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Timothy A. Philpot - Mechanics of materials _ an integrated learning system-John Wiley (2017)

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Next, consider a free-body diagram that cuts through shafts (1) and (2) and

includes gear B. Once again, a positive internal torque will be assumed in shafts

(1) and (2). The teeth of gear E exert a force F on the teeth of gear B. If the

radius of gear B is denoted by R B , a moment equilibrium equation about the x

axis can be written as

T 1

R B

(1)

B

NB

= 40 teeth

(2)

T 2

Σ M = T − T − F × R = 0

(b)

x

2 1

B

F

Next, consider a free-body diagram that cuts through shaft (3) and includes

gear E as shown. A positive internal torque T 3 is assumed to act in shaft (3).

Since the teeth of gear E exert a force F on the teeth of gear B, equilibrium

requires that the teeth of gear B exert a force of equal magnitude in the opposite

direction on the teeth of gear E. With the radius of gear E denoted by R E , a

moment equilibrium equation about the x′ axis can be written as

T3

Σ Mx′ = −T3

− F × RE

= 0 ∴ F = −

(c)

R

E

T 3

(3)

F

NE=

60 teeth

E

R E

x′

The results of Equations (a) and (c) can be substituted into Equation (b) to give

= − × = ⋅ − ⎛ T3

T T F R

⎟ R = ⋅ + T R 1 2

B 18 kip in. B 18 kip in. 3

R

R

E

B

E

The gear radii R B and R E are not known. However, the ratio R B /R E is simply the gear

ratio between gears B and E. Since the teeth on both gears must be the same size in

order for the gears to mesh properly, the ratio of the teeth on each gear is equivalent

to the ratio of the gear radii. Consequently, the torque in shaft (1) can be expressed in

terms of N B and N E , the number of teeth on gears B and E, respectively:

T

B

= 18 kip⋅ in. + T N (d)

N

1 3

Equation (d) summarizes the results of the equilibrium considerations, but there are still

two unknowns in it: T 1 and T 3 . Consequently, this problem is statically indeterminate.

To solve the problem, an additional equation must be developed. This second equation

will be derived from the relationship between the angles of twist in shafts (1) and (3).

E

Step 2 — Geometry of Deformation: The rotation of gear B is equal to the angle of

twist in shaft (1):

φ

= φ

B 1

Similarly, the rotation of gear E is equal to the angle of twist in shaft (3):

φ

= φ

E 3

However, since the gear teeth mesh, the rotation angles for gears B and E are not

independent. The arclengths associated with the respective rotations must be equal,

but the gears turn in opposite directions. Thus, the relationship between the gear

rotations can be stated as

R φ

=−R

φ

B B E E

177

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