| Src Scale | Dst Scale | Aspect | Transform | Parameters | ||
|---|---|---|---|---|---|---|
| #N/A | ra_ip_mi | si dimensionless | ra_conversion | {'a': '100/5280/2.54/12'} | ||
| #N/A | #N/A | plane angle | ra_direct | {} | ||
| ra_ip_g_0 | #N/A | acceleration | ra_conversion | {'a':'9.80665'} | ||
| #N/A | ra_ip_ft.s-1 | speed | ra_conversion | {'a':'1/0.3048'} | ||
| #N/A | ra_ip_mi.h-1 | speed | ra_conversion | {'a':'3600/5280/0.3048'} | ||
| #N/A | ra_ip_kt | speed | ra_conversion | {'a':'3.6/1.852'} | ||
| #N/A | ra_ip_in.s-2 | acceleration | ra_conversion | {'a':'1/2.54E-2'} | ||
| #N/A | ra_ip_ft.s-2 | acceleration | ra_conversion | {'a':'1/0.3048'} | ||
| #N/A | ra_ip_g_0 | acceleration | ra_conversion | {'a':'1/9.80665'} | ||
| #N/A | #N/A | acceleration | ra_conversion | {'a': '1E2'} | ||
| #N/A | #N/A | flow rate | ra_conversion | {'a': '1E3'} | ||
| #N/A | #N/A | flow rate | ra_conversion | {'a': '86400/1E-3'} | ||
| #N/A | ra_ip_ft3.s-1 | flow rate | ra_conversion | {'a':'(12*2.54E-2)**-3'} | ||
| #N/A | ra_ip_ft3.min-1 | flow rate | ra_conversion | {'a':'60/(12*2.54E-2)**3'} | ||
| #N/A | ra_ip_yd3.min-1 | flow rate | ra_conversion | {'a':'60/(3*12*2.54E-2)**3'} | ||
| #N/A | ra_ip_gal_US.min-1 | flow rate | ra_conversion | {'a':'60/231/2.54E-2**3'} | ||
| #N/A | ra_ip_gal_US.d-1 | flow rate | ra_conversion | {'a':'86400/231/2.54E-2**3'} | ||
| #N/A | #N/A | time | ra_conversion | {'a': '60'} | ||
| #N/A | #N/A | time | ra_conversion | {'a': '60*60'} | ||
| #N/A | #N/A | time | ra_conversion | {'a': '24*60*60'} | ||
| #N/A | #N/A | length | ra_conversion | {'a': '149597870700'} | ||
| #N/A | #N/A | plane angle | ra_conversion | {'a': 'math.pi/180'} | ||
| #N/A | #N/A | plane angle | ra_conversion | {'a': 'math.pi/180/60'} | ||
| #N/A | #N/A | plane angle | ra_conversion | {'a': 'math.pi/180/60/60'} | ||
| #N/A | #N/A | area | ra_conversion | {'a': '1E4'} | ||
| #N/A | #N/A | volume | ra_conversion | {'a': '1E-3'} | ||
| #N/A | #N/A | mass | ra_conversion | {'a': '1E3'} | ||
| #N/A | #N/A | mass | ra_conversion | {'a': '1.660539040E-27'} | ||
| #N/A | #N/A | energy | ra_conversion | {'a': '1.602176634E-19'} | ||
| #N/A | #N/A | acceleration | ra_conversion | {'a': '1E-2'} | ||
| #N/A | #N/A | flow rate | ra_conversion | {'a': '1E-3'} | ||
| #N/A | ra_ip_ft3.min-1 | flow rate | ra_conversion | {'a':'60/(10*12*2.54E-2)**3'} | ||
| #N/A | #N/A | flow rate | ra_conversion | {'a': '1E-3/86400'} | ||
| ra_ip_ft3.s-1 | #N/A | flow rate | ra_conversion | {'a':'(12*2.54E-2)**3'} | ||
| ra_ip_ft3.min-1 | #N/A | flow rate | ra_conversion | {'a':'(12*2.54E-2)**3/60'} | ||
| ra_ip_ft3.min-1 | #N/A | flow rate | ra_conversion | {'a':'(10*12*2.54E-2)**3/60'} | ||
| ra_ip_yd3.min-1 | #N/A | flow rate | ra_conversion | {'a':'(3*12*2.54E-2)**3/60'} | ||
| ra_ip_gal_US.min-1 | #N/A | flow rate | ra_conversion | {'a':'231*2.54E-2**3/60'} | ||
| ra_ip_gal_US.d-1 | #N/A | flow rate | ra_conversion | {'a':'231*2.54E-2**3/86400'} | ||
| ra_ip_t_long | #N/A | mass | ra_conversion | {'a': '1016.0469088'} | ||
| ra_ip_t_short | #N/A | mass | ra_conversion | {'a': '907.18474'} | ||
| ra_ip_sl | #N/A | mass | ra_conversion | {'a': '14.5939'} | ||
| ra_ip_lb_av | #N/A | mass | ra_conversion | {'a': '0.45359237'} | ||
| ra_ip_oz_t | #N/A | mass | ra_conversion | {'a': '0.0311034768'} | ||
| ra_ip_gr_ap | #N/A | mass | ra_conversion | {'a': '6.479891E-5'} | ||
| ra_ip_lb.ft | #N/A | moment of mass | ra_conversion | {'a': '0.138255'} | ||
| ra_ip_t_short.yd-3 | #N/A | density | ra_conversion | {'a': '1186.553'} | ||
| ra_ip_lb.ft-3 | #N/A | density | ra_conversion | {'a': '16.01846'} | ||
| ra_ip_lb.gal_US-1 | #N/A | concentration | ra_conversion | {'a': '119.8264'} | ||
| ra_ip_oz_av.gal_US-1 | #N/A | concentration | ra_conversion | {'a': '7.489152'} | ||
| #N/A | ra_ip_lb.ft | moment of mass | ra_conversion | {'a': '1/0.138255'} | ||
| #N/A | ra_ip_t_short.yd-3 | density | ra_conversion | {'a': '1/1186.553'} | ||
| #N/A | ra_ip_lb.ft-3 | density | ra_conversion | {'a': '1/16.01846'} | ||
| #N/A | ra_ip_lb.gal_US-1 | concentration | ra_conversion | {'a': '1/119.8264'} | ||
| #N/A | ra_ip_oz_av.gal_US-1 | concentration | ra_conversion | {'a': '1/7.489152'} | ||
| #N/A | ra_ip_lb.ft.s-1 | momentum | ra_conversion | {'a': '1/0.1382550'} | ||
| #N/A | ra_ip_lb.ft2 | moment of inertia | ra_conversion | {'a': '1/0.04214011'} | ||
| ra_ip_lb.ft.s-1 | #N/A | momentum | ra_conversion | {'a': '0.1382550'} | ||
| ra_ip_lb.ft2 | #N/A | moment of inertia | ra_conversion | {'a': '0.04214011'} | ||
| ra_ip_lb_f | #N/A | force | ra_conversion | {'a': '4.448222'} | ||
| ra_ip_pdl | #N/A | force | ra_conversion | {'a': '0.1382550'} | ||
| ra_ip_lb_f.ft | #N/A | moment of force | ra_conversion | {'a': '1.355818'} | ||
| ra_ip_lb_f.ft | #N/A | moment of force | ra_conversion | {'a': '1.355818'} | ||
| ra_ip_lb_f.in | #N/A | moment of force | ra_conversion | {'a': '0.1129848'} | ||
| ra_ip_lb_f.in | #N/A | moment of force | ra_conversion | {'a': '0.1129848'} | ||
| ra_ip_atm | #N/A | pressure | ra_conversion | {'a':'1013250'} | ||
| ra_ip_bar | #N/A | pressure | ra_conversion | {'a':'1E5'} | ||
| ra_ip_mbar | #N/A | pressure | ra_conversion | {'a':'1E2'} | ||
| ra_ip_psi | #N/A | pressure | ra_conversion | {'a':'6.894757E3'} | ||
| ra_ip_klb_f.in-2 | #N/A | pressure | ra_conversion | {'a':'6.894757E6'} | ||
| ra_ip_lb_f.ft-2 | #N/A | pressure | ra_conversion | {'a':'47.88026'} | ||
| ra_ip_in_Hg_32_deg_F | #N/A | pressure | ra_conversion | {'a':'3.38638E3'} | ||
| ra_ip_ft_H20_39.2_deg_F | #N/A | pressure | ra_conversion | {'a':'2.98898E3'} | ||
| ra_ip_in_H20_39.2_deg_F | #N/A | pressure | ra_conversion | {'a':'249.082'} | ||
| ra_ip_mm_Hg_32_deg_F | #N/A | pressure | ra_conversion | {'a':'133.3224'} | ||
| ra_ip_torr | #N/A | pressure | ra_conversion | {'a':'133.3224'} | ||
| ra_ip_cP | #N/A | dynamic viscosity | ra_conversion | {'a':'1E-3'} | ||
| #N/A | #N/A | dynamic viscosity | ra_conversion | {'a':'1E-3'} | ||
| #N/A | ra_ip_cP | dynamic viscosity | ra_conversion | {'a':'1E3'} | ||
| #N/A | #N/A | dynamic viscosity | ra_conversion | {'a':'1E3'} | ||
| #N/A | ra_ip_cSt | kinematic viscosity | ra_conversion | {'a':'1E6'} | ||
| ra_ip_kW.h | #N/A | energy | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | work | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | amount of heat | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | energy | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | work | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | amount of heat | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | energy | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | work | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_kW.h | #N/A | amount of heat | ra_conversion | {'a':'3.6E6'} | ||
| ra_ip_cal | #N/A | energy | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | work | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | amount of heat | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | energy | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | work | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | amount of heat | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | energy | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | work | ra_conversion | {'a':'4.184'} | ||
| ra_ip_cal | #N/A | amount of heat | ra_conversion | {'a':'4.184'} | ||
| ra_ip_Btu | #N/A | energy | ra_conversion | {'a':'1055.056'} |