Let <TEX>$X_k(x)=({\int}^T_o{\alpha}_1(s)dx(s),...,{\int}^T_o{\alpha}_k(s)dx(s))\;and\;X_{\tau}(x)=(x(t_1),...,x(t_k))$</TEX> on the classical Wiener space, where <TEX>${{\alpha}_1,...,{\alpha}_k}$</TEX> is an orthonormal subset of <TEX>$L_2$</TEX> [0, T] and <TEX>${\tau}:0<t_1<...<t_k=T$</TEX> is a partition of [0, T]. In this paper, we establish a change of scale formula for conditional Wiener integrals <TEX>$E[G_{\gamma}|X_k]$</TEX> of functions on classical Wiener space having the form <TEX>$$G_{\gamma}(x)=F(x){\Psi}({\int}^T_ov_1(s)dx(s),...,{\int}^T_o\;v_{\gamma}(s)dx(s))$$</TEX>, for <TEX>$F{\in}S\;and\;{\Psi}={\psi}+{\phi}({\psi}{\in}L_p(\mathbb{R}^{\gamma}),\;{\phi}{\in}\hat{M}(\mathbb{R}^{\gamma}))$</TEX>, which need not be bounded or continuous. Here S is a Banach algebra on classical Wiener space and <TEX>$\hat{M}(\mathbb{R}^{\gamma})$</TEX> is the space of Fourier transforms of measures of bounded variation over <TEX>$\mathbb{R}^{\gamma}$</TEX>. As results of the formula, we derive a change of scale formula for the conditional Wiener integrals <TEX>$E[G_{\gamma}|X_{\tau}]\;and\;E[F|X_{\tau}]$</TEX>. Finally, we show that the analytic Feynman integral of F can be expressed as a limit of a change of scale transformation of the conditional Wiener integral of F using an inversion formula which changes the conditional Wiener integral of F to an ordinary Wiener integral of F, and then we obtain another type of change of scale formula for Wiener integrals of F.