point we wish.
Let the translation be defined by the vector ; that is, it shifts every point by that vector . Similarly, let the translation be defined by the vector .
Let us denote and . Thus, we have .
Since the point is shifted by the vector , the position vector of is .
Since the point is shifted by the vector , the position vector of is .
This means that we have shifted the point by the vector . Since the point was an arbitrary choice, the same holds for all points. Thus, the composition is another translation defined by the vector .
Notice that we could have applied the transformation first, and then afterward; since vector addition is commutative, this would have given us the same result. Thus, when you have a composition of translations, one may apply the translations in any order you want.