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The composition of two translations is simply another translation.

Suppose that the point PP has position vector p⃗\vec{p}. We can let PP be any point we wish.

Let the translation T1T_1 be defined by the vector u⃗\vec{u}; that is, it shifts every point by that vector u⃗\vec{u}. Similarly, let the translation T2T_2 be defined by the vector v⃗\vec{v}.

Let us denote Q=T1(P)Q=T_1(P) and R=T2(Q)R=T_2(Q). Thus, we have R=T2∘T1(P)R=T_2\circ T_1(P).

Since the point PP is shifted by the vector u⃗\vec{u}, the position vector of QQ is p⃗+u⃗\vec{p}+\vec{u}.

Since the point QQ is shifted by the vector v⃗\vec{v}, the position vector of RR is p⃗+u⃗+v⃗=p⃗+(u⃗+v⃗)\vec{p}+\vec{u}+\vec{v}=\vec{p}+(\vec{u}+\vec{v}).

This means that we have shifted the point PP by the vector u⃗+v⃗\vec{u}+\vec{v}. Since the point PP was an arbitrary choice, the same holds for all points. Thus, the composition T2∘T1T_2\circ T_1 is another translation defined by the vector u⃗+v⃗\vec{u}+\vec{v}.

Notice that we could have applied the transformation T2T_2 first, and then T1T_1 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.

Type a concept, like “slope” or “photosynthesis”.

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