Have a query? Ask a Tutor!!

Access to best educators and exclusive paper discussions

Offsite Campus Turito Championship

Can’t find what you’re looking for?

Our tutors are from top schools around the world, and they are waiting for you 24/7, anytime, anywhere.

Homework- One to One Solutions
Understand concepts to solve better
Get your doubts solved instantly

Physics-

General

Easy

Question

The effective resistance across the points A and I is

2 $Ω$
1 $Ω$
0.5 $Ω$
5 $Ω$

The correct answer is: 1 $capital omega$

Related Questions to study

In the figure, the value of resistance to be connected between C and D so that the resistance of the entire circuit between A and B does not change with the number of elementary sets used is

In the figure, the value of resistance to be connected between C and D so that the resistance of the entire circuit between A and B does not change with the number of elementary sets used is

physics-General

The resistance of the network between the terminals A and B is

The resistance of the network between the terminals A and B is

physics-General

A current of 3A flows in a circuit shown in the figure The potential difference between A and B is

A current of 3A flows in a circuit shown in the figure The potential difference between A and B is

physics-General

parallel

A conductor has a non-uniform section as shown in the figure A steady current is flowing through it Then the drift speed of the electrons

A conductor has a non-uniform section as shown in the figure A steady current is flowing through it Then the drift speed of the electrons

physics-General

Certain plane wavefronts are shown in figure. The refractive index of medium is

Certain plane wavefronts are shown in figure. The refractive index of medium is

physics-General

Plane wave fronts are incident on a spherical mirror as shown in the figure. The reflected wave fronts will be

Plane wave fronts are incident on a spherical mirror as shown in the figure. The reflected wave fronts will be

physics-General

parallel

Wavefronts incident on an interface between the media are shown in the figure. The refracted wavefront will be as shown in

Wavefronts incident on an interface between the media are shown in the figure. The refracted wavefront will be as shown in

physics-General

Spherical wavefronts shown in figure, strike a plane mirror. Reflected wavefront will be as shown in

Spherical wavefronts shown in figure, strike a plane mirror. Reflected wavefront will be as shown in

physics-General

The figure shows the interference pattern obtained in a double–slit experiment using light of wavelength 600nm.

The third order bright fringe is

The figure shows the interference pattern obtained in a double–slit experiment using light of wavelength 600nm.

The third order bright fringe is

physics-General

parallel

The optical path length followed by ray from point A to B given that laws of reflection are obeyed as shown in figure is

The optical path length followed by ray from point A to B given that laws of reflection are obeyed as shown in figure is

physics-General

The optical path length followed by ray from point A to B given that laws of refraction are obeyed as shown in figure

The optical path length followed by ray from point A to B given that laws of refraction are obeyed as shown in figure

physics-General

In the figure an arrangement of young's double slit experiment is shown. A parallel beam of light of wavelength $blank to the power of ´ end exponent lambda to the power of ´ end exponent$ (in medium $n subscript 1 end subscript$ ) is incident at an angle $blank to the power of ´ end exponent theta to the power of ´ end exponent$ as shown. Distance $S subscript 1 end subscript O equals S subscript 2 end subscript O$ . Point 'O' is the origin of the coordinate system. The medium on the left and right side of the plane of slits has refractive index $n subscript 1 end subscript$ and $n subscript 2 end subscript$ respectively. Distance between the slits is d. The distance between the screen and the plane of slits is D Using $D equals 1 m comma d equals 1 m m comma theta equals 30 to the power of ring operator end exponent comma lambda equals 0.3 m m comma n subscript 1 end subscript equals fraction numerator 4 over denominator 3 end fraction comma n subscript 2 end subscript equals fraction numerator 10 over denominator 9 end fraction comma$ answer the following

The y-coordinate of the point where the total phase difference between the interefering waves is zero, is

In the figure an arrangement of young's double slit experiment is shown. A parallel beam of light of wavelength $blank to the power of ´ end exponent lambda to the power of ´ end exponent$ (in medium $n subscript 1 end subscript$ ) is incident at an angle $blank to the power of ´ end exponent theta to the power of ´ end exponent$ as shown. Distance $S subscript 1 end subscript O equals S subscript 2 end subscript O$ . Point 'O' is the origin of the coordinate system. The medium on the left and right side of the plane of slits has refractive index $n subscript 1 end subscript$ and $n subscript 2 end subscript$ respectively. Distance between the slits is d. The distance between the screen and the plane of slits is D Using $D equals 1 m comma d equals 1 m m comma theta equals 30 to the power of ring operator end exponent comma lambda equals 0.3 m m comma n subscript 1 end subscript equals fraction numerator 4 over denominator 3 end fraction comma n subscript 2 end subscript equals fraction numerator 10 over denominator 9 end fraction comma$ answer the following

The y-coordinate of the point where the total phase difference between the interefering waves is zero, is

physics-General

parallel

Statement–1: Two point coherent sources of light S1 and S2 are placed on a line as shown. P and Q are two points on that line. If at point P maximum intensity is observed then maximum intensity should also be observed at Q

Statement–2: In the figure of statement 1, the distance |S₁ P – S₂ P| is equal to distance |S₂Q – S₁Q|.

Statement–1: Two point coherent sources of light S1 and S2 are placed on a line as shown. P and Q are two points on that line. If at point P maximum intensity is observed then maximum intensity should also be observed at Q

Statement–2: In the figure of statement 1, the distance |S₁ P – S₂ P| is equal to distance |S₂Q – S₁Q|.

physics-General

In an interfrence arrangement similar to Young's double- slit experiment, the slits $S subscript 1 end subscript & S subscript 2 end subscript$ are illuminated with coherent microwave sources, each of frequency 106 Hz. The sources are synchronized to have zero phase difference. The slits are separated by a distance d = 150.0 m and screen is at very large distance from slits. The intensity I(q) is measured as a function of $theta$ , where $theta$ is defined as shown. Screen is at a large distance. If $I subscript 0 end subscript$ is the maximum intensity then I ( $theta$ ) for $0 less or equal than theta less or equal than 90 to the power of ring operator end exponent$ is given by:

In an interfrence arrangement similar to Young's double- slit experiment, the slits $S subscript 1 end subscript & S subscript 2 end subscript$ are illuminated with coherent microwave sources, each of frequency 106 Hz. The sources are synchronized to have zero phase difference. The slits are separated by a distance d = 150.0 m and screen is at very large distance from slits. The intensity I(q) is measured as a function of $theta$ , where $theta$ is defined as shown. Screen is at a large distance. If $I subscript 0 end subscript$ is the maximum intensity then I ( $theta$ ) for $0 less or equal than theta less or equal than 90 to the power of ring operator end exponent$ is given by:

physics-General

In an interfrence arrangement similar to Young's double- slit experiment, the slits $S subscript 1 end subscript & S subscript 2 end subscript$ are illuminated with coherent microwave sources, each of frequency 106 Hz. The sources are synchronized to have zero phase difference. The slits are separated by a distance d = 150.0 m and screen is at very large distance from slits. The intensity I(q) is measured as a function of $theta$ , where $theta$ is defined as shown. Screen is at a large distance. If $I subscript 0 end subscript$ is the maximum intensity then I ( $theta$ ) for $0 less or equal than theta less or equal than 90 to the power of ring operator end exponent$ is given by:

In an interfrence arrangement similar to Young's double- slit experiment, the slits $S subscript 1 end subscript & S subscript 2 end subscript$ are illuminated with coherent microwave sources, each of frequency 106 Hz. The sources are synchronized to have zero phase difference. The slits are separated by a distance d = 150.0 m and screen is at very large distance from slits. The intensity I(q) is measured as a function of $theta$ , where $theta$ is defined as shown. Screen is at a large distance. If $I subscript 0 end subscript$ is the maximum intensity then I ( $theta$ ) for $0 less or equal than theta less or equal than 90 to the power of ring operator end exponent$ is given by:

physics-General

parallel

card img

With Turito Academy.

card img

With Turito Foundation.

card img

Get an Expert Advice From Turito.

Turito Academy

card img

With Turito Academy.

Test Prep

card img

With Turito Foundation.