267873
Two electric charges of \(+10^{-9} \mathrm{C}\) and \(-10^{-9} \mathrm{C}\) are placed at the corners \(A\) and \(B\) of an equilateral triangle \(A B C\) side \(5 \mathrm{~cm}\). Theelectric intensity at \(C\) is
267899
' \(n\) ' charges \(Q, 4 Q, 9 Q, 16 Q \ldots\).... are placed at distances of \(1,2,3 \ldots\). . metre from a point ' 0 ' on the same straight line. The electric intensity at ' 0 ' is
267896
In the figureshown, the electric field intensity at \(r=1 m, r=6 m, r=9 m\) in \(\mathrm{Vm}^{-1}\) is
1 \(-5,-1.67,+5\)
2 \(-5,0,+5\)
3 \(0,1.67,0\)
4 \(+5,1.67,-5\)
Explanation:
\(E=-\frac{d V}{d r}\)
Electric Charges and Fields
267897
Point charges of \(3 \times 10^{-9} \mathrm{C}\) are situated at each of three corners of a square whose side is \(15 \mathrm{~cm}\). The magnitude and direction of electric field at the vacant corner of the square is
267898
A large flat metal surface has uniform charge density \(+\sigma\). An electron of mass m and charge e leaves the surface at an angle at point \(A\) with speed \(v\), and return to it at point \(B\). The maximum value of \(A B\) is \(\qquad\)
1 \(\frac{m m \epsilon_{0}}{\sigma e}\)
2 \(\frac{v^{2} m \epsilon_{0}}{\Theta \sigma}\)
3 \(\frac{v^{2} e}{\epsilon_{0} \sigma m}\)
4 \(\frac{v^{2} \sigma e}{\epsilon_{0} m}\)
Explanation:
Field near metal surface \(E=\frac{\sigma}{\epsilon_{0}}\)
Forceondectron \(=\notin=\frac{\ominus \sigma}{\epsilon_{0}}\)
Acceleration of electron \(\mathrm{a}=\frac{\ominus \sigma}{m \epsilon_{0}}\)
It will act as projectile with max range \(=\frac{u^{2}}{a}=\frac{u^{2}}{\Theta \sigma} \times m \in_{0}\)
267873
Two electric charges of \(+10^{-9} \mathrm{C}\) and \(-10^{-9} \mathrm{C}\) are placed at the corners \(A\) and \(B\) of an equilateral triangle \(A B C\) side \(5 \mathrm{~cm}\). Theelectric intensity at \(C\) is
267899
' \(n\) ' charges \(Q, 4 Q, 9 Q, 16 Q \ldots\).... are placed at distances of \(1,2,3 \ldots\). . metre from a point ' 0 ' on the same straight line. The electric intensity at ' 0 ' is
267896
In the figureshown, the electric field intensity at \(r=1 m, r=6 m, r=9 m\) in \(\mathrm{Vm}^{-1}\) is
1 \(-5,-1.67,+5\)
2 \(-5,0,+5\)
3 \(0,1.67,0\)
4 \(+5,1.67,-5\)
Explanation:
\(E=-\frac{d V}{d r}\)
Electric Charges and Fields
267897
Point charges of \(3 \times 10^{-9} \mathrm{C}\) are situated at each of three corners of a square whose side is \(15 \mathrm{~cm}\). The magnitude and direction of electric field at the vacant corner of the square is
267898
A large flat metal surface has uniform charge density \(+\sigma\). An electron of mass m and charge e leaves the surface at an angle at point \(A\) with speed \(v\), and return to it at point \(B\). The maximum value of \(A B\) is \(\qquad\)
1 \(\frac{m m \epsilon_{0}}{\sigma e}\)
2 \(\frac{v^{2} m \epsilon_{0}}{\Theta \sigma}\)
3 \(\frac{v^{2} e}{\epsilon_{0} \sigma m}\)
4 \(\frac{v^{2} \sigma e}{\epsilon_{0} m}\)
Explanation:
Field near metal surface \(E=\frac{\sigma}{\epsilon_{0}}\)
Forceondectron \(=\notin=\frac{\ominus \sigma}{\epsilon_{0}}\)
Acceleration of electron \(\mathrm{a}=\frac{\ominus \sigma}{m \epsilon_{0}}\)
It will act as projectile with max range \(=\frac{u^{2}}{a}=\frac{u^{2}}{\Theta \sigma} \times m \in_{0}\)
267873
Two electric charges of \(+10^{-9} \mathrm{C}\) and \(-10^{-9} \mathrm{C}\) are placed at the corners \(A\) and \(B\) of an equilateral triangle \(A B C\) side \(5 \mathrm{~cm}\). Theelectric intensity at \(C\) is
267899
' \(n\) ' charges \(Q, 4 Q, 9 Q, 16 Q \ldots\).... are placed at distances of \(1,2,3 \ldots\). . metre from a point ' 0 ' on the same straight line. The electric intensity at ' 0 ' is
267896
In the figureshown, the electric field intensity at \(r=1 m, r=6 m, r=9 m\) in \(\mathrm{Vm}^{-1}\) is
1 \(-5,-1.67,+5\)
2 \(-5,0,+5\)
3 \(0,1.67,0\)
4 \(+5,1.67,-5\)
Explanation:
\(E=-\frac{d V}{d r}\)
Electric Charges and Fields
267897
Point charges of \(3 \times 10^{-9} \mathrm{C}\) are situated at each of three corners of a square whose side is \(15 \mathrm{~cm}\). The magnitude and direction of electric field at the vacant corner of the square is
267898
A large flat metal surface has uniform charge density \(+\sigma\). An electron of mass m and charge e leaves the surface at an angle at point \(A\) with speed \(v\), and return to it at point \(B\). The maximum value of \(A B\) is \(\qquad\)
1 \(\frac{m m \epsilon_{0}}{\sigma e}\)
2 \(\frac{v^{2} m \epsilon_{0}}{\Theta \sigma}\)
3 \(\frac{v^{2} e}{\epsilon_{0} \sigma m}\)
4 \(\frac{v^{2} \sigma e}{\epsilon_{0} m}\)
Explanation:
Field near metal surface \(E=\frac{\sigma}{\epsilon_{0}}\)
Forceondectron \(=\notin=\frac{\ominus \sigma}{\epsilon_{0}}\)
Acceleration of electron \(\mathrm{a}=\frac{\ominus \sigma}{m \epsilon_{0}}\)
It will act as projectile with max range \(=\frac{u^{2}}{a}=\frac{u^{2}}{\Theta \sigma} \times m \in_{0}\)
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Electric Charges and Fields
267873
Two electric charges of \(+10^{-9} \mathrm{C}\) and \(-10^{-9} \mathrm{C}\) are placed at the corners \(A\) and \(B\) of an equilateral triangle \(A B C\) side \(5 \mathrm{~cm}\). Theelectric intensity at \(C\) is
267899
' \(n\) ' charges \(Q, 4 Q, 9 Q, 16 Q \ldots\).... are placed at distances of \(1,2,3 \ldots\). . metre from a point ' 0 ' on the same straight line. The electric intensity at ' 0 ' is
267896
In the figureshown, the electric field intensity at \(r=1 m, r=6 m, r=9 m\) in \(\mathrm{Vm}^{-1}\) is
1 \(-5,-1.67,+5\)
2 \(-5,0,+5\)
3 \(0,1.67,0\)
4 \(+5,1.67,-5\)
Explanation:
\(E=-\frac{d V}{d r}\)
Electric Charges and Fields
267897
Point charges of \(3 \times 10^{-9} \mathrm{C}\) are situated at each of three corners of a square whose side is \(15 \mathrm{~cm}\). The magnitude and direction of electric field at the vacant corner of the square is
267898
A large flat metal surface has uniform charge density \(+\sigma\). An electron of mass m and charge e leaves the surface at an angle at point \(A\) with speed \(v\), and return to it at point \(B\). The maximum value of \(A B\) is \(\qquad\)
1 \(\frac{m m \epsilon_{0}}{\sigma e}\)
2 \(\frac{v^{2} m \epsilon_{0}}{\Theta \sigma}\)
3 \(\frac{v^{2} e}{\epsilon_{0} \sigma m}\)
4 \(\frac{v^{2} \sigma e}{\epsilon_{0} m}\)
Explanation:
Field near metal surface \(E=\frac{\sigma}{\epsilon_{0}}\)
Forceondectron \(=\notin=\frac{\ominus \sigma}{\epsilon_{0}}\)
Acceleration of electron \(\mathrm{a}=\frac{\ominus \sigma}{m \epsilon_{0}}\)
It will act as projectile with max range \(=\frac{u^{2}}{a}=\frac{u^{2}}{\Theta \sigma} \times m \in_{0}\)
267873
Two electric charges of \(+10^{-9} \mathrm{C}\) and \(-10^{-9} \mathrm{C}\) are placed at the corners \(A\) and \(B\) of an equilateral triangle \(A B C\) side \(5 \mathrm{~cm}\). Theelectric intensity at \(C\) is
267899
' \(n\) ' charges \(Q, 4 Q, 9 Q, 16 Q \ldots\).... are placed at distances of \(1,2,3 \ldots\). . metre from a point ' 0 ' on the same straight line. The electric intensity at ' 0 ' is
267896
In the figureshown, the electric field intensity at \(r=1 m, r=6 m, r=9 m\) in \(\mathrm{Vm}^{-1}\) is
1 \(-5,-1.67,+5\)
2 \(-5,0,+5\)
3 \(0,1.67,0\)
4 \(+5,1.67,-5\)
Explanation:
\(E=-\frac{d V}{d r}\)
Electric Charges and Fields
267897
Point charges of \(3 \times 10^{-9} \mathrm{C}\) are situated at each of three corners of a square whose side is \(15 \mathrm{~cm}\). The magnitude and direction of electric field at the vacant corner of the square is
267898
A large flat metal surface has uniform charge density \(+\sigma\). An electron of mass m and charge e leaves the surface at an angle at point \(A\) with speed \(v\), and return to it at point \(B\). The maximum value of \(A B\) is \(\qquad\)
1 \(\frac{m m \epsilon_{0}}{\sigma e}\)
2 \(\frac{v^{2} m \epsilon_{0}}{\Theta \sigma}\)
3 \(\frac{v^{2} e}{\epsilon_{0} \sigma m}\)
4 \(\frac{v^{2} \sigma e}{\epsilon_{0} m}\)
Explanation:
Field near metal surface \(E=\frac{\sigma}{\epsilon_{0}}\)
Forceondectron \(=\notin=\frac{\ominus \sigma}{\epsilon_{0}}\)
Acceleration of electron \(\mathrm{a}=\frac{\ominus \sigma}{m \epsilon_{0}}\)
It will act as projectile with max range \(=\frac{u^{2}}{a}=\frac{u^{2}}{\Theta \sigma} \times m \in_{0}\)