If a spherical conductor partially enters a closed surface as shown in the figure,then the total electric flux emitted from the closed surface will be:
- A$\frac{1}{\varepsilon_0} \times (\text{charge enclosed by surface})$
- B$\varepsilon_0 \times (\text{charge enclosed by surface})$
- C$\frac{1}{4\pi\varepsilon_0} \times (\text{charge enclosed by surface})$
- D$0$
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