03. ELECTRIC FIELD
Electric Charges and Fields

272155 Two point charges $+Q$ and $+q$ are separated by a certain distance. If $+Q>+q$ then in between the charges the electric field is zero at a point

1 closer to $+Q$
2 closer to $+q$
3 exactly at the mid-point of line segment joining $+Q$ and $+q$.
4 no where on the line segment joining $+Q$ and $+q$.
Electric Charges and Fields

272156 If an electron has an initial velocity in a direction different from that of an electric field, the path of the electron is

1 a straight line
2 a circle
3 an ellipse
4 aparabolà
Electric Charges and Fields

272157 In the figure, charge $q$ is placed at origin $\rho $. When the charge $q$ is displaced from its position the electric field at point $P$ changes

1 at the same time when $q$ is displaced.
2 at a time after $\frac{OP}{c}$ where $c$ is the speed of light.
3 at a time after $\frac{OPcos\theta }{c}$
4 at a time after $\frac{OPsin\theta }{c}$
Electric Charges and Fields

272158 The electric field intensity just sufficient to balance the earth's gravitational attraction on an electron will be: (given mass, charge of an electron respectively are $9.1\times {{10}^{-31}}~kg$ and $1.6\times {{10}^{-19}}C$.)

1 $-5.6\times {{10}^{-11}}~N/C$
2 $-1.6\times {{10}^{-19}}~N/C$
3 $-4.8\times {{10}^{-15}}~N/C$
4 $-3.2\times {{10}^{-19}}~N/C$
Electric Charges and Fields

272159 $ABC$ is an equilateral triangle. Charges $+q$ are placed at each corner as shown in fig. The electric intensity at centre $O$ will be

1 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{r}$.
2 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{{{r}^{2}}}$
3 $\frac{1}{4\pi {{\epsilon }_{o}}}\frac{3q}{{{r}^{2}}}$
4 zero
Electric Charges and Fields

272155 Two point charges $+Q$ and $+q$ are separated by a certain distance. If $+Q>+q$ then in between the charges the electric field is zero at a point

1 closer to $+Q$
2 closer to $+q$
3 exactly at the mid-point of line segment joining $+Q$ and $+q$.
4 no where on the line segment joining $+Q$ and $+q$.
Electric Charges and Fields

272156 If an electron has an initial velocity in a direction different from that of an electric field, the path of the electron is

1 a straight line
2 a circle
3 an ellipse
4 aparabolà
Electric Charges and Fields

272157 In the figure, charge $q$ is placed at origin $\rho $. When the charge $q$ is displaced from its position the electric field at point $P$ changes

1 at the same time when $q$ is displaced.
2 at a time after $\frac{OP}{c}$ where $c$ is the speed of light.
3 at a time after $\frac{OPcos\theta }{c}$
4 at a time after $\frac{OPsin\theta }{c}$
Electric Charges and Fields

272158 The electric field intensity just sufficient to balance the earth's gravitational attraction on an electron will be: (given mass, charge of an electron respectively are $9.1\times {{10}^{-31}}~kg$ and $1.6\times {{10}^{-19}}C$.)

1 $-5.6\times {{10}^{-11}}~N/C$
2 $-1.6\times {{10}^{-19}}~N/C$
3 $-4.8\times {{10}^{-15}}~N/C$
4 $-3.2\times {{10}^{-19}}~N/C$
Electric Charges and Fields

272159 $ABC$ is an equilateral triangle. Charges $+q$ are placed at each corner as shown in fig. The electric intensity at centre $O$ will be

1 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{r}$.
2 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{{{r}^{2}}}$
3 $\frac{1}{4\pi {{\epsilon }_{o}}}\frac{3q}{{{r}^{2}}}$
4 zero
Electric Charges and Fields

272155 Two point charges $+Q$ and $+q$ are separated by a certain distance. If $+Q>+q$ then in between the charges the electric field is zero at a point

1 closer to $+Q$
2 closer to $+q$
3 exactly at the mid-point of line segment joining $+Q$ and $+q$.
4 no where on the line segment joining $+Q$ and $+q$.
Electric Charges and Fields

272156 If an electron has an initial velocity in a direction different from that of an electric field, the path of the electron is

1 a straight line
2 a circle
3 an ellipse
4 aparabolà
Electric Charges and Fields

272157 In the figure, charge $q$ is placed at origin $\rho $. When the charge $q$ is displaced from its position the electric field at point $P$ changes

1 at the same time when $q$ is displaced.
2 at a time after $\frac{OP}{c}$ where $c$ is the speed of light.
3 at a time after $\frac{OPcos\theta }{c}$
4 at a time after $\frac{OPsin\theta }{c}$
Electric Charges and Fields

272158 The electric field intensity just sufficient to balance the earth's gravitational attraction on an electron will be: (given mass, charge of an electron respectively are $9.1\times {{10}^{-31}}~kg$ and $1.6\times {{10}^{-19}}C$.)

1 $-5.6\times {{10}^{-11}}~N/C$
2 $-1.6\times {{10}^{-19}}~N/C$
3 $-4.8\times {{10}^{-15}}~N/C$
4 $-3.2\times {{10}^{-19}}~N/C$
Electric Charges and Fields

272159 $ABC$ is an equilateral triangle. Charges $+q$ are placed at each corner as shown in fig. The electric intensity at centre $O$ will be

1 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{r}$.
2 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{{{r}^{2}}}$
3 $\frac{1}{4\pi {{\epsilon }_{o}}}\frac{3q}{{{r}^{2}}}$
4 zero
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
Electric Charges and Fields

272155 Two point charges $+Q$ and $+q$ are separated by a certain distance. If $+Q>+q$ then in between the charges the electric field is zero at a point

1 closer to $+Q$
2 closer to $+q$
3 exactly at the mid-point of line segment joining $+Q$ and $+q$.
4 no where on the line segment joining $+Q$ and $+q$.
Electric Charges and Fields

272156 If an electron has an initial velocity in a direction different from that of an electric field, the path of the electron is

1 a straight line
2 a circle
3 an ellipse
4 aparabolà
Electric Charges and Fields

272157 In the figure, charge $q$ is placed at origin $\rho $. When the charge $q$ is displaced from its position the electric field at point $P$ changes

1 at the same time when $q$ is displaced.
2 at a time after $\frac{OP}{c}$ where $c$ is the speed of light.
3 at a time after $\frac{OPcos\theta }{c}$
4 at a time after $\frac{OPsin\theta }{c}$
Electric Charges and Fields

272158 The electric field intensity just sufficient to balance the earth's gravitational attraction on an electron will be: (given mass, charge of an electron respectively are $9.1\times {{10}^{-31}}~kg$ and $1.6\times {{10}^{-19}}C$.)

1 $-5.6\times {{10}^{-11}}~N/C$
2 $-1.6\times {{10}^{-19}}~N/C$
3 $-4.8\times {{10}^{-15}}~N/C$
4 $-3.2\times {{10}^{-19}}~N/C$
Electric Charges and Fields

272159 $ABC$ is an equilateral triangle. Charges $+q$ are placed at each corner as shown in fig. The electric intensity at centre $O$ will be

1 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{r}$.
2 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{{{r}^{2}}}$
3 $\frac{1}{4\pi {{\epsilon }_{o}}}\frac{3q}{{{r}^{2}}}$
4 zero
Electric Charges and Fields

272155 Two point charges $+Q$ and $+q$ are separated by a certain distance. If $+Q>+q$ then in between the charges the electric field is zero at a point

1 closer to $+Q$
2 closer to $+q$
3 exactly at the mid-point of line segment joining $+Q$ and $+q$.
4 no where on the line segment joining $+Q$ and $+q$.
Electric Charges and Fields

272156 If an electron has an initial velocity in a direction different from that of an electric field, the path of the electron is

1 a straight line
2 a circle
3 an ellipse
4 aparabolà
Electric Charges and Fields

272157 In the figure, charge $q$ is placed at origin $\rho $. When the charge $q$ is displaced from its position the electric field at point $P$ changes

1 at the same time when $q$ is displaced.
2 at a time after $\frac{OP}{c}$ where $c$ is the speed of light.
3 at a time after $\frac{OPcos\theta }{c}$
4 at a time after $\frac{OPsin\theta }{c}$
Electric Charges and Fields

272158 The electric field intensity just sufficient to balance the earth's gravitational attraction on an electron will be: (given mass, charge of an electron respectively are $9.1\times {{10}^{-31}}~kg$ and $1.6\times {{10}^{-19}}C$.)

1 $-5.6\times {{10}^{-11}}~N/C$
2 $-1.6\times {{10}^{-19}}~N/C$
3 $-4.8\times {{10}^{-15}}~N/C$
4 $-3.2\times {{10}^{-19}}~N/C$
Electric Charges and Fields

272159 $ABC$ is an equilateral triangle. Charges $+q$ are placed at each corner as shown in fig. The electric intensity at centre $O$ will be

1 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{r}$.
2 $\frac{1}{4\pi {{\epsilon }_{0}}}\frac{q}{{{r}^{2}}}$
3 $\frac{1}{4\pi {{\epsilon }_{o}}}\frac{3q}{{{r}^{2}}}$
4 zero