Let f be in the localized nonisotropic Sobolev space \( W^{{1,p}}_{{{\text{loc}}}} {\left( {\mathbb{H}^{n} } \right)} \) on the n-dimensional Heisenberg group ℍn = ℂn × ℝ, where 1 = p < Q and Q = 2n + 2 is the homogeneous dimension of ℍn. Suppose that the subelliptic gradient is gloablly Lp integrable, i.e., \( {\int_{\mathbb{H}^{n} } {{\left| {\nabla _{{\mathbb{H}^{n} }} f} \right|}} }^{p} du \) is finite. We prove a Poincare inequality for f on the entire space ℍn. Using this inequality we prove that the function f subtracting a certain constant is in the nonisotropic Sobolev space formed by the completion of \( C^{\infty }_{0} {\left( {\mathbb{H}^{n} } \right)} \) under the norm of $$ {\left( {{\int_{\mathbb{H}^{n} } {{\left| f \right|}} }^{{\frac{{Qp}} {{Q - p}}}} } \right)}^{{\frac{{Q - p}} {{Qp}}}} + {\left( {{\int_{\mathbb{H}^{n} } {{\left| {\nabla _{{\mathbb{H}^{n} }} f} \right|}} }^{p} } \right)}^{{\frac{1} {p}}} . $$ We will also prove that the best constants and extremals for such Poincare inequalities on ℍn are the same as those for Sobolev inequalities on ℍn. Using the results of Jerison and Lee on the sharp constant and extremals for L2 to \( L\frac{{2Q}} {{Q - 2}} \) Sobolev inequality on the Heisenberg group, we thus arrive at the explicit best constant for the aforementioned Poincare inequality on ℍn when p = 2. We also derive the lower bound of the best constants for local Poincare inequalities over metric balls on the Heisenberg group ℍn.