Well, we know that:
$$\underline{\text{V}}_{\space\text{C}}=\frac{1}{\text{j}\omega\text{C}}\cdot\frac{\hat{\text{u}}\exp\left(\theta\text{j}\right)}{\text{R}_1+\frac{1}{\text{j}\omega\text{C}}}\tag1$$
Assuming that the \$1\space\text{V}\$ is the amplitude of the voltage-source, we get:
$$\underline{\text{V}}_{\space\text{C}}=\frac{1}{\text{j}\cdot4\cdot750\cdot10^{-3}}\cdot\frac{1\exp\left(0\text{j}\right)}{1+\frac{1}{\text{j}\cdot4\cdot750\cdot10^{-3}}}\tag2$$
So, the function in the time domain will be:
$$\text{V}_\text{C}\left(t\right)=\left|\underline{\text{V}}_{\space\text{C}}\right|\sin\left(\omega t+\arg\left(\underline{\text{V}}_{\space\text{C}}\right)\right)\tag3$$
And you will find:
$$\left|\underline{\text{V}}_{\space\text{C}}\right|=\frac{1}{\sqrt{10}}\approx0.316228\space\text{V}\space\space\space\wedge\space\space\space\arg\left(\underline{\text{V}}_{\space\text{C}}\right)=-\arctan(3)\approx-1.24905\space\text{rad}\tag4$$