diff --git a/doc/RTD/source/SubgridModels/AGNSpinJets/params.rst b/doc/RTD/source/SubgridModels/AGNSpinJets/params.rst
index eef4286a1a52d0914cc5432873787f54ca8039ad..1fda66ccbf660bb2ccda898a9fd897f017f28233 100644
--- a/doc/RTD/source/SubgridModels/AGNSpinJets/params.rst
+++ b/doc/RTD/source/SubgridModels/AGNSpinJets/params.rst
@@ -50,7 +50,7 @@ Below we give an example of parameter choices applicable for e.g. a 50 Mpc box.
         include_jets:                       1          # Global switch whether to include jet feedback [1] or not [0].
         turn_off_radiative_feedback:        0          # Global switch whether to turn off radiative (thermal) feedback [1] or not [0]. This should only be used if 'include_jets' is set to 1, since we want feedback in some form or another.
         alpha_acc:                          0.2        # Viscous alpha of the subgrid accretion disks. Likely to be within the 0.1-0.3 range. The main effect is that it sets the transition accretion rate between thin and thick disk, as dot(m) = 0.2 * alpha^2.
-        mdot_crit_ADAF:                     0.01       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
+        mdot_crit_ADAF:                     0.03       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
         seed_spin:                          0.01       # The (randomly-directed) black hole spin assigned to BHs when they are seeded. Should be strictly between 0 and 1.
         AGN_jet_velocity_model:             Constant   # How AGN jet velocities are calculated. If 'Constant', a single value is used. If 'BlackHoleMass', then an empirical relation between halo mass and black hole mass is used to calculate jet velocities. 'HaloMass' is currently not supported. 
         v_jet_km_p_s:                       3160.      # Jet velocity to use if 'AGN_jet_velocity_model' is 'Constant'. Units are km/s.
diff --git a/examples/IdealisedCluster/IdealisedCluster_M13/idealised_cluster_M13.yml b/examples/IdealisedCluster/IdealisedCluster_M13/idealised_cluster_M13.yml
index 1e4987e51809807150234f11fdd58ecb1b35ea6b..2a195a5737402af5babb2c00f4f980cb8acabde0 100644
--- a/examples/IdealisedCluster/IdealisedCluster_M13/idealised_cluster_M13.yml
+++ b/examples/IdealisedCluster/IdealisedCluster_M13/idealised_cluster_M13.yml
@@ -284,6 +284,7 @@ SPINJETAGN:
   include_jets:                       1          # Global switch whether to include jet feedback [1] or not [0]. Requires the 'include_spin' parameter to also be set to 1. 
   turn_off_radiative_feedback:        1          # Global switch whether to turn off radiative feedback [1] or not [0]. This should only be used if 'include_jets' is set to 1.
   alpha_acc:                          0.2        # Viscous alpha of the subgrid accretion disks. Should be within the 0.1-0.3 range.
+  mdot_crit_ADAF:                     0.03       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
   delta_ADAF:                         0.2        # Electron heating parameter, which controls the strength of radiative feedback in thick disks. Should be between 0.1 and 0.5.
   TD_region:                          B          # How to treat the subgrid accretion disk if it is thin, according to the Shakura & Sunyaev (1973) model. If set to B, region b will be used. If set to C, region c will be used.
   N_jet:                              2          # Target number of particles to kick as part of a single jet feedback event. Should be a multiple of 2 to ensure approximate momentum conservation.
diff --git a/examples/IdealisedCluster/IdealisedCluster_M135/idealised_cluster_M135.yml b/examples/IdealisedCluster/IdealisedCluster_M135/idealised_cluster_M135.yml
index c0a8d256ed011b222ad848ad42ec97d636598e2f..5a6f29eaf0e04ef0ba3ecbb43871207ce327b4cf 100644
--- a/examples/IdealisedCluster/IdealisedCluster_M135/idealised_cluster_M135.yml
+++ b/examples/IdealisedCluster/IdealisedCluster_M135/idealised_cluster_M135.yml
@@ -284,6 +284,7 @@ SPINJETAGN:
   include_jets:                       1          # Global switch whether to include jet feedback [1] or not [0]. Requires the 'include_spin' parameter to also be set to 1. 
   turn_off_radiative_feedback:        1          # Global switch whether to turn off radiative feedback [1] or not [0]. This should only be used if 'include_jets' is set to 1.
   alpha_acc:                          0.2        # Viscous alpha of the subgrid accretion disks. Should be within the 0.1-0.3 range.
+  mdot_crit_ADAF:                     0.03       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
   delta_ADAF:                         0.2        # Electron heating parameter, which controls the strength of radiative feedback in thick disks. Should be between 0.1 and 0.5.
   TD_region:                          B          # How to treat the subgrid accretion disk if it is thin, according to the Shakura & Sunyaev (1973) model. If set to B, region b will be used. If set to C, region c will be used.
   N_jet:                              2          # Target number of particles to kick as part of a single jet feedback event. Should be a multiple of 2 to ensure approximate momentum conservation.
diff --git a/examples/IdealisedCluster/IdealisedCluster_M14/idealised_cluster_M14.yml b/examples/IdealisedCluster/IdealisedCluster_M14/idealised_cluster_M14.yml
index b29df144d0c3f5e98c918321dd64bfc7ef5a63f6..07fb7247338b34d9656cd0417883ab227ae50cee 100644
--- a/examples/IdealisedCluster/IdealisedCluster_M14/idealised_cluster_M14.yml
+++ b/examples/IdealisedCluster/IdealisedCluster_M14/idealised_cluster_M14.yml
@@ -284,6 +284,7 @@ SPINJETAGN:
   include_jets:                       1          # Global switch whether to include jet feedback [1] or not [0]. Requires the 'include_spin' parameter to also be set to 1. 
   turn_off_radiative_feedback:        1          # Global switch whether to turn off radiative feedback [1] or not [0]. This should only be used if 'include_jets' is set to 1.
   alpha_acc:                          0.2        # Viscous alpha of the subgrid accretion disks. Should be within the 0.1-0.3 range.
+  mdot_crit_ADAF:                     0.03       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
   delta_ADAF:                         0.2        # Electron heating parameter, which controls the strength of radiative feedback in thick disks. Should be between 0.1 and 0.5.
   TD_region:                          B          # How to treat the subgrid accretion disk if it is thin, according to the Shakura & Sunyaev (1973) model. If set to B, region b will be used. If set to C, region c will be used.
   N_jet:                              2          # Target number of particles to kick as part of a single jet feedback event. Should be a multiple of 2 to ensure approximate momentum conservation.
diff --git a/examples/IdealisedCluster/IdealisedCluster_M15/idealised_cluster_M15.yml b/examples/IdealisedCluster/IdealisedCluster_M15/idealised_cluster_M15.yml
index f029c7c0194d025f233a176c9edc3dd05d30cdcb..71dbf91abb66f2fecd039314d7671a17b16d7cfe 100644
--- a/examples/IdealisedCluster/IdealisedCluster_M15/idealised_cluster_M15.yml
+++ b/examples/IdealisedCluster/IdealisedCluster_M15/idealised_cluster_M15.yml
@@ -284,6 +284,7 @@ SPINJETAGN:
   include_jets:                       1          # Global switch whether to include jet feedback [1] or not [0]. Requires the 'include_spin' parameter to also be set to 1. 
   turn_off_radiative_feedback:        1          # Global switch whether to turn off radiative feedback [1] or not [0]. This should only be used if 'include_jets' is set to 1.
   alpha_acc:                          0.2        # Viscous alpha of the subgrid accretion disks. Should be within the 0.1-0.3 range.
+  mdot_crit_ADAF:                     0.03       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
   delta_ADAF:                         0.2        # Electron heating parameter, which controls the strength of radiative feedback in thick disks. Should be between 0.1 and 0.5.
   TD_region:                          B          # How to treat the subgrid accretion disk if it is thin, according to the Shakura & Sunyaev (1973) model. If set to B, region b will be used. If set to C, region c will be used.
   N_jet:                              2          # Target number of particles to kick as part of a single jet feedback event. Should be a multiple of 2 to ensure approximate momentum conservation.
diff --git a/examples/parameter_example.yml b/examples/parameter_example.yml
index c94a480fa1658b3b1c541698171dc686379b1d5c..06f73b8e2b94176ad2c5a669af5f06705b9f89a4 100644
--- a/examples/parameter_example.yml
+++ b/examples/parameter_example.yml
@@ -788,7 +788,7 @@ SPINJETAGN:
   include_jets:                       1          # Global switch whether to include jet feedback [1] or not [0].
   turn_off_radiative_feedback:        0          # Global switch whether to turn off radiative (thermal) feedback [1] or not [0]. This should only be used if 'include_jets' is set to 1, since we want feedback in some form or another.
   alpha_acc:                          0.2        # Viscous alpha of the subgrid accretion disks. Likely to be within the 0.1-0.3 range. The main effect is that it sets the transition accretion rate between the thin and thick disk, as dot(m) = 0.2 * alpha^2.
-  mdot_crit_ADAF:                     0.01       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
+  mdot_crit_ADAF:                     0.03       # The transition normalized accretion rate (Eddington ratio) at which the disc goes from thick (low accretion rates) to thin (high accretion rates). The feedback also changes from kinetic jets to thermal isotropic, respectively.
   seed_spin:                          0.01       # The (randomly-directed) black hole spin assigned to BHs when they are seeded. Should be strictly between 0 and 1.
   AGN_jet_velocity_model:             Constant   # How AGN jet velocities are calculated. If 'Constant', a single value is used. If 'BlackHoleMass', then an empirical relation between halo mass and black hole mass is used to calculate jet velocities. 'HaloMass' is currently not supported. 
   v_jet_km_p_s:                       3160.      # Jet velocity to use if 'AGN_jet_velocity_model' is 'Constant'. Units are km/s.
diff --git a/src/black_holes/SPIN_JET/black_holes_properties.h b/src/black_holes/SPIN_JET/black_holes_properties.h
index 9a044d297abd22daf8b9390453af56541de0e38d..ff497d45a951a5aef8937c451cac82cd0362f11c 100644
--- a/src/black_holes/SPIN_JET/black_holes_properties.h
+++ b/src/black_holes/SPIN_JET/black_holes_properties.h
@@ -668,9 +668,10 @@ INLINE static void black_holes_props_init(struct black_holes_props *bp,
         bp->seed_spin);
   }
 
-  /* Calculate the critical transition accretion rate between the thick and
+  /* The critical transition accretion rate between the thick and
      thin disk regimes. */
-  bp->mdot_crit_ADAF = 0.2 * bp->alpha_acc_2;
+  bp->mdot_crit_ADAF =
+      parser_get_param_float(params, "SPINJETAGN:mdot_crit_ADAF");
 
   /* Calculate the gas-to-total pressure ratio as based on simulations
      (see Yuan & Narayan 2014) */