Products / Physics Lab Instruments / Diffraction / Detector Based Apparatus for Diffraction Experiments

Detector Based Apparatus for

Diffraction Experiments

Diffraction Experiments

Model: HO-ED-D-02

This apparatus (Model No: HO-ED-D-02) is meant for graduate and post graduate level courses in physics. Here, the diffraction pattern is closely studied using a detector mounted on translation stage. The device consists of one meter long optical rail along with carriages, optics and opto-mechanics. At one end of the rail, X - translation stage with detector is mounted and at the other end, laser is held on a kinematic mount. Linear scale attached to the rail makes length measurement easy and convenient. Both the laser head and detector stages are mounted on rail carriages with locks, which in turn can be mounted anywhere on the rail conveniently.

In this apparatus, diffraction experiments are carried out with a photo sensitive detector and laser is used as light source. The diffraction element is placed at a certain distance from the detector and the pattern is allowed to fall on the detector stage. The micrometer driven stage is used to move the detector to extreme end of the diffraction pattern and the intensity is noted at close intervals by traversing the detector through the cross section of the spectrum. The intensity versus distance curve is plotted on a graph for calculations.

Experiment Examples

Diffraction of light by single slit

The diffraction equation (condition for minima) is,

**Sin θ _{m} = m λ / d**

Where **d** is the slit width, **m** is the order, **λ** is the wavelength of laser used and **θ _{m}** is the angle subtended within the central maximum and

From this we can find out the slit width **d** as

**d = m λ / Sin θ _{m}**

Diffraction of light by double slit

The diffraction equation (condition for maxima) is,

**Sin θ _{m} = m λ / d**

Where **d** is the slit width, **m** is the order, **λ** is the wavelength of laser used and **θ _{m}** is the angle subtended within the central maximum and

From this we can find out the slit width **d** as

**d = m λ / Sin θ _{m}**

Diffraction of light by single wire

The diffraction equation (condition for maxima) is,

**Sin θ _{m} = m λ / d**

Where **d** is the slit width, **m** is the order, **λ** is the wavelength of laser used and **θ _{m}** is the angle subtended within the central maximum and

From this we can find out the slit width **d** as

**d = m λ / Sin θ _{m}**

Diffraction of light by cross wire

The diffraction equation (condition for maxima) is,

**Sin θ _{m} = m λ / d**

**d** is the slit width, **m** is the order, **λ** is the wavelength of laser used and **θ _{m}** is the angle subtended within the central maximum and

From this we can find out the slit width **d** as

**d = m λ / Sin θ _{m}**

Diffraction of light by wire mesh

The diffraction equation (condition for maxima) is,

**Sin θ _{m} = m λ / d**

**d** is the slit width, **m** is the order, **λ** is the wavelength of laser used and **θ _{m}** is the angle subtended within the central maximum and

From this we can find out the slit width **d** as

**d = m λ / Sin θ _{m}**

Diffraction of light by transmission grating

The diffraction equation (condition for maxima) is,

**Sin θ _{m} = m λ / d**

**d** is the slit width, **m** is the order, **λ** is the wavelength of laser used and **θ _{m}** is the angle subtended within the central maximum and

From this we can find out the slit width **d** as

**d = m λ / Sin θ _{m}**

Diffraction of light by circular aperture (Pinhole)

Radius of the Airy’s disc,

**x = ( 1.22 l λ ) / a**

where,

**a** = Diameter of the aperture (pinhole),

**l** = Distance between the pinhole and the Screen,

**λ** = Wavelength of light,

**x** = Radius of the Airy’s disc

Thus we can find the diameter of the aperture (pinhole) using the equation

**a = ( 1.22 l λ ) / x**

Related Topics

Single slit

Double slit

Single wire

Cross wire

Wire mesh

Transmission grating

Circular aperture (pin hole)

Single slit

Double slit

Single wire

Cross wire

Wire mesh

Transmission grating

Circular aperture (pin hole)

Features

High measurement accuracy, clear and sharp diffraction patterns

Diffraction elements are fixed to metallic casing for ease of mounting

Smooth switch on and long lifetime of light source

Reliable and affordable

High measurement accuracy, clear and sharp diffraction patterns

Diffraction elements are fixed to metallic casing for ease of mounting

Smooth switch on and long lifetime of light source

Reliable and affordable

Scope of Supply

Optical Rail

Model No: ED-D-02-OR

Length

:

1000 mm

Material

:

Black anodized Aluminum alloy

Quantity

:

1 no.

Kinematic Laser Mount

Model No: ED-D-02-KLM

Material

:

Black anodized Aluminum alloy

Adjustments

:

Using 80 tpi lead screws

Adjustment Range

:

+/-4 degrees

Quantity

:

1 no.

Cell Mount

Model No: ED-D-02-CM

Material

:

Black anodized Aluminum alloy

Diameter

:

30 mm

Quantity

:

1 no.

Diffraction Cells

Model No: ED-D-02-DC

Single slit

:

50 & 100 micron

Double slit

:

100 & 200 micron

Transmission grating

:

30 lines / mm

Single wire

Cross wire

Wire mesh

Pinhole

Quantity

:

1 set.

Detector Mount with X- Translation

Model No: ED-D-02-DMX

Material

:

Black anodized Aluminum alloy

Travel

:

Micrometer controlled

Resolution

:

0.01 mm

Diameter

:

30 mm

Quantity

:

1 no.

Diode Laser with Power supply (Red)

Model No: ED-D-01-DLPR

Wave length

:

650 nm

Optical power

:

3 mW

Quantity

:

1 no.

Detector Output Measurement Unit

Model No: ED-D-02-DOMU

Sensor Type

:

Photo Transistor

Display

:

7 segment, 3 ½ digit

Range

:

0 - 199 milli / micro amperes

Quantity

:

1 no.

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