Clem Motor Explained

The Clem Motor Explained

To understand the Clem Motor one must be familiar with the principles of theory associated with the underlying dynamics of field, in that the underlying force, known as Non-linear Time Field Frequency Acceleration, (ntffa), determines the form and function of all physical structure.

For work to be done requires a dynamic differential in the underlying energy.

To understand the underlying dynamics we can look at a simple waterwheel, where we can examine the relationship of energy and resistance.

A waterwheel is driven by the flow of water pushing against the paddles of the wheel, while the flow of the water corresponds to a gravitational response as determined by the underlying condition of field.

The flowing water is following the path of least resistance in respect to the direction of Non-linear Time Field Frequency Acceleration, (ntffa), affecting a gravitational response.  And as the water flows downhill it loses energy relative the field in which it is flowing.  In other words, as the water flows downhill the water itself loses energy in proportion to the increasing energy of the field focused to the center of the Earth.

It is important to understand that if the water itself possessed sufficient energy, relative to the field in which it is located, the water would not flow.

When the water encounters the paddles of the waterwheel, the water pushes against the paddles while the paddles resist the force of the water.

As the paddles are resistant to the flow of the water, the flowing water causes the paddles to move whereby the waterwheel is forced to turn.

But so is the flow of the water resistant to the paddles, which results in the paddles slowing the flow of the water.  And as the water slows it gains energy in relation to the underlying energy of the water, as it is an increase in energy which causes the flow of the water to slow relative to the resistance of the paddles.

In turn the paddles cause the waterwheel to turn and the faster the waterwheel turns the greater is the wheels loss of energy.

If the waterwheel was not turning it would not experience a loss of energy.
It is a dynamic differential in energy which causes the waterwheel to turn, where the wheel is losing energy and the water is gaining energy relative to the field in which the waterwheel exists.

If for some reason there is insufficient water or the flow of water is diverted away from the waterwheel the wheel will stop turning as there is insufficient power or resistance to affect the motion of the wheel.

Now we come to the Clem Motor where a fluid is employed to drive the spiral grooved cone.

The rotation of the cone causes the cone to lose energy as the cone is resistant to the flow of the fluid, but so is the fluid resistant to the rotation of the cone.  This causes both the fluid and the cone to lose energy relative to the field in which the motor is located, which affects a proportional degree of resistance relative to the accelerating field in which the motor is located.

The fluid flowing through the spiral groove in the cone does not slow down as the groove becomes shallower as the radius of the cone increases.

The decrease in the channel or groove depth is proportional to an increase in the cone diameter, and as the diameter doubles so does the circumference of the cone.  This means the fluid has to travel twice as far in the same time to maintain a constant slip velocity.  So by reducing the channel or groove depth in half the fluid velocity is doubled thereby keeping the slip constant.

The spiral channels or grooves could be thought of as very long convergent nozzles.  The increase in fluid velocity is in the opposite direction of the rotor or cone spin.  We should expect a reaction force from the acceleration of the fluid.  This thrust would be directed tangent to the circumference and would increase the spin torque on the rotor or cone.  So even without the peripheral nozzles the rotor or cone experiences a thrust force in a direction that would self-propel it.

It should be noted that as the velocity increases in the channels or grooves the pressure also increases.  But Bernoulli’s Law requires the pressure to drop proportionally as the velocity increases, but this does not happen.

As the fluid is discharged at the bottom of the cone it goes directly to a heat exchanger which reduces the temperature of the fluid, which in turn increases the underlying energy of the fluid.  So when the fluid re-enters the top of the cone the fluid is in a re-energized state.

Therefore there is a continuous dynamic differential in energy existing between the rotation of the cone and the flow of the fluid which is maintained by the continuous cooling of the fluid by the heat exchanger.

At 200 pounds in weight the Clem Motor runs at 300 degrees F, the cone rotates at between 2600 and 2800 rpm and produces 350HP on a continuous basis.

If the flow of fluid is stopped the motor stops, but as long as the fluid flows the motor keeps running.

Once the motor reaches its optimum running temperature the motor becomes a self driving system, as no fuel is consumed in the process of its operation.

A twelve volt battery is employed during the start-up, which is recharged as the motor operates.  So the battery can be employed to run electronic gauges and lights as required.