Index: /issm/trunk-jpl/src/m/materials/nye.m
===================================================================
--- /issm/trunk-jpl/src/m/materials/nye.m	(revision 24718)
+++ /issm/trunk-jpl/src/m/materials/nye.m	(revision 24719)
@@ -26,7 +26,7 @@
 
 	if(ice_type==1)     % CO2 ice
-		A_const     = 10^(10.8);    % s^-1 MPa
-		Q           = 63000;        % J mol^-1
-		n           = 7;            % Glen's exponent
+		A_const     = 10^(13.0);    % s^-1 MPa
+		Q           = 66900;        % J mol^-1
+		n           = 8;            % Glen's exponent
 	elseif(ice_type==2) % H2O ice
 		A_const     = 9e4;          % s^-1 MPa
Index: /issm/trunk-jpl/src/m/materials/nye.py
===================================================================
--- /issm/trunk-jpl/src/m/materials/nye.py	(revision 24718)
+++ /issm/trunk-jpl/src/m/materials/nye.py	(revision 24719)
@@ -1,52 +1,51 @@
 import numpy as np
 
-
 def nye(temperature, ice_type):
-    """
+	"""
    NYE - figure out the rigidity of ice (either CO2 or H2O) for a given temperature
-    rigidity (in s^(1 / n)Pa) is the flow law parameter in the flow law sigma = B * e(1 / n) (Nye, p2000).
-    temperature is in Kelvin degrees
+	rigidity (in s^(1/n)Pa) is the flow law parameter in the flow law sigma=B*e(1/n) (Nye, p2000).
+	temperature is in Kelvin degrees
 
    Usage:
-       rigidity = nye(temperature, ice_type) % ice_type = 1: CO2 ice / /  ice_type = 2: H2O ice
-    """
+	   rigidity=nye(temperature,ice_type) % ice_type = 1: CO2 ice // ice_type = 2: H2O ice
+	"""
 
-    # Declaring temperature and rigidity arrays
-    if np.ndim(temperature) == 2:
-        T = temperature.flatten()
-    elif isinstance(temperature, float) or isinstance(temperature, int):
-        T = np.array([temperature])
-    else:
-        T = temperature
-    rigidity = np.zeros_like(T)
+        # Declaring temperature and rigidity arrays
+        if np.ndim(temperature)==2:
+            T=temperature.flatten()
+        elif isinstance(temperature,float) or isinstance(temperature,int):
+            T=np.array([temperature])
+        else:
+            T=temperature
+        rigidity=np.zeros_like(T)
 
-    # Beyond - melting - point cases
-    if (ice_type == 1):
-        for i in range(len(T)):
-            if (200 < T[i] < 220):
-                warnings.warn('CO2 ICE - POSSIBLE MELTING. Some temperature values are between 200K and 220K.')
-            break
-        if ((T >= 220).any()):
-            warnings.warn('CO2 ICE - GUARANTEED MELTING. Some temperature values are beyond 220K.')
-    elif (ice_type == 2) and ((T > 273.15).any()):
-        warnings.warn('H2O ICE - GUARANTEED MELTING. Some temperature values are beyond 273.15K.')
+        # Beyond-melting-point cases
+        if (ice_type==1):
+            for i in range(len(T)):
+                if (200<T[i]<220):
+                    warnings.warn('CO2 ICE - POSSIBLE MELTING. Some temperature values are between 200K and 220K.')
+                break
+            if ((T>=220).any()):
+                warnings.warn('CO2 ICE - GUARANTEED MELTING. Some temperature values are beyond 220K.')
+        elif (ice_type==2) and ((T>273.15).any()):
+            warnings.warn('H2O ICE - GUARANTEED MELTING. Some temperature values are beyond 273.15K.')
 
-    Rg = 8.3144598  # J mol^-1 K^-1
+	Rg = 8.3144598              # J mol^-1 K^-1
 
-    if ice_type == 1:  # CO2 ice
-        A_const = 10**(10.8)  # s^-1 MPa
-        Q = 63000.  # J mol^-1
-        n = 7.  # Glen's exponent
-    elif ice_type == 2:  # H2O ice
-        A_const = 9 * 10**4  # s^-1 MPa
-        Q = 60000.  #  J mol^-1
-        n = 3.  # Glen's exponent
-    else:
-        raise RuntimeError('Ice type not supported')
+	if ice_type == 1:           # CO2 ice
+	    A_const = 10**(13.0)    # s^-1 MPa
+	    Q = 66900.              # J mol^-1
+	    n = 8.                  # Glen's exponent
+	elif ice_type == 2:         # H2O ice
+	    A_const = 9*10**4       # s^-1 MPa
+	    Q = 60000.              #  J mol^-1
+	    n = 3.                  # Glen's exponent
+        else:
+            raise RuntimeError('Ice type not supported')
 
-    # Arrhenius Law
-    A = A_const * np.exp(-1 * Q / (T * Rg))  # s^-1 MPa
-    rigidity = A**(-1 / n) * 10**6  # s^(1 / n) Pa
+        # Arrhenius Law
+        A=A_const*np.exp(-1*Q/(T*Rg)) # s^-1 MPa
+        rigidity=A**(-1/n)*10**6 # s^(1/n) Pa
 
-    # Return output
-    return rigidity
+        # Return output
+        return rigidity