VELAMMAL BODHI CAMPUS KOLAPAKKAM, CHENNAI - 600 128 OF 4 e@ A Project Report On Submitted By Roll No : Name Class: XII Under the Guidance Of Department ofVELAMMAL BODHI CAMPUS OF 4 DEPARTMENT OF 2024 - 2025 IF) E The project report is entitled. This is to certify that this is the bonafide record of project work done by Master / Miss. of Grade XII during the academic year 2024-2025. Submitted for SSCE-2024 Practical Examination held on at Velammal Bodhi Campus, Kolapakkam, Kanchipuram District. Date: : Teacher In-charge PRINCIPAL INTERNAL EXAMINER EXTERNAL EXAMINERDECLARATION I hereby declare that the project work entitled submitted to the Department of : The Velammal Bodhi Campus, is a record of an original work done by me and my team. XIACKNOWLEDGEMENT First of all we thank our beloved parents for providing us the opportunity to study in Velammal Bodhi Campus, Kolapakkam. We thank our beloved Director Sri. M. V. M SASIKUMAR for being our motivational force for the completion of this project. We thank our Principal Smt. R. LAVANYA for her exceptional support. We thank our Vice Principal Mrs. Lakshmi Prabha and our Faculty for encouraging and guiding us to complete this project. Last but not the least I thank all my friends who helped me in the completion of this project.INDEX INTRODUCTION AIM & APPARATUS THEORY PROCEDURE OBSERVATIONS RESULT & CONCLUSION APPLICATIONS SOURCES OF ERROR BIBLIOGRAPHYINTRODUCTION The general purpose photoconductive cell is also known as LDR — light dependent resistor, It is a type of semiconductor and its conductivity changes with proportional change in the intensity of light. There are two common types of materials used to manufacture the photoconductive cells. They are Cadmium Sulphide (CdS) and Cadmium Selenide (CdSe). Extrinsic devices have impurities added, which have a ground state energy closer to the conduction band - since the electrons don't have as far to jump, lower energy photons (i.e. longer wavelengths and lower frequencies) are sufficient to trigger the device. Two of its earliest applications were as part of smoke and fire detection systems and camera light meters. The structure is covered with glass sheet to protect it from moisture and dust and allows only light to fall on it. fa cadmium sulphide cover mataliplastc “ ane: colar” tarrirats + for eornectionApplications Lead sulfide (PbS) and indium antimonide (InSb) LDRs are used for the mid infrared spectral region. GeCu photoconductors are among the best far- infrared detectors available, and are used for infrared astronomy and infrared spectroscopy. Analog Applications ‘ Camera Exposure Control : Auto Slide Focus - dual cell ' Photocopy Machines - density of toner : Colorimetric Test Equipment * Densitometer - Electronic Scales - dual cell * Automatic Gain Control — modulated light source : Automated Rear View Mirror Digital Applications : Automatic Headlight Dimmer - Night Light Control - Oil Burner Flame Out : Street Light Control ‘ Position Sensor “LOR hes a disadvantage that when its temperature changes, its fesistance changes drastically fora particular light intensityAIM & APPARATUS AIM: To study the variations, in current flowing in a circuit containing a LDR, because of a variation:- (a) In the power of the incandescent lamp, used to ‘illuminate’ the LDR. (Keeping all the lamps at a fixed distance). (b) In the distance of a incandescentlamp, (of fixed power), used to ‘illuminate’ the LDR. APPARATUS: Light Dependent Resistor (LDR) Connecting Wires Source of different power rating (bulbs) Bulb Holder Metre scale Multi Meter Battery etTHEORY 1,) LDR and its characteristics When fight is incident on it, a photon is absorbed and thereby it excites an electron from valence band into conduction band. Due to such new electrons coming up in conduction band area, the electrical resistance of the device decreases. Thus the LDR or photo-conductive transducer has the resistance which is the inverse function of radiation intensity. _ he o£, AQ = threshold wavelength, In meters @ = charge on one electron, in Coulombs Ew = work function of the metal used, in Ew Ao Here we must note that any radiation with wavelength greater than the value obtained in above equation CANNOT PRODUCE any change in the resistance of this device, The band gap energy of Cadmium Sulphide is 2.42eV and for Cadmium Selenide it is1.74eV. Due to such large energy gaps, both the materials have extremely high resistivity at room temperature.Characteristics of photoconductive cells Now when the device is kept in darkness, its resistance is called as dark resistance. This resistance is typically of the order of 10 ohms. When light falls on it, its resistance decreases up to several kilo ohms or even hundreds of ohms, depending on the intensity of light, falling on it. The spectral response characteristics of two commercial cells were compared in our laboratory. And we found that there is almost no response to the radiation of a wavelength which was shorter than 300nm. it was very interesting to note that the Cadmium Sulphide cell has a peak response nearer or within the green color of the spectrum within a range of 520nm. Thus it can be used nearer to the infra-red region up to 750nm. It was found that the maximum response of Cadmium Sulphoselenide is in the yellow-orange range at 615nm and also it can be used in the infra-red region up to about 970nm.Sensitivity The sensitivity of a photo detector is the relationship between the light falling on the device and the resulting output signal. In the case of a photocell, one is dealing with the relationship between the incident light and the corresponding resistance of the cell, 1000 2 100 = 8 § 10 Pa w o = 10 0.1Spectral Response Like the human eye, the relative sensitivity of a photoconductive cell is dependent on the wavelength (color) of the incident light. Each photoconductor material type has its own unique spectral response curve or plot of the relative response of the photocell versus wavelength of light. 9939 28 RHE RS ee ee ee ee ee ee ee ‘Whreclaragt (rei2.) luminous flux variation: Considering the source to be a point radiating in all directions; consider a steradian (or even a simple sphere), take a small element aA on the steradian ata distance ‘r from the source. It comprises a small part of the energy radiated (dEr). Now, go further to a distance ‘R’ (R=r) from the source, consider the same area element aA, it comprises a much smaller part of energy radiated (oEx). [aE: > aEn]. It varies inversely as the square of the distance.PROCEDURE + Choose a specific position for the source and mount it using a holder, make sure it is stable. Select the bulb with the lowest power rating and connect it to the holder as shown in the figure. Connect the LDR, baiteryi6V) and the multimeter in series. Set the multimeter to ohm section and select suitable range and measure the resistance with a bulb on. Similarly switch to current section and move to micro ampere in the multimeter. This gives the value of the current. Repeat these steps with different power sources at different distances and note down observations.OBSERVATIONS The experiment has been conducted by using various sources with different power ratings. Voltage of the battery = 6 V 1.) 15 watts (yellow) (wavelength = 570nm) “Seal | DISTANCE FROM | RESISTANCE [ CURRENT | No SOURCE (Kila ohm) (micro ampara) (em) 7 ET 1425 a0 2. a0 69 | 80 mes Eg a7 T 10 £ 20 oF 30 2.) 15 watts (incandescent) (mean wavelength = 610nm Senal DISTANCE FROM RESISTANCE CURRENT No SOURCE (Kilo ohm) (micro ampere) (om) 1 50 61 | 120 Zz 40 36 170 4, a0 22 270 = 20 1” =403.) 40 watts (incandescent) (mean wavelength = 610nm) Serial) OISTANCE FROM | RESISTANCE CURRENT | No SOURCE (Kilo ohm) — | (micro ampere} (em) 1. 50. | 20 00 | Z Fn) 3 460 1 3 30 as 700 | # 20 45 wo 4.) 20 watts (CFL) (white light) Serial | DISTANCE FROM | RESISTANCE CURRENT No SOURCE (Kilo ohm) (micro ampere) fem} i 50 15.5 380 z a0 10 600 3. » 6 1000 ; _ 5 extekCONCLUSION & RESULT + The LDR resistance decreases with increase in intensity of light and hence there is an increase in the flow of current. . There is an increase in the current as the distance from the source decreases. . The intensity decreases as the distance from the source increases - The error lies within the experimental limit.SOURCES OF ERROR + The LDR may not be perpendicular to the source, . Connections may be faulty. . The experiment should be conducted in a dark room. + Measurements should be taken accurately.BIBLIOGRAPHY . NCERT physics class Xi! . Art of Electronics by paul worowitz + www. wikipedia,com/ + www. electronics2000.co.uk/links/education-hobby/ + www.ecelab.com/ - laboratory manual in physics - Practical physics