C035-01
Uniform Warming and Snowpack Disappearance in the Western US
Abstract:
T = T0 − T1 sin(ωt)
where T0 is the annual-mean temperature, T1 is the amplitude of the annual cycle in temperature, ω is the frequency of the annual cycle, and t is time in days. We analytically solve the model for the date of disappearance ζ, and then take the partial derivative with respect to annual-mean temperature to find the sensitivity of ζ to warming,
∂ζ/∂T0 = − 1/ω (1+Ra/Rm) (T12−T02)—1/2
where Ra and Rm are the rates of snow accumulation and melting, respectively. The magnitude of the solution is large when the difference between T1 and |T0| is small, in which case the temperature either spends most of the year above the melting point, or most of the year below the melting point. The mechanism behind the dependence of ∂ζ/∂T0 on T0 and T1 is related to the shape of the seasonal cycle in T. In regions where T0 > 0 and T1 is only slightly larger than |T0|, T crosses zero near the flat trough of the sinusoid, with temperatures below zero occurring only during a brief part of the year. In this case, when T warms there is a large reduction in the number of days when T < 0, leading to a substantially earlier time of complete snowmelt. We validate the proposed theory via comparison with SNOTEL-derived values of ∂ζ/∂T0, and from simulations performed with the Variable Infiltration Capacity (VIC) hydrologic model, finding that our theory can explain approximately 70% and 100% of the observed and VIC modeled variability in ∂ζ/∂T0, respectively.