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(II) If 25 kg is the maximum mass mthat a person can hold in a hand when the arm is positioned with a 105° angle at the elbow as shown in Fig. 9–74, what is the maximum force\({F_{{\bf{max}}}}\) that the biceps muscle exerts on the forearm? Assume the forearm and hand have a total mass of 2.0 kg with a CG that is 15 cm from the elbow, and that the biceps muscle attaches 5.0 cm from the elbow.

Short Answer

Expert verified

The magnitude of the maximum force that the biceps muscle exerts on the forearm is 1849.58 N.

Step by step solution

01

Identification of given data

The given data can be listed below as:

  • The maximum force due to the biceps muscle is\({F_{{\rm{max}}}}\).
  • The total mass of the forearm and the hand is\({m_l} = 2{\rm{ kg}}\).
  • The mass of the ball is\(m = 25{\rm{ kg}}\).
  • The acceleration due to gravity is \(g = 9.81{\rm{ m/}}{{\rm{s}}^2}\).
02

Understanding the forces acting on the forearm

The person holds the ball whose weight acts in the downward direction. The force is due to the biceps muscle acting at an angle in the upward direction. The force due to the total mass of the arm acts in the downward direction.

Apply the equilibrium conditions; the net torque about the elbow joint can be equated to zero.

On solving these equations, the maximum force exerted by the biceps muscle can be estimated.

03

Determination of the magnitude of the maximum force that the biceps muscle exerts on the forearm

The forces acting on the forearm can be represented as:

At equilibrium, the net torques acting on the forearm about the elbow joint (A) becomes zero.

From the above figure, the torques’ equation can be expressed as:

\(\begin{array}{c}\sum {{T_{net}}} = 0\\{F_{{\rm{max}}}}\sin \phi \times AB = AC \times {m_l}g + AD \times mg\\{F_{{\rm{max}}}}\sin \left( {180^\circ - 105^\circ } \right) \times 5{\rm{ cm}}\left( {\frac{{1{\rm{ m}}}}{{100{\rm{ cm}}}}} \right) = 15{\rm{ cm}}\left( {\frac{{1{\rm{ m}}}}{{100{\rm{ cm}}}}} \right) \times {m_l}g + 35{\rm{ cm}}\left( {\frac{{1{\rm{ m}}}}{{100{\rm{ cm}}}}} \right) \times mg\\{F_{{\rm{max}}}}\sin 75^\circ \times 0.05{\rm{ m}} = 0.15{\rm{ m}} \times {m_l}g + 0.35{\rm{ m}} \times mg\end{array}\)

Substitute the values in the above equation.

\(\begin{array}{c}{F_{{\rm{max}}}}\sin 75^\circ \times 0.05{\rm{ m}} = 0.15{\rm{ m}} \times 2{\rm{ kg}} \times 9.81{\rm{ m/}}{{\rm{s}}^2} + 0.35{\rm{ m}} \times 25{\rm{ kg}} \times 9.81{\rm{ m/}}{{\rm{s}}^2}\\{F_{{\rm{max}}}} = \frac{{88.78}}{{0.048}}\;{\rm{kg}} \cdot {\rm{m/}}{{\rm{s}}^2}\left( {\frac{{1{\rm{ N}}}}{{1{\rm{ kg}} \cdot {\rm{m/}}{{\rm{s}}^2}}}} \right)\\ = 1849.58{\rm{ N}}\end{array}\)

Thus, the magnitude of the maximum force that the biceps muscle exerts on the forearm is 1849.58 N.

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Most popular questions from this chapter

(I) A nylon string on a tennis racket is under a tension of 275 N. If its diameter is 1.00 mm, by how much is it lengthened from its untensioned length of 30.0 cm?

(II) How much pressure is needed to compress the volume of an iron block by 0.10%? Express your answer in \({\bf{N/}}{{\bf{m}}^{\bf{2}}}\), and compare it to atmospheric pressure \(\left( {{\bf{1}}{\bf{.0 \times 1}}{{\bf{0}}^{\bf{5}}}\;{\bf{N/}}{{\bf{m}}^{\bf{2}}}} \right)\).

(III) A door 2.30 m high and 1.30 m wide has a mass of 13.0 kg. A hinge 0.40 m from the top and another hinge 0.40 m from the bottom each support half the door’s weight (Fig. 9–69). Assume that the center of gravity is at the geometrical center of the door, and determine the horizontal and vertical force components exerted by each hinge on the door.

(III) A uniform ladder of mass mand length leans at an angle\(\theta \)against a frictionless wall, Fig. 9–70. If the coefficient of static friction between the ladder and the ground is\({\mu _s}\). Determine a formula for the minimum angle at which the ladder will not slip.

A home mechanic wants to raise the 280-kg engine out of a car. The plan is to stretch a rope vertically from the engine to a branch of a tree 6.0 m above, and back to the bumper (Fig. 9–88). When the mechanic climbs up a stepladder and pulls horizontally on the rope at its midpoint, the engine rises out of the car. (a) How much force must the mechanic exert to hold the engine 0.50 m above its normal position? (b) What is the system’s mechanical advantage?

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