Cell
PHXII03:CURRENT ELECTRICITY

356914 The terminal voltage of the battery, whose emf is \(10\,V\) and internal resistance \({1 \Omega}\), when connected through an external resistance of \({4 \Omega}\) as shown in the figure is:
supporting img

1 \({4 V}\)
2 \({6 V}\)
3 \({8 V}\)
4 \({10 V}\)
PHXII03:CURRENT ELECTRICITY

356915 The direction of current inside a cell is

1 \(( - )ve\) pole to \(( + )ve\) pole during discharging
2 \(( + )ve\) pole to \(( - )ve\) pole during discharging
3 Always \(( - )ve\) pole to \(( + )ve\) pole
4 Always flows from \(( + )ve\) pole to \(( - )ve\) pole
PHXII03:CURRENT ELECTRICITY

356916 A cell of emf 4 \(V\) and internal resistance \({0.2 \Omega}\) is connected with the resistance of \({1.8 \Omega}\). The voltage across the cell terminal will be

1 6.3 \(V\)
2 2.4 \(V\)
3 3.8 \(V\)
4 3.6 \(V\)
PHXII03:CURRENT ELECTRICITY

356917 Two cells of emf \({E_1}\,{\rm{and}}\,{E_2}\) are joined in opposition (such that \({E_1}\, > {E_2}\)). If \({r_1}\,{\rm{and}}\,{r_2}\) be the internal resistance and \(R\) be the external resistance, then the terminal potential difference is
supporting img

1 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
2 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
3 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2}}} \times R\)
4 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2}}} \times R\)
PHXII03:CURRENT ELECTRICITY

356914 The terminal voltage of the battery, whose emf is \(10\,V\) and internal resistance \({1 \Omega}\), when connected through an external resistance of \({4 \Omega}\) as shown in the figure is:
supporting img

1 \({4 V}\)
2 \({6 V}\)
3 \({8 V}\)
4 \({10 V}\)
PHXII03:CURRENT ELECTRICITY

356915 The direction of current inside a cell is

1 \(( - )ve\) pole to \(( + )ve\) pole during discharging
2 \(( + )ve\) pole to \(( - )ve\) pole during discharging
3 Always \(( - )ve\) pole to \(( + )ve\) pole
4 Always flows from \(( + )ve\) pole to \(( - )ve\) pole
PHXII03:CURRENT ELECTRICITY

356916 A cell of emf 4 \(V\) and internal resistance \({0.2 \Omega}\) is connected with the resistance of \({1.8 \Omega}\). The voltage across the cell terminal will be

1 6.3 \(V\)
2 2.4 \(V\)
3 3.8 \(V\)
4 3.6 \(V\)
PHXII03:CURRENT ELECTRICITY

356917 Two cells of emf \({E_1}\,{\rm{and}}\,{E_2}\) are joined in opposition (such that \({E_1}\, > {E_2}\)). If \({r_1}\,{\rm{and}}\,{r_2}\) be the internal resistance and \(R\) be the external resistance, then the terminal potential difference is
supporting img

1 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
2 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
3 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2}}} \times R\)
4 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2}}} \times R\)
PHXII03:CURRENT ELECTRICITY

356914 The terminal voltage of the battery, whose emf is \(10\,V\) and internal resistance \({1 \Omega}\), when connected through an external resistance of \({4 \Omega}\) as shown in the figure is:
supporting img

1 \({4 V}\)
2 \({6 V}\)
3 \({8 V}\)
4 \({10 V}\)
PHXII03:CURRENT ELECTRICITY

356915 The direction of current inside a cell is

1 \(( - )ve\) pole to \(( + )ve\) pole during discharging
2 \(( + )ve\) pole to \(( - )ve\) pole during discharging
3 Always \(( - )ve\) pole to \(( + )ve\) pole
4 Always flows from \(( + )ve\) pole to \(( - )ve\) pole
PHXII03:CURRENT ELECTRICITY

356916 A cell of emf 4 \(V\) and internal resistance \({0.2 \Omega}\) is connected with the resistance of \({1.8 \Omega}\). The voltage across the cell terminal will be

1 6.3 \(V\)
2 2.4 \(V\)
3 3.8 \(V\)
4 3.6 \(V\)
PHXII03:CURRENT ELECTRICITY

356917 Two cells of emf \({E_1}\,{\rm{and}}\,{E_2}\) are joined in opposition (such that \({E_1}\, > {E_2}\)). If \({r_1}\,{\rm{and}}\,{r_2}\) be the internal resistance and \(R\) be the external resistance, then the terminal potential difference is
supporting img

1 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
2 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
3 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2}}} \times R\)
4 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2}}} \times R\)
PHXII03:CURRENT ELECTRICITY

356914 The terminal voltage of the battery, whose emf is \(10\,V\) and internal resistance \({1 \Omega}\), when connected through an external resistance of \({4 \Omega}\) as shown in the figure is:
supporting img

1 \({4 V}\)
2 \({6 V}\)
3 \({8 V}\)
4 \({10 V}\)
PHXII03:CURRENT ELECTRICITY

356915 The direction of current inside a cell is

1 \(( - )ve\) pole to \(( + )ve\) pole during discharging
2 \(( + )ve\) pole to \(( - )ve\) pole during discharging
3 Always \(( - )ve\) pole to \(( + )ve\) pole
4 Always flows from \(( + )ve\) pole to \(( - )ve\) pole
PHXII03:CURRENT ELECTRICITY

356916 A cell of emf 4 \(V\) and internal resistance \({0.2 \Omega}\) is connected with the resistance of \({1.8 \Omega}\). The voltage across the cell terminal will be

1 6.3 \(V\)
2 2.4 \(V\)
3 3.8 \(V\)
4 3.6 \(V\)
PHXII03:CURRENT ELECTRICITY

356917 Two cells of emf \({E_1}\,{\rm{and}}\,{E_2}\) are joined in opposition (such that \({E_1}\, > {E_2}\)). If \({r_1}\,{\rm{and}}\,{r_2}\) be the internal resistance and \(R\) be the external resistance, then the terminal potential difference is
supporting img

1 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
2 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2} + R}} \times R\)
3 \(\frac{{{E_1} + {E_2}}}{{{r_1} + {r_2}}} \times R\)
4 \(\frac{{{E_1} - {E_2}}}{{{r_1} + {r_2}}} \times R\)