ebook img

Principles of Instrumental Analysis 6th Edition Instructor's Manual PDF

235 Pages·1987·5.92 MB·English
Save to my drive
Quick download
Download
Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.

Preview Principles of Instrumental Analysis 6th Edition Instructor's Manual

Skoog/Holler/Crouch Chapter 1 Principles of Instrumental Analysis, 6th ed. Instructor’s Manual CHAPTER 1 1-1. A transducer is a device that converts chemical or physical information into an electrical signal or the reverse. The most common input transducers convert chemical or physical information into a current, voltage, or charge, and the most common output transducers convert electrical signals into some numerical form. 1-2. The information processor in a visual color measuring system is the human brain. 1-3. The detector in a spectrograph is a photographic film or plate. 1-4. Smoke detectors are of two types: photodetectors and ionization detectors. The photodetectors consist of a light source, such as a light-emitting diode (LED) and a photodiode to produce a current proportional to the intensity of light from the LED. When smoke enters the space between the LED and the photodiode, the photocurrent decreases, which sets off an alarm. In this case the photodiode is the transducer. In ionization detectors, which are the typical battery-powered detectors found in homes, a small radioactive source (usually Americium) ionizes the air between a pair of electrodes. When smoke enters the space between the electrodes, the conductivity of the ionized air changes, which causes the alarm to sound. The transducer in this type of smoke detector is the pair of electrodes and the air between them. 1-5. A data domain is one of the modes in which data may be encoded. Examples of data domain classes are the analog, digital and time domains. Examples of data domains are voltage, current, charge, frequency, period, number. 1 Principles of Instrumental Analysis, 6th ed. Chapter 1 1-6. Analog signals include voltage, current, charge, and power. The information is encoded in the amplitude of the signal. 1-7. Output Transducer Use LCD display Alphanumeric information Computer monitor Alphanumeric information, text, graphics Laser printer Alphanumeric and graphical information Motor Rotates to change position of attached elements 1-8. A figure of merit is a number that provides quantitative information about some performance criterion for an instrument or method. 1-9. Let c = molar concentration of Cu2+ in standard = 0.0287 M s c = unknown Cu2+ concentration x V = volume of standard = 0.500 mL s V = volume of unknown = 25.0 mL x S = signal for unknown = 23.6 1 S = signal for unknown plus standard = 37.9 2 Assuming the signal is proportional to c and c , we can write x s S = Kc or K = S /c 1 x 1 x After adding the standard ⎛V c +V c ⎞ S = K⎜ x x s s ⎟ 2 V +V ⎝ ⎠ x s Substituting for K and rearranging gives, SV c c = 1 s s x S (V +V )−SV 2 x s 1 x 2 Principles of Instrumental Analysis, 6th ed. Chapter 1 23.6×0.500 mL×0.0287 M c = = 9.00×10−4 M x 37.9(0.500 mL + 25.0 mL)−(23.6×25.0 mL) 1-10. The results are shown in the spreadsheet below. (a) Slope, m = 0.0701, intercept, b = 0.0083 (b) From LINEST results, SD slope, s = 0.0007, SD intercept, s = 0.0040 m b (c) 95% CI for slope m is m ± ts where t is the Student t value for 95% probability and N – m 2 = 4 degrees of freedom = 2.78 95% CI for m = 0.0701 ± 2.78 × 0.0007 = 0.0701 ± 0.0019 or 0.070 ± 0.002 For intercept, 95% CI = b ± ts = 0.0083 ± 2.78 × 0.004 = 0.0083 ± 0.011 or 0.08 ± 0.01 b (d) c = 4.87 ± 0.086 mM or 4.87 ± 0.09 mM u 3 Principles of Instrumental Analysis, 6th ed. Chapter 1 1-11. The spreadsheet below gives the results (a) See plot in spreadsheet. (b) c = 0.410 μg/mL u (c) S = 3.16V + 3.25 s bc 3.246×2.000 μg/mL (d) c = s = =0.410 μg/mL u mV 3.164 mL−1×5.00 mL u (e) From the spreadsheet s = 0.002496 or 0.002 μg/mL c 4 Principles of Instrumental Analysis, 6th ed. Chapter 2 2-3. V = 12.0 × [(2.5 + 4.0) × 103]/[(1.0 + 2.5 + 4.0) × 103] = 10.4 V 2.4 With meter in parallel across contacts 2 and 4, 1 1 1 R + 6.5 kΩ = + = M R (2.5 + 4.0) kΩ R R ×6.5 kΩ 2,4 M M R = (R × 6.5 kΩ)/(R + 6.5 kΩ) 2,4 M M (a) R = (5.0 kΩ × 6.5 kΩ)/(5.0 kΩ + 6.5 kΩ) = 2.83 kΩ 2,4 V = (12.0 V × 2.83 kΩ)/(1.00 kΩ + 2.83 kΩ) = 8.87 V M 8.87 V−10.4 V rel error = × 100% = −15% 10.4 V Proceeding in the same way, we obtain (b) –1.7% and (c) –0.17% 2-4. Applying Equation 2-19, we can write 750 Ω (a) −1.0% = ×100% (R −750 Ω) M R = (750 × 100 – 750) Ω = 74250 Ω or 74 kΩ M 750 Ω (b) −0.1% = ×100% (R −750 Ω) M R = 740 kΩ M 2-5. Resistors R and R are in parallel, the parallel combination R is given by Equation 2-17 2 3 p R = (500 × 200)/(500 + 200) = 143 Ω p (a) This 143 Ω R is in series with R and R . Thus, the voltage across R is p 1 4 1 V = (15.0 × 100)/(100 + 143 + 1000) = 1.21 V 1 V = V = 15.0 V × 143/1243 = 1.73 V 2 3 V = 15.0 V × 1000/1243 = 12.1 V 4 2 Principles of Instrumental Analysis, 6th ed. Chapter 2 (b) I = I = 15.0/(100 + 143 + 1000) = 1.21 × 10–2 A 1 5 I = 1.73 V/500 Ω= 3.5 × 10–3 A 2 I = I = 1.73 V /200 Ω = 8.6 × 10–3 A 3 4 (c) P = IV = 1.73 V× 8.6 × 10–3 A = 1.5 × 10–2 W (d) Since point 3 is at the same potential as point 2, the voltage between points 3 and 4 V′ is the sum of the drops across the 143 W and the 1000 W resistors. Or, V ′ = 1.73 V + 12.1 V = 13.8 V. It is also the source voltage minus the V 1 V ′ = 15.0 – 1.21 = 13.8 V 2-6. The resistance between points 1 and 2 is the parallel combination or R and R B C R = 2.0 kΩ × 4.0 kΩ/(2.0 kΩ + 4.0 kΩ) = 1.33 kΩ 1,2 Similarly the resistance between points 2 and 3 is R = 2.0 kΩ × 1.0 kΩ/(2.0 kΩ + 1.0 kΩ) = 0.667 kΩ 2,3 These two resistors are in series with R for a total series resistance R of A T R = 1.33 kΩ + 0.667 kΩ + 1.0 kΩ = 3.0 kΩ T I = 24/(3000 Ω) = 8.0 × 10–3 A (a) P = I2R = (8.0 × 10–3)2 × 1.33 × 103 = 0.085 W 1,2 1,2 (b) As above I = 8.0 × 10–3 A (c) V = IR = 8.0× 10–3 A × 1.0 × 103 Ω = 8.0 V A A (d) V = 14 × R /R = 24 × 0.667/3.0 = 5.3 V D 2,3 T (e) V = 24 – V = 24 -8.0 = 16 V 5,2 A 2-7. With the standard cell in the circuit, V = V × AC/AB where V is the battery voltage std b b 3 Principles of Instrumental Analysis, 6th ed. Chapter 2 1.018 = V × 84.3/AB b With the unknown voltage V in the circuit, x V = V × 44.2/AB x b Dividing the third equation by the second gives, 1.018 V 84.3 cm = V 44.3 cm x V = 1.018 × 44.3 cm/84.3 cm = 0.535 V x R 2-8. E = − S ×100% r R +R M S 20 For R = 20 Ω and R = 10 Ω, E = − ×100% = −67% S M r 10+20 20 Similarly, for R = 50 Ω, E = − ×100% = −29% M r 50+20 The other values are shown in a similar manner. R 2-9. Equation 2-20 is E = − std ×100% r R +R L std 1 Ω For R = 1 Ω and R = 1 Ω, E = − ×100% = −50% std L r 1 Ω+1 Ω 1 Ω Similarly for R = 10 Ω, E = − ×100% = −9.1% L r 10 Ω+1 Ω The other values are shown in a similar manner. 2-10. (a) R = V/I = 1.00 V/50 × 10–6 A = 20000 Ω or 20 kΩ s (b) Using Equation 2-19 20 kΩ −1% = − ×100% R +20 kΩ M 4 Principles of Instrumental Analysis, 6th ed. Chapter 2 R = 20 kΩ × 100 – 20 kΩ = 1980 kΩ or ≈ 2 MΩ M 2−11. Ι = 90/(20 + 5000) = 1.793 × 10–2 A 1 I = 90/(40 + 5000) = 1.786 × 10–2 A 2 % change = [(1.786 × 10–2 – 1.793 × 10–2 A)/ 1.793 × 10–2 A] × 100% = – 0.4% 2-12. I = 9.0/520 = 1.731 × 10–2 A 1 I = 9.0/540 = 1.667 × 10–2 A 2 % change = [(1.667 × 10–2 – 1.731 × 10–2 A)/ 1.731 × 10–2 A] × 100% = – 3.7% 2-13. i = I e–t/RC (Equation 2-35) init RC = 10 × 106 Ω × 0.2 × 10–6 F = 2.00 s I = 24V/(10 × 106 Ω) = 2.4 × 10–6 A init i = 2.4 × 10–6 e–t/2.00 A or 2.4 e–t/2.0 μA t, s i, μA t, s i, μA 0.00 2.40 1.0 1.46 0.010 2.39 10 0.0162 0.10 2.28 2-14. v = V e–t/RC (Equation 2-40) C C v /V = 1.00/100 for discharge to 1% C C 0.0100 = e–t/RC = e−t/R×0.015×10−6 ln 0.0100 = –4.61 = –t/1.5 × 10–8R t = 4.61 × 1.5 × 10–8R = 6.90 × 10–8R (a) When R = 10 MΩ or 10 × 106 Ω, t = 0.69 s (b) Similalry, when R = 1 MΩ, t = 0.069 s 5 Principles of Instrumental Analysis, 6th ed. Chapter 2 (c) When R = 1 kΩ, t = 6.9 × 10–5 s 2-15. (a) When R = 10 MΩ, RC = 10 × 106 Ω × 0.015 × 10–6 F = 0.15 s (b) RC = 1 × 106 × 0.015 × 10–6 = 0.015 s (c) RC = 1 × 103 × 0.015 × 10–6 = 1.5 × 10–5 s 2-16. Parts (a) and (b) are given in the spreadsheet below. For part (c), we calculate the quantities from i = I e-t/RC, v = iR, and v = 25 – v init R C R For part (d) we calculate the quantities from −v i = C e−t/RC, v = iR, and v = –v R C R R The results are given in the spreadsheet. 6 PPrriinncciipplleess ooff IInnssttrruummeennttaall AAnnaallyyssiiss,, 66tthh eedd.. CChhaapptteerr 22 77

See more

The list of books you might like

Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.