Source code for pvlib.tracking

from __future__ import division

import logging
pvl_logger = logging.getLogger('pvlib')

import numpy as np
import pandas as pd

from pvlib.tools import cosd, sind


[docs]def singleaxis(apparent_zenith, apparent_azimuth, axis_tilt=0, axis_azimuth=0, max_angle=90, backtrack=True, gcr=2.0/7.0): """ Determine the rotation angle of a single axis tracker using the equations in [1] when given a particular sun zenith and azimuth angle. backtracking may be specified, and if so, a ground coverage ratio is required. Rotation angle is determined in a panel-oriented coordinate system. The tracker azimuth axis_azimuth defines the positive y-axis; the positive x-axis is 90 degress clockwise from the y-axis and parallel to the earth surface, and the positive z-axis is normal and oriented towards the sun. Rotation angle tracker_theta indicates tracker position relative to horizontal: tracker_theta = 0 is horizontal, and positive tracker_theta is a clockwise rotation around the y axis in the x, y, z coordinate system. For example, if tracker azimuth axis_azimuth is 180 (oriented south), tracker_theta = 30 is a rotation of 30 degrees towards the west, and tracker_theta = -90 is a rotation to the vertical plane facing east. Parameters ---------- apparent_zenith : Series Solar apparent zenith angles in decimal degrees. apparent_azimuth : Series Solar apparent azimuth angles in decimal degrees. axis_tilt : float The tilt of the axis of rotation (i.e, the y-axis defined by axis_azimuth) with respect to horizontal, in decimal degrees. axis_azimuth : float A value denoting the compass direction along which the axis of rotation lies. Measured in decimal degrees East of North. max_angle : float A value denoting the maximum rotation angle, in decimal degrees, of the one-axis tracker from its horizontal position (horizontal if axis_tilt = 0). A max_angle of 90 degrees allows the tracker to rotate to a vertical position to point the panel towards a horizon. max_angle of 180 degrees allows for full rotation. backtrack : bool Controls whether the tracker has the capability to "backtrack" to avoid row-to-row shading. False denotes no backtrack capability. True denotes backtrack capability. gcr : float A value denoting the ground coverage ratio of a tracker system which utilizes backtracking; i.e. the ratio between the PV array surface area to total ground area. A tracker system with modules 2 meters wide, centered on the tracking axis, with 6 meters between the tracking axes has a gcr of 2/6=0.333. If gcr is not provided, a gcr of 2/7 is default. gcr must be <=1. Returns ------- DataFrame with the following columns: * tracker_theta: The rotation angle of the tracker. tracker_theta = 0 is horizontal, and positive rotation angles are clockwise. * aoi: The angle-of-incidence of direct irradiance onto the rotated panel surface. * surface_tilt: The angle between the panel surface and the earth surface, accounting for panel rotation. * surface_azimuth: The azimuth of the rotated panel, determined by projecting the vector normal to the panel's surface to the earth's surface. References ---------- [1] Lorenzo, E et al., 2011, "Tracking and back-tracking", Prog. in Photovoltaics: Research and Applications, v. 19, pp. 747-753. """ pvl_logger.debug('tracking.singleaxis') pvl_logger.debug(('axis_tilt={}, axis_azimuth={}, max_angle={}, ' + 'backtrack={}, gcr={:.3f}') .format(axis_tilt, axis_azimuth, max_angle, backtrack, gcr)) pvl_logger.debug('\napparent_zenith=\n{}\napparent_azimuth=\n{}' .format(apparent_zenith.head(), apparent_azimuth.head())) # MATLAB to Python conversion by # Will Holmgren (@wholmgren), U. Arizona. March, 2015. # Calculate sun position x, y, z using coordinate system as in [1], Eq 2. # Positive y axis is oriented parallel to earth surface along tracking axis # (for the purpose of illustration, assume y is oriented to the south); # positive x axis is orthogonal, 90 deg clockwise from y-axis, and parallel # to the earth's surface (if y axis is south, x axis is west); # positive z axis is normal to x, y axes, pointed upward. # Equations in [1] assume solar azimuth is relative to reference vector # pointed south, with clockwise positive. # Here, the input solar azimuth is degrees East of North, # i.e., relative to a reference vector pointed # north with clockwise positive. # Rotate sun azimuth to coordinate system as in [1] # to calculate sun position. try: pd.util.testing.assert_index_equal(apparent_azimuth.index, apparent_zenith.index) except AssertionError: raise ValueError('apparent_azimuth.index and ' + 'apparent_zenith.index must match.') times = apparent_azimuth.index az = apparent_azimuth - 180 apparent_elevation = 90 - apparent_zenith x = cosd(apparent_elevation) * sind(az) y = cosd(apparent_elevation) * cosd(az) z = sind(apparent_elevation) # translate array azimuth from compass bearing to [1] coord system # wholmgren: strange to see axis_azimuth calculated differently from az, # (not that it matters, or at least it shouldn't...). axis_azimuth_south = axis_azimuth - 180 pvl_logger.debug('axis_azimuth_south={}'.format(axis_azimuth_south)) # translate input array tilt angle axis_tilt to [1] coordinate system. # In [1] coordinates, axis_tilt is a rotation about the x-axis. # For a system with array azimuth (y-axis) oriented south, # the x-axis is oriented west, and a positive axis_tilt is a # counterclockwise rotation, i.e, lifting the north edge of the panel. # Thus, in [1] coordinate system, in the northern hemisphere a positive # axis_tilt indicates a rotation toward the equator, # whereas in the southern hemisphere rotation toward the equator is # indicated by axis_tilt<0. Here, the input axis_tilt is # always positive and is a rotation toward the equator. # Calculate sun position (xp, yp, zp) in panel-oriented coordinate system: # positive y-axis is oriented along tracking axis at panel tilt; # positive x-axis is orthogonal, clockwise, parallel to earth surface; # positive z-axis is normal to x-y axes, pointed upward. # Calculate sun position (xp,yp,zp) in panel coordinates using [1] Eq 11 # note that equation for yp (y' in Eq. 11 of Lorenzo et al 2011) is # corrected, after conversation with paper's authors. xp = x*cosd(axis_azimuth_south) - y*sind(axis_azimuth_south); yp = (x*cosd(axis_tilt)*sind(axis_azimuth_south) + y*cosd(axis_tilt)*cosd(axis_azimuth_south) - z*sind(axis_tilt)) zp = (x*sind(axis_tilt)*sind(axis_azimuth_south) + y*sind(axis_tilt)*cosd(axis_azimuth_south) + z*cosd(axis_tilt)) # The ideal tracking angle wid is the rotation to place the sun position # vector (xp, yp, zp) in the (y, z) plane; i.e., normal to the panel and # containing the axis of rotation. wid = 0 indicates that the panel is # horizontal. Here, our convention is that a clockwise rotation is # positive, to view rotation angles in the same frame of reference as # azimuth. For example, for a system with tracking axis oriented south, # a rotation toward the east is negative, and a rotation to the west is # positive. # Use arctan2 and avoid the tmp corrections. # angle from x-y plane to projection of sun vector onto x-z plane # tmp = np.degrees(np.arctan(zp/xp)) # Obtain wid by translating tmp to convention for rotation angles. # Have to account for which quadrant of the x-z plane in which the sun # vector lies. Complete solution here but probably not necessary to # consider QIII and QIV. # wid = pd.Series(index=times) # wid[(xp>=0) & (zp>=0)] = 90 - tmp[(xp>=0) & (zp>=0)] # QI # wid[(xp<0) & (zp>=0)] = -90 - tmp[(xp<0) & (zp>=0)] # QII # wid[(xp<0) & (zp<0)] = -90 - tmp[(xp<0) & (zp<0)] # QIII # wid[(xp>=0) & (zp<0)] = 90 - tmp[(xp>=0) & (zp<0)] # QIV # Calculate angle from x-y plane to projection of sun vector onto x-z plane # and then obtain wid by translating tmp to convention for rotation angles. wid = pd.Series(90 - np.degrees(np.arctan2(zp, xp)), index=times) # filter for sun above panel horizon wid[zp <= 0] = np.nan # Account for backtracking; modified from [1] to account for rotation # angle convention being used here. if backtrack: pvl_logger.debug('applying backtracking') axes_distance = 1/gcr temp = np.minimum(axes_distance*cosd(wid), 1) # backtrack angle # (always positive b/c acosd returns values between 0 and 180) wc = np.degrees(np.arccos(temp)) v = wid < 0 widc = pd.Series(index=times) widc[~v] = wid[~v] - wc[~v]; # Eq 4 applied when wid in QI widc[v] = wid[v] + wc[v]; # Eq 4 applied when wid in QIV else: pvl_logger.debug('no backtracking') widc = wid tracker_theta = widc.copy() tracker_theta[tracker_theta > max_angle] = max_angle tracker_theta[tracker_theta < -max_angle] = -max_angle # calculate panel normal vector in panel-oriented x, y, z coordinates. # y-axis is axis of tracker rotation. tracker_theta is a compass angle # (clockwise is positive) rather than a trigonometric angle. # the *0 is a trick to preserve NaN values. panel_norm = np.array([sind(tracker_theta), tracker_theta*0, cosd(tracker_theta)]) # sun position in vector format in panel-oriented x, y, z coordinates sun_vec = np.array([xp, yp, zp]) # calculate angle-of-incidence on panel aoi = np.degrees(np.arccos(np.abs(np.sum(sun_vec*panel_norm, axis=0)))) aoi = pd.Series(aoi, index=times) # calculate panel tilt and azimuth # in a coordinate system where the panel tilt is the # angle from horizontal, and the panel azimuth is # the compass angle (clockwise from north) to the projection # of the panel's normal to the earth's surface. # These outputs are provided for convenience and comparison # with other PV software which use these angle conventions. # project normal vector to earth surface. # First rotate about x-axis by angle -axis_tilt so that y-axis is # also parallel to earth surface, then project. # Calculate standard rotation matrix rot_x = np.array([[1, 0, 0], [0, cosd(-axis_tilt), -sind(-axis_tilt)], [0, sind(-axis_tilt), cosd(-axis_tilt)]]) pvl_logger.debug('rot_x=\n{}'.format(rot_x)) # panel_norm_earth contains the normal vector # expressed in earth-surface coordinates # (z normal to surface, y aligned with tracker axis parallel to earth) panel_norm_earth = np.dot(rot_x, panel_norm).T pvl_logger.debug('panel_norm_earth={}'.format(panel_norm_earth)) # projection to plane tangent to earth surface, # in earth surface coordinates projected_normal = np.array([panel_norm_earth[:,0], panel_norm_earth[:,1], panel_norm_earth[:,2]*0]).T pvl_logger.debug('projected_normal={}'.format(projected_normal)) # calculate vector magnitudes panel_norm_earth_mag = np.sqrt(np.nansum(panel_norm_earth**2, axis=1)) projected_normal_mag = np.sqrt(np.nansum(projected_normal**2, axis=1)) pvl_logger.debug('panel_norm_earth_mag={}, projected_normal_mag={}' .format(panel_norm_earth_mag, projected_normal_mag)) # renormalize the projected vector # avoid creating nan values. non_zeros = projected_normal_mag != 0 projected_normal[non_zeros] = (projected_normal[non_zeros].T / projected_normal_mag[non_zeros]).T pvl_logger.debug('renormalized projected_normal={}' .format(projected_normal)) # calculation of surface_azimuth # 1. Find the angle. # surface_azimuth = pd.Series( # np.degrees(np.arctan(projected_normal[:,1]/projected_normal[:,0])), # index=times) surface_azimuth = pd.Series( np.degrees(np.arctan2(projected_normal[:,1], projected_normal[:,0])), index=times) # 2. Clean up atan when x-coord or y-coord is zero # surface_azimuth[(projected_normal[:,0]==0) & (projected_normal[:,1]>0)] = 90 # surface_azimuth[(projected_normal[:,0]==0) & (projected_normal[:,1]<0)] = -90 # surface_azimuth[(projected_normal[:,1]==0) & (projected_normal[:,0]>0)] = 0 # surface_azimuth[(projected_normal[:,1]==0) & (projected_normal[:,0]<0)] = 180 # 3. Correct atan for QII and QIII # surface_azimuth[(projected_normal[:,0]<0) & (projected_normal[:,1]>0)] += 180 # QII # surface_azimuth[(projected_normal[:,0]<0) & (projected_normal[:,1]<0)] += 180 # QIII # 4. Skip to below # at this point surface_azimuth contains angles between -90 and +270, # where 0 is along the positive x-axis, # the y-axis is in the direction of the tracker azimuth, # and positive angles are rotations from the positive x axis towards # the positive y-axis. # Adjust to compass angles # (clockwise rotation from 0 along the positive y-axis) # surface_azimuth[surface_azimuth<=90] = 90 - surface_azimuth[surface_azimuth<=90] # surface_azimuth[surface_azimuth>90] = 450 - surface_azimuth[surface_azimuth>90] # finally rotate to align y-axis with true north # PVLIB_MATLAB has this latitude correction, # but I don't think it's latitude dependent if you always # specify axis_azimuth with respect to North. # if latitude > 0 or True: # surface_azimuth = surface_azimuth - axis_azimuth # else: # surface_azimuth = surface_azimuth - axis_azimuth - 180 # surface_azimuth[surface_azimuth<0] = 360 + surface_azimuth[surface_azimuth<0] # the commented code above is mostly part of PVLIB_MATLAB. # My (wholmgren) take is that it can be done more simply. # Say that we're pointing along the postive x axis (likely west). # We just need to rotate 90 degrees to get from the x axis # to the y axis (likely south), # and then add the axis_azimuth to get back to North. # Anything left over is the azimuth that we want, # and we can map it into the [0,360) domain. # 4. Rotate 0 reference from panel's x axis to it's y axis and # then back to North. surface_azimuth += 90 + axis_azimuth # 5. Map azimuth into [0,360) domain. surface_azimuth[surface_azimuth<0] += 360 surface_azimuth[surface_azimuth>=360] -= 360 # Calculate surface_tilt # Use pandas to calculate the sum because it handles nan values better. surface_tilt = (90 - np.degrees(np.arccos( pd.DataFrame(panel_norm_earth * projected_normal, index=times).sum(axis=1)))) # Bundle DataFrame for return values and filter for sun below horizon. df_out = pd.DataFrame({'tracker_theta':tracker_theta, 'aoi':aoi, 'surface_azimuth':surface_azimuth, 'surface_tilt':surface_tilt}, index=times) df_out[apparent_zenith > 90] = np.nan return df_out