TY - GEN
T1 - Poled PVDF-TrFE coatings on quartz microbalance sensors
T2 - 2011 IEEE 14th International Symposium on Electrets, ISE 2011
AU - Lang, S. B.
AU - Abuhatzira, Y.
AU - Gandhi, A. A.
AU - Korostynska, O.
AU - Tofail, S. A.M.
AU - Kost, J.
AU - Robin, S.
AU - Soulimane, T.
PY - 2011/12/1
Y1 - 2011/12/1
N2 - A quartz crystal microbalance (QCM) measures mass per unit area by determining the change in frequency of a quartz crystal resonator caused by the addition of a small mass. The nominal resonance frequency of the shear mode of the quartz sensor is 5 MHz. A frequency change of 0.1 Hz corresponds to an addition of about 2 ng/cm 2 of mass to the quartz surface. Sauerbrey was the first to recognize the potential usefulness of the QCM technology and demonstrate its extreme sensitivity to mass changes [1]. He developed the fundamental equation describing the QCM: Δ f o 2/(ρ qμ q 1/2 Δm=-56.6 Δm (1) Here Δf = change in frequency (Hz), f 0 = fundamental frequency of resonator (MHz), ρ q = quartz density (2.648 g cm -3), μ q = shear modulus of AT-cut quartz (2.947 x 10 11 g cm -1 s -2), and Δm = mass change/unit area (μg/cm 2). The AT-cut is used because its resonant frequency is almost temperature-independent.
AB - A quartz crystal microbalance (QCM) measures mass per unit area by determining the change in frequency of a quartz crystal resonator caused by the addition of a small mass. The nominal resonance frequency of the shear mode of the quartz sensor is 5 MHz. A frequency change of 0.1 Hz corresponds to an addition of about 2 ng/cm 2 of mass to the quartz surface. Sauerbrey was the first to recognize the potential usefulness of the QCM technology and demonstrate its extreme sensitivity to mass changes [1]. He developed the fundamental equation describing the QCM: Δ f o 2/(ρ qμ q 1/2 Δm=-56.6 Δm (1) Here Δf = change in frequency (Hz), f 0 = fundamental frequency of resonator (MHz), ρ q = quartz density (2.648 g cm -3), μ q = shear modulus of AT-cut quartz (2.947 x 10 11 g cm -1 s -2), and Δm = mass change/unit area (μg/cm 2). The AT-cut is used because its resonant frequency is almost temperature-independent.
UR - http://www.scopus.com/inward/record.url?scp=84855289566&partnerID=8YFLogxK
U2 - 10.1109/ISE.2011.6085042
DO - 10.1109/ISE.2011.6085042
M3 - Conference contribution
AN - SCOPUS:84855289566
SN - 9781457710230
T3 - Proceedings - International Symposium on Electrets
SP - 181
EP - 182
BT - 2011 - 14th International Symposium on Electrets, ISE 2011
Y2 - 28 August 2011 through 31 August 2011
ER -