Electric flux through a closed surface and Gauss’s Law
PHXII01:ELECTRIC CHARGES AND FIELDS

358286 The electric flux linked with the closed surface in \(N m^{2} C^{-1}\) is \(\left(\epsilon_{0}=8.85 \times 10^{-12} C^{2} N^{-1} m^{-2}\right)\)
supporting img

1 \(10^{10}\)
2 \(8.85 \times 10^{-13}\)
3 \(10^{12}\)
4 \(10^{11}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358287 An infinitely long line of charge having a uniform charge per unit length \(\lambda \) lies at a distance \(x\) from a point \(O\) as shown in the figure. Determine the total electric flux through the surface of a sphere of radius \(R\). \((x < R)\)
supporting img

1 \(\frac{{2\lambda R}}{{{\varepsilon _o}}}\)
2 \(\frac{{\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
3 \(\frac{{2\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
4 \(\frac{{\lambda R}}{{{\varepsilon _o}}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358288 What is the electric flux linked with closed surface?
supporting img

1 \({10^{12}}N{m^2}{C^{ - 1}}\)
2 \({10^{11}}N{m^2}{C^{ - 1}}\)
3 \(8.86 \times {10^{13}}N{m^2}{C^{ - 1}}\)
4 \({10^{10}}N{m^2}{C^{ - 1}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358289 The electric field in a region is
\(E = \frac{{5 \times {{10}^3}(N{C^{ - 1}}c{m^{ - 1}})x}}{2}\widehat i\)
The charge contained inside a cubical volume bounded by the surfaces
\(x = 0,x = 2,y = 0,y = 2,z = 0,z = 2\) is (where \(x\),\(y\),\(z\) are in \(cm\))

1 \(1.76 \times {10^{ - 11}}C\)
2 \(3.52 \times {10^{ - 11}}C\)
3 \(2.21 \times {10^{ - 8}}C\)
4 \(2 \times {10^{ - 10}}C\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358290 Consider an infinite line of charge having uniform linear charge density and passing through the axis of a cylinder. What will be the effect on the flux passing through the curved surface if the portions of the line charge outside the cylinder is removed.
supporting img

1 Decreases
2 Increases
3 Remains same
4 Cannot say
PHXII01:ELECTRIC CHARGES AND FIELDS

358286 The electric flux linked with the closed surface in \(N m^{2} C^{-1}\) is \(\left(\epsilon_{0}=8.85 \times 10^{-12} C^{2} N^{-1} m^{-2}\right)\)
supporting img

1 \(10^{10}\)
2 \(8.85 \times 10^{-13}\)
3 \(10^{12}\)
4 \(10^{11}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358287 An infinitely long line of charge having a uniform charge per unit length \(\lambda \) lies at a distance \(x\) from a point \(O\) as shown in the figure. Determine the total electric flux through the surface of a sphere of radius \(R\). \((x < R)\)
supporting img

1 \(\frac{{2\lambda R}}{{{\varepsilon _o}}}\)
2 \(\frac{{\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
3 \(\frac{{2\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
4 \(\frac{{\lambda R}}{{{\varepsilon _o}}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358288 What is the electric flux linked with closed surface?
supporting img

1 \({10^{12}}N{m^2}{C^{ - 1}}\)
2 \({10^{11}}N{m^2}{C^{ - 1}}\)
3 \(8.86 \times {10^{13}}N{m^2}{C^{ - 1}}\)
4 \({10^{10}}N{m^2}{C^{ - 1}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358289 The electric field in a region is
\(E = \frac{{5 \times {{10}^3}(N{C^{ - 1}}c{m^{ - 1}})x}}{2}\widehat i\)
The charge contained inside a cubical volume bounded by the surfaces
\(x = 0,x = 2,y = 0,y = 2,z = 0,z = 2\) is (where \(x\),\(y\),\(z\) are in \(cm\))

1 \(1.76 \times {10^{ - 11}}C\)
2 \(3.52 \times {10^{ - 11}}C\)
3 \(2.21 \times {10^{ - 8}}C\)
4 \(2 \times {10^{ - 10}}C\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358290 Consider an infinite line of charge having uniform linear charge density and passing through the axis of a cylinder. What will be the effect on the flux passing through the curved surface if the portions of the line charge outside the cylinder is removed.
supporting img

1 Decreases
2 Increases
3 Remains same
4 Cannot say
PHXII01:ELECTRIC CHARGES AND FIELDS

358286 The electric flux linked with the closed surface in \(N m^{2} C^{-1}\) is \(\left(\epsilon_{0}=8.85 \times 10^{-12} C^{2} N^{-1} m^{-2}\right)\)
supporting img

1 \(10^{10}\)
2 \(8.85 \times 10^{-13}\)
3 \(10^{12}\)
4 \(10^{11}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358287 An infinitely long line of charge having a uniform charge per unit length \(\lambda \) lies at a distance \(x\) from a point \(O\) as shown in the figure. Determine the total electric flux through the surface of a sphere of radius \(R\). \((x < R)\)
supporting img

1 \(\frac{{2\lambda R}}{{{\varepsilon _o}}}\)
2 \(\frac{{\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
3 \(\frac{{2\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
4 \(\frac{{\lambda R}}{{{\varepsilon _o}}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358288 What is the electric flux linked with closed surface?
supporting img

1 \({10^{12}}N{m^2}{C^{ - 1}}\)
2 \({10^{11}}N{m^2}{C^{ - 1}}\)
3 \(8.86 \times {10^{13}}N{m^2}{C^{ - 1}}\)
4 \({10^{10}}N{m^2}{C^{ - 1}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358289 The electric field in a region is
\(E = \frac{{5 \times {{10}^3}(N{C^{ - 1}}c{m^{ - 1}})x}}{2}\widehat i\)
The charge contained inside a cubical volume bounded by the surfaces
\(x = 0,x = 2,y = 0,y = 2,z = 0,z = 2\) is (where \(x\),\(y\),\(z\) are in \(cm\))

1 \(1.76 \times {10^{ - 11}}C\)
2 \(3.52 \times {10^{ - 11}}C\)
3 \(2.21 \times {10^{ - 8}}C\)
4 \(2 \times {10^{ - 10}}C\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358290 Consider an infinite line of charge having uniform linear charge density and passing through the axis of a cylinder. What will be the effect on the flux passing through the curved surface if the portions of the line charge outside the cylinder is removed.
supporting img

1 Decreases
2 Increases
3 Remains same
4 Cannot say
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PHXII01:ELECTRIC CHARGES AND FIELDS

358286 The electric flux linked with the closed surface in \(N m^{2} C^{-1}\) is \(\left(\epsilon_{0}=8.85 \times 10^{-12} C^{2} N^{-1} m^{-2}\right)\)
supporting img

1 \(10^{10}\)
2 \(8.85 \times 10^{-13}\)
3 \(10^{12}\)
4 \(10^{11}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358287 An infinitely long line of charge having a uniform charge per unit length \(\lambda \) lies at a distance \(x\) from a point \(O\) as shown in the figure. Determine the total electric flux through the surface of a sphere of radius \(R\). \((x < R)\)
supporting img

1 \(\frac{{2\lambda R}}{{{\varepsilon _o}}}\)
2 \(\frac{{\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
3 \(\frac{{2\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
4 \(\frac{{\lambda R}}{{{\varepsilon _o}}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358288 What is the electric flux linked with closed surface?
supporting img

1 \({10^{12}}N{m^2}{C^{ - 1}}\)
2 \({10^{11}}N{m^2}{C^{ - 1}}\)
3 \(8.86 \times {10^{13}}N{m^2}{C^{ - 1}}\)
4 \({10^{10}}N{m^2}{C^{ - 1}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358289 The electric field in a region is
\(E = \frac{{5 \times {{10}^3}(N{C^{ - 1}}c{m^{ - 1}})x}}{2}\widehat i\)
The charge contained inside a cubical volume bounded by the surfaces
\(x = 0,x = 2,y = 0,y = 2,z = 0,z = 2\) is (where \(x\),\(y\),\(z\) are in \(cm\))

1 \(1.76 \times {10^{ - 11}}C\)
2 \(3.52 \times {10^{ - 11}}C\)
3 \(2.21 \times {10^{ - 8}}C\)
4 \(2 \times {10^{ - 10}}C\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358290 Consider an infinite line of charge having uniform linear charge density and passing through the axis of a cylinder. What will be the effect on the flux passing through the curved surface if the portions of the line charge outside the cylinder is removed.
supporting img

1 Decreases
2 Increases
3 Remains same
4 Cannot say
PHXII01:ELECTRIC CHARGES AND FIELDS

358286 The electric flux linked with the closed surface in \(N m^{2} C^{-1}\) is \(\left(\epsilon_{0}=8.85 \times 10^{-12} C^{2} N^{-1} m^{-2}\right)\)
supporting img

1 \(10^{10}\)
2 \(8.85 \times 10^{-13}\)
3 \(10^{12}\)
4 \(10^{11}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358287 An infinitely long line of charge having a uniform charge per unit length \(\lambda \) lies at a distance \(x\) from a point \(O\) as shown in the figure. Determine the total electric flux through the surface of a sphere of radius \(R\). \((x < R)\)
supporting img

1 \(\frac{{2\lambda R}}{{{\varepsilon _o}}}\)
2 \(\frac{{\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
3 \(\frac{{2\lambda \sqrt {{R^2} - {x^2}} }}{{{\varepsilon _o}}}\)
4 \(\frac{{\lambda R}}{{{\varepsilon _o}}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358288 What is the electric flux linked with closed surface?
supporting img

1 \({10^{12}}N{m^2}{C^{ - 1}}\)
2 \({10^{11}}N{m^2}{C^{ - 1}}\)
3 \(8.86 \times {10^{13}}N{m^2}{C^{ - 1}}\)
4 \({10^{10}}N{m^2}{C^{ - 1}}\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358289 The electric field in a region is
\(E = \frac{{5 \times {{10}^3}(N{C^{ - 1}}c{m^{ - 1}})x}}{2}\widehat i\)
The charge contained inside a cubical volume bounded by the surfaces
\(x = 0,x = 2,y = 0,y = 2,z = 0,z = 2\) is (where \(x\),\(y\),\(z\) are in \(cm\))

1 \(1.76 \times {10^{ - 11}}C\)
2 \(3.52 \times {10^{ - 11}}C\)
3 \(2.21 \times {10^{ - 8}}C\)
4 \(2 \times {10^{ - 10}}C\)
PHXII01:ELECTRIC CHARGES AND FIELDS

358290 Consider an infinite line of charge having uniform linear charge density and passing through the axis of a cylinder. What will be the effect on the flux passing through the curved surface if the portions of the line charge outside the cylinder is removed.
supporting img

1 Decreases
2 Increases
3 Remains same
4 Cannot say