Replace \rm{} commands

docs/LaTeX/tmtemod.tex

@@ -199,13 +199,13 @@ \section*{Adjust Hunziker et al. (2015) for TM/TE-split}
   \hat{E}^{+-}_{xx;H} &= \frac{y^2}{4\pi r^2}
   \int^\infty_{\kappa=0} \frac{\zeta_1}{\Gamma_1} 
   \frac{R^-_{H;1}}{M_{H;1}}
-  \exp(-\Gamma_1 h^{+-})J_0(\kappa r)\kappa\rm{d}\kappa \nonumber \\
+  \exp(-\Gamma_1 h^{+-})J_0(\kappa r)\kappa\mr{d}\kappa \nonumber \\
   %
   &\quad + \frac{x^2-y^2}{4\pi r^3}
   \int^\infty_{\kappa=0} \frac{\zeta_1}{\Gamma_1} 
   \left(\frac{R^-_{H;1}}{M_{H;1}} -
   \frac{R^-_{H;1}(\kappa=0)}{M_{H;1}(\kappa=0)}\right)
-  \exp(-\Gamma_1 h^{+-})J_1(\kappa r)\rm{d}\kappa \nonumber \\
+  \exp(-\Gamma_1 h^{+-})J_1(\kappa r)\mr{d}\kappa \nonumber \\
   %
   &\quad - \frac{\zeta_1 (x^2-y^2)}{4\pi\gamma_1 r^4}
   \frac{R^-_{H;1}(\kappa=0)}{M_{H;1}(\kappa=0)}

examples/educational/coordinate_system.py

@@ -57,12 +57,13 @@
   - ``depth = [0, -100, -1000, -1050]``: **RHS** (+z up)
 
 - A source or a receiver *exactly on* a boundary is taken as being in the lower
-  layer. Hence, if :math:`z_\rm{rec} = z_0`, where :math:`z_0` is the surface,
-  then the receiver is taken as in the air in the LHS, but as in the subsurface
-  in the RHS. Similarly, if :math:`z_\rm{rec} = z_\rm{seafloor}`, then the
-  receiver is taken as in the sea in the LHS, but as in the subsurface in the
-  RHS. This can be avoided by never placing it exactly on a boundary, but
-  slightly (e.g., 1 mm) in the layer where you want to have it.
+  layer. Hence, if :math:`z_\mathrm{rec} = z_0`, where :math:`z_0` is the
+  surface, then the receiver is taken as in the air in the LHS, but as in the
+  subsurface in the RHS. Similarly, if :math:`z_\mathrm{rec} =
+  z_\mathrm{seafloor}`, then the receiver is taken as in the sea in the LHS,
+  but as in the subsurface in the RHS. This can be avoided by never placing it
+  exactly on a boundary, but slightly (e.g., 1 mm) in the layer where you want
+  to have it.
 
 - Sign switches:
 

examples/educational/dipoles_and_loops.py

@@ -126,7 +126,7 @@
 
 # Frequency Domain
 plt.subplot(231)
-plt.title(r'$G^{ee}_{\rm{dip-dip}}$', fontsize=fs)
+plt.title(r'$G^{ee}_\mathrm{dip-dip}$', fontsize=fs)
 plt.plot(freq, fee_dip_dip.real, 'C0-', label='Real')
 plt.plot(freq, -fee_dip_dip.real, 'C0--')
 plt.plot(freq, fee_dip_dip.imag, 'C1-', label='Imag')
@@ -136,7 +136,7 @@
 plt.ylim([5e-8, 2e-5])
 
 ax1 = plt.subplot(232)
-plt.title(r'$G^{mm}_{\rm{dip-dip}}$', fontsize=fs)
+plt.title(r'$G^{mm}_\mathrm{dip-dip}$', fontsize=fs)
 plt.plot(freq, fmm_dip_dip.real, 'C0-', label='Real')
 plt.plot(freq, -fmm_dip_dip.real, 'C0--')
 plt.plot(freq, fmm_dip_dip.imag, 'C1-', label='Imag')
@@ -147,7 +147,7 @@
 plt.legend()
 
 plt.subplot(233)
-plt.title(r'$G^{mm}_{\rm{loop-dip}}$', fontsize=fs)
+plt.title(r'$G^{mm}_\mathrm{loop-dip}$', fontsize=fs)
 plt.plot(freq, f_loo_dip.real, 'C0-', label='Real')
 plt.plot(freq, -f_loo_dip.real, 'C0--')
 plt.plot(freq, f_loo_dip.imag, 'C1-', label='Imag')

examples/frequency_domain/magnetotelluric.py

@@ -45,7 +45,7 @@
     :label: ph-13
 
     z_{oj} \equiv \text{intrinsic impedance}
-        \equiv \sqrt{\rm{i}\omega \mu \rho_j} \, ,
+        \equiv \sqrt{\mathrm{i}\omega \mu \rho_j} \, ,
 
 .. math::
     :label: ph-14

examples/reproducing/ward1988.py

@@ -33,16 +33,17 @@
 # .. math::
 #
 #     h_z = \frac{m}{4\pi r^3} \left[
-#           \frac{9}{2\theta^2 r^2} \rm{erf}(\theta r) - \rm{erf}(\theta r) -
+#           \frac{9}{2\theta^2 r^2} \mathrm{erf}(\theta r) -
+#           \mathrm{erf}(\theta r) -
 #           \frac{1}{\pi^{1/2}} \left(\frac{9}{\theta r} + 4\theta r\right)
-#           \exp(-\theta^2 r^2) \right] \, , \qquad (4.69\rm{a})
+#           \exp(-\theta^2 r^2) \right] \, , \qquad (4.69\mathrm{a})
 #
 # and
 #
 # .. math::
 #
 #     \frac{\partial h_z}{\partial t} = -\frac{m\rho}{2\pi\mu_0 r^5} \left[
-#          9\rm{erf}(\theta r) -
+#          9\mathrm{erf}(\theta r) -
 #          \frac{2\theta r}{\pi^{1/2}} \left(9 + 6\theta^2 r^2 +
 #          4\theta^4 r^4\right) \exp(-\theta^2 r^2) \right] \, , \qquad (4.70)
 #

examples/time_domain/step_and_impulse.py

@@ -39,8 +39,9 @@
 # .. math::
 #
 #     E_x(\rho_h,\lambda,r,t) = \frac{\rho_h}{2 \pi r^3} \left[ 2\lambda +
-#     \rm{erf}\left(\frac{\tau_h}{2}\right) - 2\lambda
-#     \rm{erf}\left(\frac{\tau_h}{2\lambda}\right) + \frac{\tau_h}{\sqrt{\pi}}
+#     \mathrm{erf}\left(\frac{\tau_h}{2}\right) - 2\lambda
+#     \mathrm{erf}\left(\frac{\tau_h}{2\lambda}\right) +
+#     \frac{\tau_h}{\sqrt{\pi}}
 #     \exp\left(- \frac{\tau_h^2}{4\lambda^2}\right)   \right]
 #
 # Time Domain: Impulse Response :math:`\mathbf{\delta(t)}`