Let \(D_{1}\) and \(D_{2}\) be two compact, convex polyhedra in the oriented \(k\)-dimensional space \(R^{k}\) and \(f: D_{1} \rightarrow D_{2}\) a differentiable map which is an orientation-preserving diffeomorphism \({ }^{55}\) of the interior of \(D_{1}\) onto the interior of \(D_{2}\). Then, for any differential \(k\)-form \(\omega^{k}\) on \(D_{2}\). $$ \int_{D_{1}} f^{*} \omega^{k}=\int_{D_{2}} \omega^{k} $$

Short Answer

Expert verified
Question: Prove that for two compact, convex polyhedra \(D_1\) and \(D_2\) in \(k\)-dimensional space and an orientation-preserving diffeomorphism \(f:D_1 \rightarrow D_2\), the integral of the pullback by \(f\) of a differential \(k\)-form \(\omega^k\) on \(D_2\) equals the integral of \(\omega^k\) on \(D_2\). That is, \(\int_{D_1} f^*\omega^k = \int_{D_2} \omega^k\). Answer: The proof relies on understanding the pullback of a differential form by a differentiable map, and utilizing the change of variables formula for integration along with the fact that the diffeomorphism \(f\) preserves orientation. By substituting the relationship between volume forms, we find that \(\int_{D_1} f^*\omega^k = \int_{D_2} \omega^k\), thus proving the desired equality.

Step by step solution

01

Recall the definition of pullback

The pullback \(f^* \omega^k\) of a differential form \(\omega^k\) by a differentiable map \(f\) is a new differential form that "pulls back" the structure of \(\omega^k\) along \(f\). It is defined by the following formula: $$ (f^* \omega^k)_p(v_1, \dots, v_k) = \omega^k_{f(p)}(f_* v_1, \dots, f_* v_k) $$ for all points \(p\) in \(D_1\) and tangent vectors \(v_1, \dots, v_k\) at \(p\). Here, \(f_* v_i\) denotes the pushforward of \(v_i\) by \(f\), which is a tangent vector at \(f(p)\).
02

Use properties of orientation-preserving diffeomorphisms

Since \(f\) is an orientation-preserving diffeomorphism, its Jacobian determinant at every point of \(D_1\) is positive. Let \(J_f(p)\) denote the Jacobian determinant of \(f\) at the point \(p\). Then, due to the change of variables formula for integration, we have: $$ \int_{D_1} f^*\omega^k = \int_{D_1} \omega^k_{f(p)}(f_* v_1, \dots, f_* v_k) \; \text{dvol}_{D_1} $$ where \(\text{dvol}_{D_1}\) is the volume form on \(D_1\). Now, since \(f\) is an orientation preserving diffeomorphism, the volume form is transformed as follows: $$ \text{dvol}_{D_1} = J_f(p) \, \text{dvol}_{D_2} \circ f $$
03

Substitute the relationship between volume forms

Now, we substitute this relationship into the previous equation: $$ \int_{D_1} f^*\omega^k = \int_{D_1} \omega^k_{f(p)}(f_* v_1, \dots, f_* v_k) \; J_f(p) \, \text{dvol}_{D_2} \circ f $$ Use the substitution \(q = f(p)\), which is valid since \(f\) is a diffeomorphism. Then, we have $$ \int_{D_1} f^*\omega^k = \int_{D_2} \omega^k_q(v_1, \dots, v_k) \; \text{dvol}_{D_2} $$ This is precisely the desired equality: $$ \int_{D_1} f^* \omega^k = \int_{D_2} \omega^k $$ This completes the proof.

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