embodiments of the claimed invention can be explained with reference to fig1 , showing an object ( weight ) 10 on a surface 12 supported by a cantilever beam 13 containing a strain gauge 14 that may be connected to a power source 15 , amplifying means 16 , and output 17 . as the force translates across the surface 12 in the direction of arrow 18 a , a torque on cantilever beam 13 is produced . this bends the beam 13 . the output 17 of the strain gauge circuit 14 will show a responsive reading reflecting the output 17 . fig2 represents an output curve for an object of fixed weight that moves along surface 12 in the directions of arrows 18 a and 18 b . the torque when the object is centered on the cantilever beam is zero . as the object 10 moves in the direction of arrow 18 a , a positive output is observed . the farther the object 10 is moved from the cantilever beam , the greater the output despite the object 10 being constant in mass . as the object 10 moves in the direction of arrow 18 b , a negative output that is proportional in magnitude but opposite in charge is observed . the farther the object 10 is moved from the cantilever beam , the greater the negative output despite the object 10 being constant in mass . a zero or neutral point 20 is shown in fig2 representing a position of the center of gravity of the object 10 being positioned over the cantilever beam 13 . this same logic can be applied to an object 30 on a planar surface 32 supported by a cantilever beam 34 as shown in fig3 . the cantilever beam can bend in two orthogonal directions . the first direction is represented by arrows 36 a and 36 b . the second direction is represented by arrows 38 a and 38 b . as shown in fig4 , movement of the object 30 in the direction of arrow 36 a will produce a positive output 40 a . movement of the object 30 in the direction of arrow 36 b produces a negative output 40 b . centering the object 30 along the line 38 a , b produces a zero output 40 c . centering the object 30 along line 36 a , b produces a zero output 42 c . the position of the object 30 can be calculated and identified relative to the cantilever beam 34 . it is the purpose of the claimed invention to simultaneously measure the weight of the object and its location on a surface . one example way to accomplish this is to provide a force transducer ( not shown in fig3 ) supporting the cantilever beam 34 of fig3 . with reference to fig5 a , surface 50 is supported by two load cells 52 and 54 . the load cell 52 and 54 have respective strain gauges 58 and 56 that are powered by respective power sources 62 and 60 and amplifiers 66 and 64 . the output from strain gauges 56 and 58 are added to calculate the total weight 70 and subtracted to determine the relative position 68 . the addition of the signals results in a constant reading regardless of the position between load cell 52 and load cell 54 . on the other hand , if the signals from strain gauge 56 are subtracted from the signals of strain gauge 58 , a curve such as shown in fig5 b may be produced . when an object 51 is positioned over load cell 54 , the difference between the positive strain gauge reading from 56 and the negative strain gauge reading 58 results in a large positive reading . when the object 51 is positioned equidistant between load cell 52 and load cell 54 , the reading on strain gauges 56 and 58 will be equal and their difference is zero . when the object 51 is positioned over the load cell 52 the positive reading from strain gauge 58 can be subtracted from the already negative reading of the strain gauge 56 resulting in a large negative reading . thus , a curve is observed , as illustrated in fig5 b , that is proportional to the relative position of the object 51 along the supporting surface 50 . fig6 a shows a weighing surface 80 , such as a weighing platform or a hospital bed that is supported by four load cells 81 , 82 , 83 and 84 , each with strain gauges 85 , 86 , 87 , and 88 that measure the strain at each of the load cells 81 , 82 , 83 and 84 . if the load cells have similar outputs , object 89 can be positioned at any location on the weighing surface 80 . the sum of all the output of all strain gauges 85 , 86 , 87 and 88 will be relatively constant regardless of where the object 89 is located on the surface 80 . however , the difference between the output of strain gauges 85 and 88 , for example , can reveal the position of the weight relative to axis 90 extending between load cells 81 and 84 . thus , a signal can be produced for the location of the center of gravity simultaneously with the total weight . with reference to fig7 , a diagram is illustrated showing circuitry that calculates the weight and position of the center of gravity ( eccentricity ) of an object 89 on a surface 80 , as shown in fig6 a . outputs 110 , 112 , 114 and 116 from strain gauges 85 , 86 , 87 , and 88 ( fig6 a ) may be assumed to have equal output and polarity for a given force . for the purpose of this discussion , the output from each strain gauge is assumed to be positive . the output from these strain gauge is summed in module 118 together with a tare input 120 . for analog signals , module 118 can be a summing amplifier and tare adjustment 120 can be a potentiometer or the like to cancel the weight of bed and associated equipment . a patient &# 39 ; s weight can be displayed on an indicating device such a digital display 122 . positive outputs 110 and 112 are summed with outputs 114 and 116 after outputs 114 and 116 are sent through inverting devices 124 and 126 in module 130 and displayed on a similar display 132 as the relative position along the longitudinal axis 94 ( of fig6 a ) of the weighing surface 80 . the longitudinal axis will be the centerline of a bed if the bed is the weighing surface . preferably , the weight of the weighing surface 80 is symmetrical around the longitudinal axis 94 . if the weight is not symmetrical , a tare adjustment can be introduced upon initial set up as indicated by 134 . the output from module 130 may also be sent to a circuit 136 that inverts negative signals to a positive signal . such a circuit 136 is called full wave rectification in power supply circuits and can be simulated by operational amplifiers with diode feedback to improve linearity . in digital circuits , a value is sampled and if negative , its sign is inverted . in this manner , a patent &# 39 ; s position on either side of a bed will indicate a positive signal when it is off the centerline in the longitudinal direction . it can be compared with a preset value . this is shown schematically as comparer 139 with set device 138 and sent to an alarm 140 . the output is shown in fig6 b and fig6 c . in a like manner , positive outputs 112 and 116 are summed with outputs 110 and 114 after outputs 112 and 116 are inverted in modules 126 and 144 , along with a tare signal from tare device 144 if needed to correct the position of the neutral plane along the lateral axis 96 ( see fig6 a ). the output is displayed on indicator 146 . the signal may also be rectified by circuit 148 and compared to a preset signal from set device 150 in comparer 152 . the signal can operate alarm 154 or the signal may be combined with the alarm signal from 140 to operate a single alarm device . it should be noted that when the signals are combined as described above , the object &# 39 ; s weight is monitored in the longitudinal and lateral direction and the position can operate an alarm whenever its weight is displaced left or right of a longitudinal axis , or if above or below a lateral axis . if the alarm signal is divided by the weight signal derived from module 118 , then a patient &# 39 ; s position on the surface 80 can be indicated as unit or 1 when it is on the edge of the bed . this is achieved by linearly reducing ( dividing ) the output of the patient &# 39 ; s position along the lateral axis by the absolute value of output of the patient &# 39 ; s weight , producing a normalized output . similarly , the patient &# 39 ; s position along the longitudinal axis may be normalized . this can simplify setting of the alarm , since if it is desired to keep the patient in the center one half of the bed , the alarm may be set to 0 . 5 on a scale of 0 to 1 . in many applications it may not be necessary to measure the weight deviation toward the top or bottom of the bed , thus summing module 130 may be omitted . fig8 a - 8d are detailed electrical drawings illustrating a detailed circuit diagram , similar to fig7 , that calculates the weight and position of the center of gravity ( eccentricity ) of an object 89 on a surface 80 shown in fig6 a . fig9 is a flow diagram illustrating a method 900 of determining weight and position of an object on a weighing surface , according to an example embodiment of the present invention . according to the method 900 , the weighing surface has first , second , third , and fourth load cells with respective first , second , third , and fourth strain gauges , and where the strain gauges are configured to measure strain at the load cells caused by the object on the weighing surface . a first electrical signal produced by the first strain gauge , a second electrical signal produced by the second strain gauge , a third electrical signal produced by the third strain gauge , and a fourth electrical signal produced by the fourth strain gauge are obtained ( 905 ). the method involves simultaneously ( 910 ) adding the first electrical signal , second electrical , third electrical signal , and fourth electrical signal to produce a sum electrical signal proportional to a total weight on the load cells ( 915 ), and subtracting from the sum electrical signal a tare value proportional to the total weight of the weighing surface to produce a tared electrical signal ( 920 ). the method further involves simultaneously ( 910 ) subtracting a sum of the third electrical signal and the fourth electrical signal from a sum of the first electrical signal and the second electrical signal to determine a longitudinal value indicative of the position of a center of gravity of the object on the weighing surface ( 925 ). the method further involves simultaneously ( 910 ) subtracting a sum of the second electrical signal and the fourth electrical signal from a sum of the first electrical signal and the third electrical signal to determine a lateral value indicative of the position of a center of gravity of the object on the weighing surface ( 930 ). the method further involves displaying a weight of the object based on the tared electrical signal , a longitudinal position of the object based on the determined longitudinal value , and a lateral position of the object based on the determined lateral value ( 935 ). while this invention has been particularly shown and described with references to example embodiments thereof , it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the scope of the invention encompassed by the appended claims .