Lab 5: Spectroscopy & the Hydrogen Atom Phy248 Spring 2009

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Lab 5: Spectroscopy & the Hydrogen Atom Phy248 Spring 2009 Name Section Return this spreadsheet to your TA that will use it to score your lab. To receive full credit you must use complete sentences and explain your reasoning clearly. Introduction This lab is about atomic physics. Emission and absorption spectra can be a unique fingerprint of an atom or molecule. The photon energies and wavelengths in absorption or emission spectra are directly related to the allowed quantum energy states of the system. Your goal is to measure emission lines of the Hydrogen atom, and correlate them with transitions of the atom between different quantum states. You do this by measuring the wavelength of photons emitted by Hydrogen atoms in excited quantum states. You use a diffraction grating to disperse the wavelengths at different angles (by constructive interference), and a spectrometer to accurately measure the angles. Any safety issues? The green plastic filter is in front of the Mercury source to block ultraviolet radiation, so don t remove it. PARTA: Measuring diffraction angles and the grating spacing with the spectrometer In Lab 2 we used a CD or DVD, consisting of many closely spaced tracks acting as slits, behaving as a reflective diffraction grating. The grating you use in the spectrometer in this lab works in transmission, but is otherwise the same: it has many closely spaced slits, with a density of 600 slits/mm. d sin! = m" This is actually close to the track spacing that you found for the CD. In that experiment you aimed a red laser at the CD and found that each groove acted as a source of spherical waves, and these canceled by destructive interference except at particular angles " determined by the wavelength according to m" = dsin#, where d is the slit spacing and m an integer indicating the order of diffraction. In that experiment you used a laser that emits in a very small interval of wavelengths, so it is approximately a monochromatic source. Here the incoming light may be made of several different wavelengths. Each wavelength will diffract constructively at particular angles given by the

above formula. The spectrometer allows for very accurate measurements of the angles for which constructive interference occurs for light passing through the diffraction grating. By considering the precision of the instruments you use you will have to determine the errors on each measurement you do. A1) Suppose you see only four diffracted rays from the diffraction grating, at angles of " = 20, " = 23, " = 43.16, and " = 51.4. You detect these with your eye, so you know they are all in the visible spectrum. What wavelengths are in the incoming light? Angle d sin" (nm) m λ (nm) 20 570.15 1 23 651.35 1 43.16 1140.29 2 51.4 1302.79 2 51.4 1302.79 3 Apparatus: precision spectrometer, mercury and hydrogen discharge tubes; diffraction grating. The spectrometer has three main pieces (shown in the figure): 1. A collimator (makes rays hitting the diffraction grating parallel); 2

2. Diffraction grating; 3. An observation telescope (to accurately view the spectral lines) Operation of the spectrometer and adjustments: The collimator has a slit on the far end, and a lens on the near end that makes the light rays from the slit parallel. You turn the knurled knob C) to open and close the slit. Opening the slit gives a brighter image, but less angular resolution. The viewing telescope can be focused, and its angle can be changed. Two adjustments to focus the viewing telescope: i) Slide the eyepiece tube in or out until the crosshairs are in focus. ii) Sight telescope at a distant object and focus the telescope by rotating its focus ring until the object's clear image falls on the cross hairs. The telescope, now focused for parallel rays, will stay so as long as the focus ring is unmoved; but one may still adjust the eyepiece to suit the observer. Become familiar with the clamping and fine adjustment controls for telescope and prism table angles. You can: i) loosen the telescope clamp and move the telescope with your hand (coarse adjust) ii) tighten the telescope clamp, and turn the fine-adjust knurled knob (fine adjust) Never force a motion - you may damage the instrument. If at the end of a fine adjustment, loosen and reclamp! The prism table clamp sets table elevation: no fine adjustment is necessary [K and L are to make the grating perpendicular to the collimator, and to adjust the angle scale so that it indicates 0 when the viewing telescope is aligned exactly on the axis of the collimator]. I and J are 2 angle scale reading ports and verniers with 30 divisions per half degree. Each division has 1/30 x ½ = 1/60 of a degree. Read carefully the description on how to measure angles with the vernier scale on the last page of this handout. A2) Why does the collimator improve the accuracy of the spectrometer? What would be different if it didn t have a collimator? 3

A3) Align the telescope with the collimator so that the slit image falls exactly on the vertical cross hair. Mount the grating on the dowel pins in the prism table. Adjust and clamp the table so that the grating is approximately perpendicular to the telescopecollimator axis. Adjust the table so that the front grating face is accurately perpendicular to the telescope: the reflected image of the cross hairs should fall on the cross hairs. (Two reflected images can result if the sides of the grating glass are not parallel. If so, test which image comes from the grating side by wetting the other side.) Clamp prism table in this position and record the telescope direction. A4) Turn on the desk lamp so it shines through the slit. Put the black cloth over the spectrometer to block out stray light. Unlock the telescope and rotate it left and right while viewing to find the continuous spectrum on either side of the central maximum. 1. Is the order of the colors what you would expect from d sin! = m"? Explain 2. Pick a color or edge of a color in the spectrum with the telescope crosshairs and lock the telescope in place. Use the angle scale and vernier to determine the angle away from the central maximum. 3. Unlock the telescope and align it with the same color or edge of a color on the opposite side of the central maximum. Record the angle away from the central maximum using the vernier. If there are two windows in which to read angles, use the one that reads zero straight ahead. But notice that if you read 20 to the left, you will read 340 to the right, (which you should record as 20 ). Always use the same window (the other will be different by 180 ). 4

4. Average the two angle readings and compute the wavelength of the color you chose. What is the precision of your angular measurement? A6) Replace the desk lamp with the Hg lamp. Make sure the green safety filter is in place (the filter blocks the UV part of the spectrum). Here you accurately determine the grating spacing d by measuring the diffraction angle of the " = 546.1 nm spectral line of mercury. Assume this value is accurate. (The table of wavelengths for Hg and H is given at the end of this spreadsheet). 1. Write down the angles (left and right) for the first and second order lines for λ = 546.1 nm. It is the by far the brightest green line in the spectrum. You should be able to see the green line, the doubled yellow line to the left, and some faint blue lines. If you can t resolve the two yellow lines, reduce the slit width until you can. 2. Calculate d and its error and the lines/mm for your grating. Show all your work and compare the result to the value written on your grating. [Hint: To calculate the error on d consider the error on the average of the angles you measured for each of the 2 orders and then make a weighted average using the values of the errors you obtain]. 5

PART B. Measuring spectral lines of the hydrogen atom Replace the Hg lamp with the hydrogen source and make sure it is exactly in front of the slit (if it is not, the lines will not be bright enough to see). B1) Measure for 3 or 4 atomic H spectral lines the wavelength assuming d from part A and repeat the procedure you did in part A to measure angles. Organize your data and calculations in the table including errors (see below) and make a plot of wavelength vs sinθ average. B2) Use the Balmer formula to calculate the Rydberg constant with its accuracy: Compare this value to the official value: R = 10 973 731.6 m -. B3) Calculate the photon energy for each line and show your work here. Remember hc =1240 ev " nm. color θ-left θ-right θ ± σ θ λ photon ± σ λ R H ±σ R E photon 6

B4) Atomic energy levels for hydrogen: Using the expression for the energy levels of the H 13.6 atom En =! ev 2, mark the energy levels on the n graph at right. Show your calculations. 0-1 - 2-3 - 4-5 - 6-7 - 8-9 -10-11 -12-13 E (ev) B5) Determine which transitions are responsible for the spectral lines in your table. Mark those transitions on the energy level diagram with an arrow drawn from the initial state to the final state. Indicate which spectral line (color) goes with which arrow. Explain your reasoning and give examples of why other transitions cannot be responsible for these lines. -14 7

Reading the vernier scale on the spectrometer The knurled ring about the collimator, B, controls the slit opening. The collimator has been already focused for parallel light and the collimator and telescope are perpendicular to the spectrometer's rotation axis. REMINDER ON READING A VERNIER 1) Position and tighten the telescope. 2) Move the magnifying glass to see the scale marking 3) Look where the zero mark on the upper scale is located. The degree reading is the first full degree mark to the left of the zero (210 in the top figure; 229 in the bottom figure). 4) Now make the minute reading: if the zero mark on the upper scale comes after a degree mark (the short lines on the lower scale) then start at 30', otherwise at 0'. 5) Next look for the two lines which match up best between the two scales. Read the number of the appropriate line on the upper scale and add it to the zero mark is just past a degree mark so we begin with 30'. The 15' mark is the one that lines up best so we get 210 15' for the top reading and 229 146' for the bottom one. 6) Now convert to decimal degrees, in this case 15/60 = 0.25, so = 210.25 8

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