/* Functions that calculate the gravitational potential and its first and second derivatives for the rectangular prism using the formulas in Nagy et al. (2000). The coordinate system used is that of the article, ie: x -> North y -> East z -> Down References ---------- * Nagy, D., Papp, G., Benedek, J. (2000): The gravitational potential and its derivatives for the prism. Journal of Geodesy, 74, 552–560. */ #include #include #include "geometry.h" #include "constants.h" #include "grav_prism.h" double safe_atan2(double y, double x) { if(y == 0) { return 0; } if((y > 0) && (x < 0)) { return atan2(y, x) - PI; } if((y < 0) && (x < 0)) { return atan2(y, x) + PI; } return atan2(y, x); } double safe_log(double x) { if(x == 0) { return 0; } else { return log(x); } } /* Calculates the potential cause by a prism. */ double prism_pot(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); kernel = (x[i]*y[j]*safe_log(z[k] + r) + y[j]*z[k]*safe_log(x[i] + r) + x[i]*z[k]*safe_log(y[j] + r) - 0.5*x[i]*x[i]*safe_atan2(z[k]*y[j], x[i]*r) - 0.5*y[j]*y[j]*safe_atan2(z[k]*x[i], y[j]*r) - 0.5*z[k]*z[k]*safe_atan2(x[i]*y[j], z[k]*r)); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density */ res *= G*prism.density; return res; } /* Calculates the x component of gravitational attraction cause by a prism. */ double prism_gx(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); kernel = -(y[j]*safe_log(z[k] + r) + z[k]*safe_log(y[j] + r) - x[i]*safe_atan2(z[k]*y[j], x[i]*r)); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to mGal units */ res *= G*SI2MGAL*prism.density; return res; } /* Calculates the y component of gravitational attraction cause by a prism. */ double prism_gy(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); kernel = -(z[k]*safe_log(x[i] + r) + x[i]*safe_log(z[k] + r) - y[j]*safe_atan2(z[k]*x[i], y[j]*r)); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to mGal units */ res *= G*SI2MGAL*prism.density; return res; } /* Calculates the z component of gravitational attraction cause by a prism. */ double prism_gz(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); kernel = -(x[i]*safe_log(y[j] + r) + y[j]*safe_log(x[i] + r) - z[k]*safe_atan2(x[i]*y[j], z[k]*r)); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to mGal units */ res *= G*SI2MGAL*prism.density; return res; } /* Calculates the gxx gravity gradient tensor component cause by a prism. */ double prism_gxx(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); kernel = -safe_atan2(z[k]*y[j], x[i]*r); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to Eotvos units */ res *= G*SI2EOTVOS*prism.density; return res; } /* Calculates the gxy gravity gradient tensor component cause by a prism. */ double prism_gxy(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r, xtmp, ytmp; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { if(x[i] == 0 && y[j] == 0 && z[k] < 0) { xtmp = 0.0001*(prism.x2 - prism.x1); ytmp = 0.0001*(prism.y2 - prism.y1); r = sqrt(xtmp*xtmp + ytmp*ytmp + z[k]*z[k]); } else { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); } kernel = safe_log(z[k] + r); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to Eotvos units */ res *= G*SI2EOTVOS*prism.density; return res; } /* Calculates the gxz gravity gradient tensor component cause by a prism. */ double prism_gxz(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r, xtmp, ztmp; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { if(x[i] == 0 && z[k] == 0 && y[j] < 0) { xtmp = 0.0001*(prism.x2 - prism.x1); ztmp = 0.0001*(prism.z2 - prism.z1); r = sqrt(xtmp*xtmp + ztmp*ztmp + y[j]*y[j]); } else { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); } kernel = safe_log(y[j] + r); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to Eotvos units */ res *= G*SI2EOTVOS*prism.density; return res; } /* Calculates the gyy gravity gradient tensor component cause by a prism. */ double prism_gyy(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); kernel = -safe_atan2(z[k]*x[i], y[j]*r); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to Eotvos units */ res *= G*SI2EOTVOS*prism.density; return res; } /* Calculates the gyz gravity gradient tensor component cause by a prism. */ double prism_gyz(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r, ytmp, ztmp; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { if(z[k] == 0 && y[j] == 0 && x[i] < 0) { ytmp = 0.0001*(prism.y2 - prism.y1); ztmp = 0.0001*(prism.z2 - prism.z1); r = sqrt(ztmp*ztmp + ytmp*ytmp + x[i]*x[i]); } else { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); } kernel = safe_log(x[i] + r); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to Eotvos units */ res *= G*SI2EOTVOS*prism.density; return res; } /* Calculates the gzz gravity gradient tensor component cause by a prism. */ double prism_gzz(PRISM prism, double xp, double yp, double zp) { double x[2], y[2], z[2], kernel, res, r; register int i, j, k; /* First thing to do is make P the origin of the coordinate system */ x[0] = prism.x2 - xp; x[1] = prism.x1 - xp; y[0] = prism.y2 - yp; y[1] = prism.y1 - yp; z[0] = prism.z2 - zp; z[1] = prism.z1 - zp; res = 0; /* Evaluate the integration limits */ for(k=0; k<=1; k++) { for(j=0; j<=1; j++) { for(i=0; i<=1; i++) { r = sqrt(x[i]*x[i] + y[j]*y[j] + z[k]*z[k]); kernel = -safe_atan2(x[i]*y[j], z[k]*r); res += pow(-1, i + j + k)*kernel; } } } /* Now all that is left is to multiply res by the gravitational constant and density and convert it to Eotvos units */ res *= G*SI2EOTVOS*prism.density; return res; }