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X Ō Pas‰˜©ĀĆ,-cØ¢£¶½źAŸėģōR†Śt¬Ų¬Š¬$¬$ėt$¬$¬$¬$¬$¬$¬’$t $ ¦’$:Š$ ¦’$:Š$¬’$Ē6$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬’$zŗ$­Ż$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$¬$­Ż$¬$¬ą!X Ō P½źR†Śœ€€˜€€œ€€š€€œ€€˜€€˜€€ž€€š€€ž€€˜€€ž€€˜€€,.¬UU’’UnknownSethŲē茒’Seth8Seth's HD:Temporary Items:AutoRecovery save of Document1Seth(Seth's HD:Desktop Folder:Wave String LabSeth9Seth's HD:Temporary Items:AutoRecovery save of Wave StrinSeth9Seth's HD:Temporary Items:AutoRecovery save of Wave StrinSeth(Seth's HD:Desktop Folder:Wave String LabSeth/Seth's HD:section of string and then measure its mass. Be sure that all knots are removed from the string. 2. Set up the equipment. Tie one end of a piece of string to a vertical support rod that is clamped to one end of a table. Pass the other end of the string over a pulley that is mounted on a rod that is clamped to the other end of the table. Tie a mass hanger to the end of the string that hangs over the pulley. Put about 500 grams on the mass hanger. 3. Place the wave driver under the string near the vertical support rod. Insert the string in the slot on the top of the driver plug of the wave driver so the wave driver can cause the string to vibrate up and down. Use patch cords to connect the wave driver into the output jacks of the power amplifier. 4. Use the meter stick to measure the length of the section of the string, L, that will be vibrating (the part between the driver plug of the wave driver and the top of the pulley). Part I - Constant tension, vary frequency 1. Vary the output frequency of the Signal Generator until the string vibrates in one segment (the fundamental frequency). Hint: Frequency Adjustment - You can adjust the frequency of the output by using the cursor and clicking on the frequency “up-down” arrows. You can also enter a value from the keyboard. To type in a value from the keyboard, click once on the value of frequency. A small edit box will appear where you can type a new value. Press or to accept the value. When using the cursor and mouse button to click on the up-down arrows next to the frequency value, the default change is 10 Hz per click. You can use modifier keys (Control, Option and Command or CTRL and ALT) to increase or decrease the amount of change per click. Windows Key Dš f Shift key 100 Hz No modifier key 10 Hz Ctrl key 1 Hz Alt key 0.1 Hz Alt + Ctrl keys 0.01 Hz 2. Find the frequencies required for the higher harmonics (n = 2 through 7) and record these in Table 2. Part II - Constant frequency and length, vary tension 1. Put enough mass on the mass hanger to make the string vibrate in its fundamental mode (one antinode in the center) at a frequency of 60 Hz. Adjust the amount of mass until the nodes at each end are very dark and “clean” (not vibrating). Record the initial mass in the Table 1. (Be sure to include the mass of the hanger.) 2. Now change the amount of mass on the mass hanger until the string vibrates in each of the higher harmonics (for 2 segments through 8 segments) and record these masses in Table 1 section. Hint: Decrease the mass to increase the number of segments. ANALYZING THE DATA Part I 1. Plot the frequency vs. the period (1/f). 2. Find the slope of the line on the frequency vs. period. This is the wave velocity. 3. Calculate the wave velocity from the string tension and linear mass density of the string. 4. Calculate the percent difference between two wave velocity calculations. Part II 1. Plot the tension vs. the wavelength 2. Find the slope of the. The slope is equal to f2mš. 3. Calculate the linear mass density of the string. 4. Calculate the percent difference between two linear mass density calculations. 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After the slope has been determined, the linear mass density of the string can be calculated. PROCEEDURE Set-up 1. Calculate the linear mass density of the string - measure the length of a $78?@v|} vx " $ 2 4 6 ¢ ° ² ŗ X Z “ ¶ Ų ę č ź ņ Ä Ę z|~€BXf­×Ym$*ž“øŗ¼¾¬āåé"5<deŌä”–˜šU&.(.,.ū÷õ÷õšõõšīźšõźõõäõäõąššīŽš÷õõõŲŲ÷õŠ÷Ėõõ÷õīõīŽšŽīŽ 56>*5>*OJQJ 5OJQJH*5H* 5OJQJ566OJQJ55>*5CJ(M "#$78@uv}ą¢ ŗ Ų ņ ę × @BXfbĆõ¬ü÷ėéęééāééāāßéßéāāéé飣ŁŁ„h„˜ž$„Š$ $$–lÖ”’ą$$$$ "#$78@uv}ąH¢ ŗ Ų ņ ę × @BXfbĆõ¬­×SžĄä(AB«¬ā'!"5<hæ:ŅŌä2ž3GTUżżūłł÷÷łłłł :ģ„Įc 4æUjbjbšSšS ų0š1š1Ų’’’’’’]rrrrrr¶d<<<< HĻ $”””””””œ ž ž ž ž ž ž ,óōēPŹ r”””””Ź žrr””p žžž” r”r”œ †žrrrr”œ žžžœ rrœ d WŻ…ø"<žœ Physics 142Allen Hancock College Waves on a Strings PURPOSE The purpose of this laboratory is to investigate standing waves in a string and to use the relationship between the tension in the string, the linear mass density of the string, the frequency of oscillation, the length of the string, and the number of segments in the standing wave to find the wave velocity. THEORY When a stretched string is plucked it will vibrate in its fundamental mode in a single segment with nodes on each end. If the strin„Ą““€0½;’’ Physics 142SethSeth [0@ń’0NormalCJOJQJmH D`"D Heading 1 $¤š@&5CJ$OJPJQJ@`2@ Heading 2 ¤š@&g is driven at this fundamental frequency, a standing wave is formed. Standing waves also form if the string is driven at any integer multiple of the fundamental frequency. These higher frequencies are called the harmonics. Each segment is equal to half a wavelength. In general for a given harmonic, the wavelength is shown by ‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰lš = 2L/n where L is the length of the stretched string and n is the number of segments in the string. The velocity of any wave is given by v = lšf where f šis the frequency of the wave. For a stretched string: v = (2Lf)/n The velocity of a wave traveling in a string is also dependent on the tension, T, in the string and the linear mass density, mš, of the string: v = (T/mš)1/2 The linear mass density of the string can be directly measured by weighing a known length of the string: mš = mass/length. 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The slope of this line can be used to calculate the velocity of a wave in the string. If the tension is varied while the length and frequency are held constant, a plot of tension vs. ų?šĄ 0’’’’’’’’’’’’’’’’’’’’’’’’pģšų?ųų?ų?šĄ 3333333333333333333333333333333333333333:3333333333333333£333333333333333£333333333333333:Ŗ3333333333333333£333333333333333£33333lš will give a straight line which will have a slope equal to f2mš. After the slope has been determined, the linear mass density of the string can be calculated. PROCEEDURE Set-up 1. Calculate the linear mass density of the string - measure the length of a |,, € ’Ī’Ķ ² Ćg(ü,, € d'h|,, € ’Ī’Ķ ² Ćg(ü,, € d'h€equency of oscillation, the length of the string, and the number of segments in the standing wave to find the wave velocity. THEORY When a stretched string is plucked it will vibrate in its fundamental mode in a single segment with nodes on each end. If the strinž’’’’’ ĄFMicrosoft Word Documentž’’’NB6WWord.Document.8@ āž’ ÕĶ՜.“—+,ł®DÕĶ՜.“—+,ł®D hpˆ˜  Ø°øĄ Č ą'UCSB - MEE Dept":  Physics 142 Title˜ 6> _PID_GUID'AN{84E64481-1A1F-11D6-ABAE-000502F0FA2F}` €` €ž’ ą…ŸņłOh«‘+'³Ł0l˜¬øČŌä ō  ( 4 @LT\d' Physics 142hysSethcs ethNormal Sethl 7thMicrosoft Word 8.0d@P·Ņ@J·ŗw®Į@ų›^n®Į@>& ÜĮßaˆ˜ˆˆˆˆˆ™˜™ˆˆˆˆ™ˆ‰ˆˆˆˆ™ˆˆ˜˜ˆˆ™ˆˆˆˆ˜ˆ‰ [0@ń’0NormalCJOJQJmH @`2@ Heading 2 ¤š@&5B*OJPJQJ<A@ņ’”<Default Paragraph FontJžOņJEquationdą¤x¤x ĘŠ$ OJPJQJVžOVFigure Caption„8„Čūd ž¤ Ę8 OJPJQJFR@FBody Text Indent 2„hd,.61`1p1~1€1„1²1“1¶1ų1ś1÷õóķźåćß6H*H*OJQJCJ H*OJQJ5>*5CJOJQJ ģ„Įc DæUjbjbšSšS 4š1š1Ž’’’’’’]E¶ūūūūūST9999M§{&`•™™™™™™™æ Į Į Į Į Į Į ,Ū'ōĻ)Pķ Žū™™™™™ķ ¬­×SžĄä(AB«¬ā'!"5<hæ:ŅŌä2žżż÷żńńńńńńżżżż÷÷żżż÷÷÷÷÷ż÷÷÷„ „Š„h„˜žUł„h„˜ž €°Š/ °ą=!° "° # $ %° 2 2Æūū™™u ÆÆÆ™ū™ū™æ "1"ūūūū™æ ÆÆæ ūūæ i §SŅø§’9Ææ Physics 142Allen Hancock College Waves on a Strings PURPOSE The purpose of this laboratory is to investigate standing waves in a string and to use the relationship between the tension in the string, the linear mass density of the string, the frequency of oscillation, the length of the string, and the number of segments in the standing wave to find the wave velocity. THEORY When a stretched string is plucked it will vibrate in its fundamental mode in a single segment with nodes on each end. If the string is driven at this fundamental frequency, a standing wave is formed. Standing waves also form if the string is driven at any integer multiple of the fundamental frequency. These higher frequencies are called the harmonics. Each segment is equal to half a wavelength. In general for a given harmonic, the wavelength is shown by ‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰‰lš = 2L/n where L is the length of the stretched string and n is the number of segments in the string. The velocity of any wave is given by v = lšf where f šis the frequency of the wave. For a stretched string: v = (2Lf)/n The velocity of a wave traveling in a string is also dependent on the tension, T, in the string and the linear mass density, mš, of the string: v = (T/mš)1/2 The linear mass density of the string can be directly measured by weighing a known length of the string: mš = mass/length. If the frequency is varied while the tension and the length are held constant, a plot of frequency vs. wavelength will give a straight line. The slope of this line can be used to calculate the velocity of a wave in the string. If the tension is varied while the length and frequency are held constant, a plot of tension vs. ų?šĄ 0’’’’’’’’’’’’’’’’’’’’’’’’pģšų?ųų?ų?šĄ 3333333333333333333333333333333333333333:3333333333333333£333333333333333£333333333333333:Ŗ3333333333333333£333333333333333£33333lš will give a straight line which will have a slope equal to f2mš. After the slope has been determined, the linear mass density of the string can be calculated. PROCEEDURE Set-up 1. Calculate the linear mass density of the string - measure the length of a $78?@v|} vx " $ 2 4 6 ¢ ° ² ŗ X Z “ ¶ Ų ę č ź ņ Ä Ę z|~€BXf­×Ym$*ž“øŗ¼¾¬āåé"5<deŌä”–˜šU&.(.,.ū÷õ÷õšõõšīźšõźõõäõäõąššīŽš÷õõõŲŲ÷õŠ÷Ėõõ÷õīõīŽšŽīŽ 56>*5>*OJQJ 5OJQJH*5H* 5OJQJ566OJQJ55>*5CJ(M "#$78@uv}ą¢ ŗ Ų ņ ę × @BXfbĆõ¬ü÷ėéęééāééāāßéßéāāéé飣ŁŁ„h„˜ž$„Š$ $$–lÖ”’ą$$$$ "#$78@uv}ąH¢ ŗ Ų ņ ę × @BXfbĆõ¬­×SžĄä(AB«¬ā'!"5<hæ:ŅŌä2ž3GTUżżūłł÷÷łłłł :¬­×SžĄä(AB«¬ā'!"5<hæ:ŅŌä2žżż÷żńńńńńńżżżż÷÷żżż÷÷÷÷÷ż÷÷÷„ „Š„h„˜žU 16181:1`1p1łņėßŪŪŁ¤ $$–lÖ”’Hü$$¤$$¤$„h„˜ž €°Š/ °ą=!° "° # $ %° 2 2|,, € ’Ī’Ķ ² Ćg(ü,, € d'h|,, € ’Ī’Ķ ² Ćg(ü,, € d'h€Phys 142Allan Hancock College Waves on a String PURPOSE (2Lf)/n2š a table squared (T vs. lš2) graph by dividing the slope by 2