/* Copyright 2002-2022 CS GROUP
    * Licensed to CS GROUP (CS) under one or more
    * contributor license agreements.  See the NOTICE file distributed with
    * this work for additional information regarding copyright ownership.
    * CS licenses this file to You under the Apache License, Version 2.0
    * (the "License"); you may not use this file except in compliance with
    * the License.  You may obtain a copy of the License at
    *
    *   http://www.apache.org/licenses/LICENSE-2.0
   *
   * Unless required by applicable law or agreed to in writing, software
   * distributed under the License is distributed on an "AS IS" BASIS,
   * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
   * See the License for the specific language governing permissions and
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  package org.orekit.propagation.analytical.tle;
  
  import java.util.ArrayList;
  import java.util.Collections;
  import java.util.List;
  
  import org.hipparchus.geometry.euclidean.threed.Vector3D;
  import org.hipparchus.linear.RealMatrix;
  import org.hipparchus.util.FastMath;
  import org.hipparchus.util.MathUtils;
  import org.hipparchus.util.SinCos;
  import org.orekit.annotation.DefaultDataContext;
  import org.orekit.attitudes.Attitude;
  import org.orekit.attitudes.AttitudeProvider;
  import org.orekit.attitudes.InertialProvider;
  import org.orekit.data.DataContext;
  import org.orekit.errors.OrekitException;
  import org.orekit.errors.OrekitMessages;
  import org.orekit.frames.Frame;
  import org.orekit.frames.Frames;
  import org.orekit.orbits.CartesianOrbit;
  import org.orekit.orbits.Orbit;
  import org.orekit.propagation.AbstractMatricesHarvester;
  import org.orekit.propagation.MatricesHarvester;
  import org.orekit.propagation.SpacecraftState;
  import org.orekit.propagation.analytical.AbstractAnalyticalPropagator;
  import org.orekit.time.AbsoluteDate;
  import org.orekit.time.TimeScale;
  import org.orekit.utils.DoubleArrayDictionary;
  import org.orekit.utils.PVCoordinates;
  import org.orekit.utils.ParameterDriver;
  
  
  /** This class provides elements to propagate TLE's.
   * <p>
   * The models used are SGP4 and SDP4, initially proposed by NORAD as the unique convenient
   * propagator for TLE's. Inputs and outputs of this propagator are only suited for
   * NORAD two lines elements sets, since it uses estimations and mean values appropriate
   * for TLE's only.
   * </p>
   * <p>
   * Deep- or near- space propagator is selected internally according to NORAD recommendations
   * so that the user has not to worry about the used computation methods. One instance is created
   * for each TLE (this instance can only be get using {@link #selectExtrapolator(TLE)} method,
   * and can compute {@link PVCoordinates position and velocity coordinates} at any
   * time. Maximum accuracy is guaranteed in a 24h range period before and after the provided
   * TLE epoch (of course this accuracy is not really measurable nor predictable: according to
   * <a href="https://www.celestrak.com/">CelesTrak</a>, the precision is close to one kilometer
   * and error won't probably rise above 2 km).
   * </p>
   * <p>This implementation is largely inspired from the paper and source code <a
   * href="https://www.celestrak.com/publications/AIAA/2006-6753/">Revisiting Spacetrack
   * Report #3</a> and is fully compliant with its results and tests cases.</p>
   * @author Felix R. Hoots, Ronald L. Roehrich, December 1980 (original fortran)
   * @author David A. Vallado, Paul Crawford, Richard Hujsak, T.S. Kelso (C++ translation and improvements)
   * @author Fabien Maussion (java translation)
   * @see TLE
   */
  public abstract class TLEPropagator extends AbstractAnalyticalPropagator {
  
      // CHECKSTYLE: stop VisibilityModifier check
  
      /** Initial state. */
      protected TLE tle;
  
      /** UTC time scale. */
      protected final TimeScale utc;
  
      /** final RAAN. */
      protected double xnode;
  
      /** final semi major axis. */
      protected double a;
  
      /** final eccentricity. */
      protected double e;
  
      /** final inclination. */
      protected double i;
  
      /** final perigee argument. */
      protected double omega;
  
     /** L from SPTRCK #3. */
     protected double xl;
 
     /** original recovered semi major axis. */
     protected double a0dp;
 
     /** original recovered mean motion. */
     protected double xn0dp;
 
     /** cosinus original inclination. */
     protected double cosi0;
 
     /** cos io squared. */
     protected double theta2;
 
     /** sinus original inclination. */
     protected double sini0;
 
     /** common parameter for mean anomaly (M) computation. */
     protected double xmdot;
 
     /** common parameter for perigee argument (omega) computation. */
     protected double omgdot;
 
     /** common parameter for raan (OMEGA) computation. */
     protected double xnodot;
 
     /** original eccentricity squared. */
     protected double e0sq;
     /** 1 - e2. */
     protected double beta02;
 
     /** sqrt (1 - e2). */
     protected double beta0;
 
     /** perigee, expressed in KM and ALTITUDE. */
     protected double perige;
 
     /** eta squared. */
     protected double etasq;
 
     /** original eccentricity * eta. */
     protected double eeta;
 
     /** s* new value for the contant s. */
     protected double s4;
 
     /** tsi from SPTRCK #3. */
     protected double tsi;
 
     /** eta from SPTRCK #3. */
     protected double eta;
 
     /** coef for SGP C3 computation. */
     protected double coef;
 
     /** coef for SGP C5 computation. */
     protected double coef1;
 
     /** C1 from SPTRCK #3. */
     protected double c1;
 
     /** C2 from SPTRCK #3. */
     protected double c2;
 
     /** C4 from SPTRCK #3. */
     protected double c4;
 
     /** common parameter for raan (OMEGA) computation. */
     protected double xnodcf;
 
     /** 3/2 * C1. */
     protected double t2cof;
 
     // CHECKSTYLE: resume VisibilityModifier check
 
     /** TLE frame. */
     private final Frame teme;
 
     /** Spacecraft mass (kg). */
     private final double mass;
 
     /** Protected constructor for derived classes.
      *
      * <p>This constructor uses the {@link DataContext#getDefault() default data context}.
      *
      * @param initialTLE the unique TLE to propagate
      * @param attitudeProvider provider for attitude computation
      * @param mass spacecraft mass (kg)
      * @see #TLEPropagator(TLE, AttitudeProvider, double, Frame)
      */
     @DefaultDataContext
     protected TLEPropagator(final TLE initialTLE, final AttitudeProvider attitudeProvider,
                             final double mass) {
         this(initialTLE, attitudeProvider, mass,
                 DataContext.getDefault().getFrames().getTEME());
     }
 
     /** Protected constructor for derived classes.
      * @param initialTLE the unique TLE to propagate
      * @param attitudeProvider provider for attitude computation
      * @param mass spacecraft mass (kg)
      * @param teme the TEME frame to use for propagation.
      * @since 10.1
      */
     protected TLEPropagator(final TLE initialTLE,
                             final AttitudeProvider attitudeProvider,
                             final double mass,
                             final Frame teme) {
         super(attitudeProvider);
         setStartDate(initialTLE.getDate());
         this.tle       = initialTLE;
         this.teme      = teme;
         this.mass      = mass;
         this.utc       = initialTLE.getUtc();
 
         initializeCommons();
         sxpInitialize();
         // set the initial state
         final Orbit orbit = propagateOrbit(initialTLE.getDate());
         final Attitude attitude = attitudeProvider.getAttitude(orbit, orbit.getDate(), orbit.getFrame());
         super.resetInitialState(new SpacecraftState(orbit, attitude, mass));
     }
 
     /** Selects the extrapolator to use with the selected TLE.
      *
      * <p>This method uses the {@link DataContext#getDefault() default data context}.
      *
      * @param tle the TLE to propagate.
      * @return the correct propagator.
      * @see #selectExtrapolator(TLE, Frames)
      */
     @DefaultDataContext
     public static TLEPropagator selectExtrapolator(final TLE tle) {
         return selectExtrapolator(tle, DataContext.getDefault().getFrames());
     }
 
     /** Selects the extrapolator to use with the selected TLE.
      * @param tle the TLE to propagate.
      * @param frames set of Frames to use in the propagator.
      * @return the correct propagator.
      * @since 10.1
      */
     public static TLEPropagator selectExtrapolator(final TLE tle, final Frames frames) {
         return selectExtrapolator(
                 tle,
                 InertialProvider.of(frames.getTEME()),
                 DEFAULT_MASS,
                 frames.getTEME());
     }
 
     /** Selects the extrapolator to use with the selected TLE.
      *
      * <p>This method uses the {@link DataContext#getDefault() default data context}.
      *
      * @param tle the TLE to propagate.
      * @param attitudeProvider provider for attitude computation
      * @param mass spacecraft mass (kg)
      * @return the correct propagator.
      * @see #selectExtrapolator(TLE, AttitudeProvider, double, Frame)
      */
     @DefaultDataContext
     public static TLEPropagator selectExtrapolator(final TLE tle, final AttitudeProvider attitudeProvider,
                                                    final double mass) {
         return selectExtrapolator(tle, attitudeProvider, mass,
                 DataContext.getDefault().getFrames().getTEME());
     }
 
     /** Selects the extrapolator to use with the selected TLE.
      * @param tle the TLE to propagate.
      * @param attitudeProvider provider for attitude computation
      * @param mass spacecraft mass (kg)
      * @param teme the TEME frame to use for propagation.
      * @return the correct propagator.
      * @since 10.1
      */
     public static TLEPropagator selectExtrapolator(final TLE tle,
                                                    final AttitudeProvider attitudeProvider,
                                                    final double mass,
                                                    final Frame teme) {
 
         final double a1 = FastMath.pow( TLEConstants.XKE / (tle.getMeanMotion() * 60.0), TLEConstants.TWO_THIRD);
         final double cosi0 = FastMath.cos(tle.getI());
         final double temp = TLEConstants.CK2 * 1.5 * (3 * cosi0 * cosi0 - 1.0) *
                             FastMath.pow(1.0 - tle.getE() * tle.getE(), -1.5);
         final double delta1 = temp / (a1 * a1);
         final double a0 = a1 * (1.0 - delta1 * (TLEConstants.ONE_THIRD + delta1 * (delta1 * 134.0 / 81.0 + 1.0)));
         final double delta0 = temp / (a0 * a0);
 
         // recover original mean motion :
         final double xn0dp = tle.getMeanMotion() * 60.0 / (delta0 + 1.0);
 
         // Period >= 225 minutes is deep space
         if (MathUtils.TWO_PI / (xn0dp * TLEConstants.MINUTES_PER_DAY) >= (1.0 / 6.4)) {
             return new DeepSDP4(tle, attitudeProvider, mass, teme);
         } else {
             return new SGP4(tle, attitudeProvider, mass, teme);
         }
     }
 
     /** Get the Earth gravity coefficient used for TLE propagation.
      * @return the Earth gravity coefficient.
      */
     public static double getMU() {
         return TLEConstants.MU;
     }
 
     /** Get the extrapolated position and velocity from an initial TLE.
      * @param date the final date
      * @return the final PVCoordinates
      */
     public PVCoordinates getPVCoordinates(final AbsoluteDate date) {
 
         sxpPropagate(date.durationFrom(tle.getDate()) / 60.0);
 
         // Compute PV with previous calculated parameters
         return computePVCoordinates();
     }
 
     /** Computation of the first commons parameters.
      */
     private void initializeCommons() {
 
         // Sine and cosine of inclination
         final SinCos scI0 = FastMath.sinCos(tle.getI());
 
         final double a1 = FastMath.pow(TLEConstants.XKE / (tle.getMeanMotion() * 60.0), TLEConstants.TWO_THIRD);
         cosi0 = scI0.cos();
         theta2 = cosi0 * cosi0;
         final double x3thm1 = 3.0 * theta2 - 1.0;
         e0sq = tle.getE() * tle.getE();
         beta02 = 1.0 - e0sq;
         beta0 = FastMath.sqrt(beta02);
         final double tval = TLEConstants.CK2 * 1.5 * x3thm1 / (beta0 * beta02);
         final double delta1 = tval / (a1 * a1);
         final double a0 = a1 * (1.0 - delta1 * (TLEConstants.ONE_THIRD + delta1 * (1.0 + 134.0 / 81.0 * delta1)));
         final double delta0 = tval / (a0 * a0);
 
         // recover original mean motion and semi-major axis :
         xn0dp = tle.getMeanMotion() * 60.0 / (delta0 + 1.0);
         a0dp = a0 / (1.0 - delta0);
 
         // Values of s and qms2t :
         s4 = TLEConstants.S;  // unmodified value for s
         double q0ms24 = TLEConstants.QOMS2T; // unmodified value for q0ms2T
 
         perige = (a0dp * (1 - tle.getE()) - TLEConstants.NORMALIZED_EQUATORIAL_RADIUS) * TLEConstants.EARTH_RADIUS; // perige
 
         //  For perigee below 156 km, the values of s and qoms2t are changed :
         if (perige < 156.0) {
             if (perige <= 98.0) {
                 s4 = 20.0;
             } else {
                 s4 = perige - 78.0;
             }
             final double temp_val = (120.0 - s4) * TLEConstants.NORMALIZED_EQUATORIAL_RADIUS / TLEConstants.EARTH_RADIUS;
             final double temp_val_squared = temp_val * temp_val;
             q0ms24 = temp_val_squared * temp_val_squared;
             s4 = s4 / TLEConstants.EARTH_RADIUS + TLEConstants.NORMALIZED_EQUATORIAL_RADIUS; // new value for q0ms2T and s
         }
 
         final double pinv = 1.0 / (a0dp * beta02);
         final double pinvsq = pinv * pinv;
         tsi = 1.0 / (a0dp - s4);
         eta = a0dp * tle.getE() * tsi;
         etasq = eta * eta;
         eeta = tle.getE() * eta;
 
         final double psisq = FastMath.abs(1.0 - etasq); // abs because pow 3.5 needs positive value
         final double tsi_squared = tsi * tsi;
         coef = q0ms24 * tsi_squared * tsi_squared;
         coef1 = coef / FastMath.pow(psisq, 3.5);
 
         // C2 and C1 coefficients computation :
         c2 = coef1 * xn0dp * (a0dp * (1.0 + 1.5 * etasq + eeta * (4.0 + etasq)) +
              0.75 * TLEConstants.CK2 * tsi / psisq * x3thm1 * (8.0 + 3.0 * etasq * (8.0 + etasq)));
         c1 = tle.getBStar() * c2;
         sini0 = scI0.sin();
 
         final double x1mth2 = 1.0 - theta2;
 
         // C4 coefficient computation :
         c4 = 2.0 * xn0dp * coef1 * a0dp * beta02 * (eta * (2.0 + 0.5 * etasq) +
              tle.getE() * (0.5 + 2.0 * etasq) -
              2 * TLEConstants.CK2 * tsi / (a0dp * psisq) *
              (-3.0 * x3thm1 * (1.0 - 2.0 * eeta + etasq * (1.5 - 0.5 * eeta)) +
               0.75 * x1mth2 * (2.0 * etasq - eeta * (1.0 + etasq)) * FastMath.cos(2.0 * tle.getPerigeeArgument())));
 
         final double theta4 = theta2 * theta2;
         final double temp1 = 3 * TLEConstants.CK2 * pinvsq * xn0dp;
         final double temp2 = temp1 * TLEConstants.CK2 * pinvsq;
         final double temp3 = 1.25 * TLEConstants.CK4 * pinvsq * pinvsq * xn0dp;
 
         // atmospheric and gravitation coefs :(Mdf and OMEGAdf)
         xmdot = xn0dp +
                 0.5 * temp1 * beta0 * x3thm1 +
                 0.0625 * temp2 * beta0 * (13.0 - 78.0 * theta2 + 137.0 * theta4);
 
         final double x1m5th = 1.0 - 5.0 * theta2;
 
         omgdot = -0.5 * temp1 * x1m5th +
                  0.0625 * temp2 * (7.0 - 114.0 * theta2 + 395.0 * theta4) +
                  temp3 * (3.0 - 36.0 * theta2 + 49.0 * theta4);
 
         final double xhdot1 = -temp1 * cosi0;
 
         xnodot = xhdot1 + (0.5 * temp2 * (4.0 - 19.0 * theta2) + 2.0 * temp3 * (3.0 - 7.0 * theta2)) * cosi0;
         xnodcf = 3.5 * beta02 * xhdot1 * c1;
         t2cof = 1.5 * c1;
 
     }
 
     /** Retrieves the position and velocity.
      * @return the computed PVCoordinates.
      */
     private PVCoordinates computePVCoordinates() {
 
         // Sine and cosine of final perigee argument
         final SinCos scOmega = FastMath.sinCos(omega);
 
         // Long period periodics
         final double axn = e * scOmega.cos();
         double temp = 1.0 / (a * (1.0 - e * e));
         final double xlcof = 0.125 * TLEConstants.A3OVK2 * sini0 * (3.0 + 5.0 * cosi0) / (1.0 + cosi0);
         final double aycof = 0.25 * TLEConstants.A3OVK2 * sini0;
         final double xll = temp * xlcof * axn;
         final double aynl = temp * aycof;
         final double xlt = xl + xll;
         final double ayn = e * scOmega.sin() + aynl;
         final double elsq = axn * axn + ayn * ayn;
         final double capu = MathUtils.normalizeAngle(xlt - xnode, FastMath.PI);
         double epw = capu;
         double ecosE = 0;
         double esinE = 0;
         double sinEPW = 0;
         double cosEPW = 0;
 
         // Dundee changes:  items dependent on cosio get recomputed:
         final double cosi0Sq = cosi0 * cosi0;
         final double x3thm1 = 3.0 * cosi0Sq - 1.0;
         final double x1mth2 = 1.0 - cosi0Sq;
         final double x7thm1 = 7.0 * cosi0Sq - 1.0;
 
         if (e > (1 - 1e-6)) {
             throw new OrekitException(OrekitMessages.TOO_LARGE_ECCENTRICITY_FOR_PROPAGATION_MODEL, e);
         }
 
         // Solve Kepler's' Equation.
         final double newtonRaphsonEpsilon = 1e-12;
         for (int j = 0; j < 10; j++) {
 
             boolean doSecondOrderNewtonRaphson = true;
 
             final SinCos scEPW = FastMath.sinCos(epw);
             sinEPW = scEPW.sin();
             cosEPW = scEPW.cos();
             ecosE = axn * cosEPW + ayn * sinEPW;
             esinE = axn * sinEPW - ayn * cosEPW;
             final double f = capu - epw + esinE;
             if (FastMath.abs(f) < newtonRaphsonEpsilon) {
                 break;
             }
             final double fdot = 1.0 - ecosE;
             double delta_epw = f / fdot;
             if (j == 0) {
                 final double maxNewtonRaphson = 1.25 * FastMath.abs(e);
                 doSecondOrderNewtonRaphson = false;
                 if (delta_epw > maxNewtonRaphson) {
                     delta_epw = maxNewtonRaphson;
                 } else if (delta_epw < -maxNewtonRaphson) {
                     delta_epw = -maxNewtonRaphson;
                 } else {
                     doSecondOrderNewtonRaphson = true;
                 }
             }
             if (doSecondOrderNewtonRaphson) {
                 delta_epw = f / (fdot + 0.5 * esinE * delta_epw);
             }
             epw += delta_epw;
         }
 
         // Short period preliminary quantities
         temp = 1.0 - elsq;
         final double pl = a * temp;
         final double r = a * (1.0 - ecosE);
         double temp2 = a / r;
         final double betal = FastMath.sqrt(temp);
         temp = esinE / (1.0 + betal);
         final double cosu = temp2 * (cosEPW - axn + ayn * temp);
         final double sinu = temp2 * (sinEPW - ayn - axn * temp);
         final double u = FastMath.atan2(sinu, cosu);
         final double sin2u = 2.0 * sinu * cosu;
         final double cos2u = 2.0 * cosu * cosu - 1.0;
         final double temp1 = TLEConstants.CK2 / pl;
         temp2 = temp1 / pl;
 
         // Update for short periodics
         final double rk = r * (1.0 - 1.5 * temp2 * betal * x3thm1) + 0.5 * temp1 * x1mth2 * cos2u;
         final double uk = u - 0.25 * temp2 * x7thm1 * sin2u;
         final double xnodek = xnode + 1.5 * temp2 * cosi0 * sin2u;
         final double xinck = i + 1.5 * temp2 * cosi0 * sini0 * cos2u;
 
         // Orientation vectors
         final SinCos scuk   = FastMath.sinCos(uk);
         final SinCos scik   = FastMath.sinCos(xinck);
         final SinCos scnok  = FastMath.sinCos(xnodek);
         final double sinuk  = scuk.sin();
         final double cosuk  = scuk.cos();
         final double sinik  = scik.sin();
         final double cosik  = scik.cos();
         final double sinnok = scnok.sin();
         final double cosnok = scnok.cos();
         final double xmx = -sinnok * cosik;
         final double xmy = cosnok * cosik;
         final double ux  = xmx * sinuk + cosnok * cosuk;
         final double uy  = xmy * sinuk + sinnok * cosuk;
         final double uz  = sinik * sinuk;
 
         // Position and velocity
         final double cr = 1000 * rk * TLEConstants.EARTH_RADIUS;
         final Vector3D pos = new Vector3D(cr * ux, cr * uy, cr * uz);
 
         final double rdot   = TLEConstants.XKE * FastMath.sqrt(a) * esinE / r;
         final double rfdot  = TLEConstants.XKE * FastMath.sqrt(pl) / r;
         final double xn     = TLEConstants.XKE / (a * FastMath.sqrt(a));
         final double rdotk  = rdot - xn * temp1 * x1mth2 * sin2u;
         final double rfdotk = rfdot + xn * temp1 * (x1mth2 * cos2u + 1.5 * x3thm1);
         final double vx     = xmx * cosuk - cosnok * sinuk;
         final double vy     = xmy * cosuk - sinnok * sinuk;
         final double vz     = sinik * cosuk;
 
         final double cv = 1000.0 * TLEConstants.EARTH_RADIUS / 60.0;
         final Vector3D vel = new Vector3D(cv * (rdotk * ux + rfdotk * vx),
                                           cv * (rdotk * uy + rfdotk * vy),
                                           cv * (rdotk * uz + rfdotk * vz));
 
         return new PVCoordinates(pos, vel);
 
     }
 
     /** Initialization proper to each propagator (SGP or SDP).
      */
     protected abstract void sxpInitialize();
 
     /** Propagation proper to each propagator (SGP or SDP).
      * @param t the offset from initial epoch (min)
      */
     protected abstract void sxpPropagate(double t);
 
     /** {@inheritDoc}
      * <p>
      * For TLE propagator, calling this method is only recommended
      * for covariance propagation when the new <code>state</code>
      * differs from the previous one by only adding the additional
      * state containing the derivatives.
      * </p>
      */
     public void resetInitialState(final SpacecraftState state) {
         super.resetInitialState(state);
         super.setStartDate(state.getDate());
         final TLE newTLE = TLE.stateToTLE(state, tle, utc, teme);
         this.tle = newTLE;
         initializeCommons();
         sxpInitialize();
     }
 
     /** {@inheritDoc} */
     protected void resetIntermediateState(final SpacecraftState state, final boolean forward) {
         throw new OrekitException(OrekitMessages.NON_RESETABLE_STATE);
     }
 
     /** {@inheritDoc} */
     protected double getMass(final AbsoluteDate date) {
         return mass;
     }
 
     /** {@inheritDoc} */
     protected Orbit propagateOrbit(final AbsoluteDate date) {
         return new CartesianOrbit(getPVCoordinates(date), teme, date, TLEConstants.MU);
     }
 
     /** Get the underlying TLE.
      * @return underlying TLE
      */
     public TLE getTLE() {
         return tle;
     }
 
     /** {@inheritDoc} */
     public Frame getFrame() {
         return teme;
     }
 
     /** {@inheritDoc} */
     @Override
     protected AbstractMatricesHarvester createHarvester(final String stmName, final RealMatrix initialStm,
                                                         final DoubleArrayDictionary initialJacobianColumns) {
         // Create the harvester
         final TLEHarvester harvester = new TLEHarvester(this, stmName, initialStm, initialJacobianColumns);
         // Update the list of additional state provider
         addAdditionalStateProvider(harvester);
         // Return the configured harvester
         return harvester;
     }
 
     /**
      * Get the names of the parameters in the matrix returned by {@link MatricesHarvester#getParametersJacobian}.
      * @return names of the parameters (i.e. columns) of the Jacobian matrix
      */
     protected List<String> getJacobiansColumnsNames() {
         final List<String> columnsNames = new ArrayList<>();
         for (final ParameterDriver driver : tle.getParametersDrivers()) {
             if (driver.isSelected() && !columnsNames.contains(driver.getName())) {
                 columnsNames.add(driver.getName());
             }
         }
         Collections.sort(columnsNames);
         return columnsNames;
     }
 
 }