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Objective
• To characterize the friction force at the bowing point with the following variables– Normal force– Bow velocity– Rosin layer thickness– Contact temperature
• Current models are not adequate
Traditional Models
• Linear model– Constant friction force characterized by
coefficients µk, µs
– Ff = µk Fn
• Velocity dependent model– Functional dependence on bow velocity– Single value
Shortcomings
• Friction on a bowed string is not directly measurable
• Frictional force is cyclical• The rosin is a dynamic system
– Properties are time and temperature dependent• Softening• Viscosity
• Force is not single-valued for given velocity• Physical system is history dependent
Helmholtz Motion
• Describes ideal string with rigid terminations and no energy losses– Bow movement supplies lost energy
• Slip-stick cycle
• String acts on rosin– Wear tracks– Softening-hardening
Rosin
• What is rosin?– Intermediary between bow and string– Facilitates Helmholtz motion– Abietic acid and impurities– ClearTone™
• Polymer which has properties which mimic rosin
Procedure
• Coat glass rod in rosin solution
• Make reference mark in rosin layer– Causes disturbance in data to correlate with
images
• Run glass rod across E string (660 Hz)
Procedure
• Measure force at terminations of string
• From these measurements, the friction force can be reconstructed
nut bridge
Observation Techniques
• CCD Camera– Used to obtain string deflection data
• Optical Microscopy– Ordinary microscope + camera
• Scanning Electron Microscopy (SEM)– CMU Materials Science Department
Conclusions
• Able to reconstruct friction force
• Able to calculate energy deposited during slip region of cycle
• Able to correlate forces to wear tracks
Image Credits
• http://www.hilaryhahn.com
• http://www.pbs.org/wnet/americanmasters/database/menuhin_y.html
• http://www.centrum.is/hansi/
• http://library.thinkquest.org/27178/en/index.html
• http://www.nelson.planet.org.nz/~matthew/cbt.html
• http://www.theviolinman.co.uk/about.html